Clear Event Space and Conservative Fields, Space Time ... · Clear Event Space and Conservative...

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International Journal of Scientific and Research Publications, Volume 3, Issue 1, January 2013 1 ISSN 2250-3153 www.ijsrp.org Clear Event Space and Conservative Fields, Space Time Transposition, Energy Mass Equivalence, and Buckshot effect: Predicational Interiorities and Ontological Phenomenology thereof Sir Allan Zade* and Dr. K.N.Prasanna Kumar** *Author of famous Z-Theory **Post-doctoral Scholar, Department of mathematics, Kuvempu University, India Abstract: Systems of Z-Theory and Quantum Field Theory are investigated. It is shown that the time independence of the contributions portrays another system by itself and constitutes the equilibrium solution of the original time independent system. Further papers extensively draw inferences upon such concatenation process, ipso facto fait accompli. One work that relates Structural stability, electronic properties, and quantum conductivity of small-diameter silicon nanowires is that of Inna Ponomareva, Madhu Menon, Ernst Richter, and Antonis N. Andriotis, wherein they study structures and energetics of various types of silicon nanowires have been investigated using quantum molecular dynamics simulations to determine the most stable forms. The tetrahedral type nanowires oriented in the 111direction are found to be the most stable. The stability of the cage like nanowires is determined to lie somewhere between this and tetrahedral nanowires oriented in other directions. Furthermore, their electrical conducting properties are found to be better than those of tetrahedral nanowires, suggesting useful molecular electronic applications. quantum dots which we shall later concatenate and with Z-Theory is Stability of quantum dots in live cells by Zheng-Jiang Zhu, etal. Quantum dots are highly fluorescent and photostable, making them excellent tools for imaging. When using these quantum dots in cells and animals, however, intracellular biothiols (such as glutathione and cysteine) can degrade the quantum dot monolayer, compromising function. Here, we describe a label-free method to quantify the intracellular stability of monolayers on quantum dot surfaces that couples laser desorption/ionization mass spectrometry with inductively coupled plasma mass spectrometry. INTRODUCTION : We have to acknowledge that the Introduction is prepared by Google Search results and Wikipedia, for which we humbly pay homage. Following systems are taken in to consideration towards the end of consummation and consolidation and consubstantiation of a holistic Model. we study the stability analysis, Solution behaviour and asymptotic behaviour of the system (1) Intrusion Area and Maximal Transportation Time (2) Hidden Event Space and Passing Systems (3) Half Time Decay and Positive Time Shift Effect

Transcript of Clear Event Space and Conservative Fields, Space Time ... · Clear Event Space and Conservative...

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Clear Event Space and Conservative

Fields, Space Time Transposition,

Energy Mass Equivalence, and

Buckshot effect: Predicational

Interiorities and Ontological

Phenomenology thereof

Sir Allan Zade* and Dr. K.N.Prasanna Kumar**

*Author of famous Z-Theory

**Post-doctoral Scholar, Department of mathematics, Kuvempu University, India

Abstract: Systems of Z-Theory and Quantum Field Theory are investigated. It is shown that

the time independence of the contributions portrays another system by itself and constitutes

the equilibrium solution of the original time independent system. Further papers extensively

draw inferences upon such concatenation process, ipso facto fait accompli. One work that

relates Structural stability, electronic properties, and quantum conductivity of small-diameter

silicon nanowires is that of Inna Ponomareva, Madhu Menon, Ernst Richter, and Antonis N.

Andriotis, wherein they study structures and energetics of various types of silicon nanowires

have been investigated using quantum molecular dynamics simulations to determine the most

stable forms. The tetrahedral type nanowires oriented in the ⟨111⟩ direction are found to be the

most stable. The stability of the cage like nanowires is determined to lie somewhere between

this and tetrahedral nanowires oriented in other directions. Furthermore, their electrical

conducting properties are found to be better than those of tetrahedral nanowires, suggesting

useful molecular electronic applications. quantum dots which we shall later concatenate and

with Z-Theory is Stability of quantum dots in live cells by Zheng-Jiang Zhu, etal. Quantum

dots are highly fluorescent and photostable, making them excellent tools for imaging. When

using these quantum dots in cells and animals, however, intracellular biothiols (such as

glutathione and cysteine) can degrade the quantum dot monolayer, compromising function.

Here, we describe a label-free method to quantify the intracellular stability of monolayers on

quantum dot surfaces that couples laser desorption/ionization mass spectrometry with

inductively coupled plasma mass spectrometry.

INTRODUCTION :

We have to acknowledge that the Introduction is prepared by Google Search results and

Wikipedia, for which we humbly pay homage.

Following systems are taken in to consideration towards the end of consummation and

consolidation and consubstantiation of a holistic Model. we study the stability analysis,

Solution behaviour and asymptotic behaviour of the system

(1) Intrusion Area and Maximal Transportation Time

(2) Hidden Event Space and Passing Systems

(3) Half Time Decay and Positive Time Shift Effect

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(4) E is less than mc^2

(5) Space Time Transposition and Z Phenomenon

(6) Path integral formalism and canonical quantization

(7) Cross Shield Interaction and Space Time Transposition

(8) (1)

In the equation (1) variable have the following meaning: Vr is relative speed between a

moving observer and a beam of light; Vc is the speed of light relatively to the space; Vo is

the speed of the observer relatively to the space

(9) (1)

In the equation (1) variable have the following meaning: Vr is relative speed between a moving

observer and a beam of light; Vc is the speed of light relatively to the space; Vo is the speed of

the observer relatively to the space.

—VARIABLES USED

NOTATION

Module One

Intrusion Area and Maximal Transportation Time

: Category one of Intrusion Area

: Category two of Intrusion Area

: Category three of Intrusion Area

: Category one of Maximal Transportation Time

: Category two of Maximal Transportation Time

: Category three of Maximal Transportation Time

Module Two

Hidden Event Space and Passing Systems

: Category one of Hidden Event Space

: Category two of Hidden Event Space

: Category three of Hidden Event Space

: Category one of Passing Systems

: Category two of Passing Systems

: Category three of Passing Systems

Module three

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Half Time Decay and Positive Time Shift Effect

: Category one of Half Time Decay

: Category two of Half Time Decay

: Category three of Half Time Decay

: Category one of Positive Time Shift Effect

: Category two of Positive Time Shift Effect

: Category three of Positive Time Shift Effect

Module four

E is less than mc^2

: Category one of mc^2: here we are talking of the total energy of the universe. And the

systems to which Einstein’s Theory could be applied Classification is based on systemic

properties

: Category two of mc^2: here we are talking of the total energy of the universe. And the

systems to which Einstein’s Theory could be applied Classification is based on systemic

properties

: Category three of Clear Event Space mc^2: here we are talking of the total energy of

the universe. And the systems to which Einstein’s Theory could be applied Classification is

based on systemic properties

: Category one of Energy. Total energy in the universe. Stratification is based upon the

characteristics’ of the systems to which Mass energy equivalence can be applied.

: Category two of Energy. Total energy in the universe. Stratification is based upon the

characteristics’ of the systems to which Mass energy equivalence can be applied Note that

there is no sancrosanctness or sacrilege associated with the classification methodology.

Parametricization and concomitant characteristics’ which are higher parameters of the systems

are taken in to consideration.

: Category three of Energy. Total energy in the universe. Stratification is based upon the

characteristics’ of the systems to which Mass energy equivalence can be applied Note that

there is no sancrosanctness or sacrilege associated with the classification methodology.

Parametricization and concomitant characteristics’ which are higher parameters of the systems

are taken in to consideration.

Module five

Space Time Transposition and Z Phenomenon

: Category one of Space Time Transposition

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: Category two of Space Time Transposition

: Category three of Space Time Transposition

: Category one of Z Phenomenon

: Category two of Z Phenomenon

: Category three of Z Phenomenon

Module six

Surge effect and Buckshot effect

: Category one of Quantum Phase Transition

: Category two of Quantum Phase Transition

: Category three of Quantum Phase Transition

: Category one of Buckshot effect

: Category two of Buckshot effect

: Category three of Buckshot effect

Module seven

Cross Shield Interaction and Space Time Transposition

: Category one of Cross Shield Interaction

: Category two of Cross Shield Interaction

: Category three of Cross Shield Interaction

: Category one of Space Time Transposition

: Category two of Space Time Transposition

: Category three of Space Time Transposition

Module eight

(1) (1)

In the equation (1) variable have the following meaning: Vr is relative speed between a

moving observer and a beam of light; Vc is the speed of light relatively to the space; Vo is

the speed of the observer relatively to the space

: Category one of lhs of the equation (10( sytemal classification based on the

characteristics’ of the systems to which the equation becomes applicable)

: Category two of lhs of the equation (10( sytemal classification based on the

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characteristics’ of the systems to which the equation becomes applicable)

: Category three of lhs of the equation (10( sytemal classification based on the

characteristics’ of the systems to which the equation becomes applicable)

: Category one of first term on RHS

: Category two of first term on RHS

: Category three of first term on RHS

Module Nine

(1) (1)

In the equation (1) variable have the following meaning: Vr is relative speed between a

moving observer and a beam of light; Vc is the speed of light relatively to the space; Vo is

the speed of the observer relatively to the space

: Category one of Term on LHS of the equation (1)

: Category two of Term on LHS of the equation (1)

: Category three of Term on LHS of the equation (1)

: Category one of second term on the RHS

: Category two of second term on the RHS

: Category three of second term on the RHS

In perturbative quantum field theory, the forces between particles are mediated by other particles. The

electromagnetic force between two electrons is caused by an exchange of photons. Intermediate vector

bosons mediate the weak force and gluons mediate the strong force. There is currently no complete

quantum theory of the remaining fundamental force, gravity, but many of the proposed theories postulate

the existence of a graviton particle that mediates it. These force-carrying particles are virtual particles

and, by definition, cannot be detected while carrying the force, because such detection will imply that the

force is not being carried. In addition, the notion of "force mediating particle" comes from perturbation

theory, and thus does not make sense in a context of bound states.

In QFT, photons are not thought of as "little billiard balls" but are rather viewed as field quanta –

necessarily chunked ripples in a field, or "excitations", that "look like" particles. Fermions, like the

electron, can also be described as ripples/excitations in a field, where each kind of fermion has its own

field. In summary, the classical visualization of "everything is particles and fields", in quantum field

theory, resolves into "everything is particles", which then resolves into "everything is fields". In the end,

particles are regarded as excited states of a field (field quanta). The gravitational field and the

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electromagnetic field are the only two fundamental fields in Nature that have infinite range and a

corresponding classical low-energy limit, which greatly diminishes and hides their "particle-like"

excitations. Albert Einstein, in 1905, attributed "particle-like" and discrete exchanges of momenta and

energy, characteristic of "field quanta", to the electromagnetic field. Originally, his principal motivation

was to explain the thermodynamics of radiation. Although it is often claimed that the photoelectric and

Compton effects require a quantum description of the EM field, this is now understood to be untrue, and

proper proof of the quantum nature of radiation is now taken up into modern quantum optics as in the

antibunching effect. The word "photon" was coined in 1926 by physical chemist Gilbert Newton Lewis

(see also the articles photon antibunching and laser).

Prigogine developed the concept of “dissipative structures” to describe the coherent space-time structures

that form in open systems in which an exchange of matter and energy occurs between a system and its

environment. Ilya Prigogine received the Nobel Prize in Chemistry in 1977 for “his contributions to

nonequilibrium thermodynamics, particularly the theories of dissipative structures.” Prigogine’s primary

interest was in nonequilibrium irreversible phenomena because in these systems the arrow of time

becomes manifest. Prigogine viewed the arrow of time and irreversibility as playing a constructive role

in nature. For him the arrow of time was essential to the existence of biological systems, which contain

highly organized irreversible structures. Prigogine’s first major work on irreversible systems was his

theorem of minimum entropy production which was applicable to nonequilibrium stationary states near

equilibrium. Prigogine next began to work on far-from-equilibrium irreversible phenomena, both in

hydrodynamic systems and chemical systems. Such systems, because of nonlinear interactions, can form

spatial and temporal structures (dissipative structures) that can exist as long as the system is held far

from equilibrium due to a continual flow of energy or matter through the system.

Irreversible systems have an arrow of time which appears to be incompatible with Newtonian and

quantum dynamics, which are reversible theories. This incompatibility of the reversible foundations of

science with the irreversible behavior that is actually observed in chemical, hydrodynamic, and

biological systems remains one of the great mysteries of science. What is the origin of the arrow of time?

Is it a fundamental property of nature, or is it only an illusion? Prigogine’s view was that it must be a

fundamental property of nature. In the 1950s, he began to work on the foundations of statistical

mechanics and the question of how to reconcile Newtonian mechanics with an irreversible world. The

Newtonian foundations of equilibrium statistical mechanics require that the Newtonian dynamics be

chaotic. Prigogine’s early work at UT was focused on the problem of dissipative structures, but in later

years he became more and more involved with the problem of reconciling the arrow of time with

Newtonian and quantum dynamics. While working with non-equilibrium chemical systems, it was a

natural step to extend concepts found in these systems to complex social and economic systems.

Prigogine is considered one of the founders of complexity science.

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ):

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ),

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

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are Accentuation coefficients

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( )

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( )

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( )

( )( ) (

)( ) ( )( ) , (

)( ) ( )( ) (

)( ) ( )( ) (

)( ) ( )( )

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( )

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( )

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) (

)( )

are Dissipation coefficients Module Numbered One The differential system of this model is now (Module Numbered one)

( )

( ) [( )( ) (

)( )( )] 1

( )

( ) [( )( ) (

)( )( )] 2

( )

( ) [( )( ) (

)( )( )] 3

( )

( ) [( )( ) (

)( )( )] 4

( )

( ) [( )( ) (

)( )( )] 5

( )

( ) [( )( ) (

)( )( )] 6

( )( )( ) First augmentation factor

( )( )( ) First detritions factor

Module Numbered Two The differential system of this model is now ( Module numbered two)

( )

( ) [( )( ) (

)( )( )] 7

( )

( ) [( )( ) (

)( )( )] 8

( )

( ) [( )( ) (

)( )( )] 9

( )

( ) [( )( ) (

)( )(( ) )] 10

( )

( ) [( )( ) (

)( )(( ) )] 11

( )

( ) [( )( ) (

)( )(( ) )] 12

( )( )( ) First augmentation factor

( )( )(( ) ) First detritions factor

Module Numbered Three

The differential system of this model is now (Module numbered three)

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( )

( ) [( )( ) (

)( )( )] 13

( )

( ) [( )( ) (

)( )( )] 14

( )

( ) [( )( ) (

)( )( )] 15

( )

( ) [( )( ) (

)( )( )] 16

( )

( ) [( )( ) (

)( )( )] 17

( )

( ) [( )( ) (

)( )( )] 18

( )( )( ) First augmentation factor

( )( )( ) First detritions factor

Module Numbered Four The differential system of this model is now (Module numbered Four)

( )

( ) [( )( ) (

)( )( )] 19

( )

( ) [( )( ) (

)( )( )] 20

( )

( ) [( )( ) (

)( )( )] 21

( )

( ) [( )( ) (

)( )(( ) )] 22

( )

( ) [( )( ) (

)( )(( ) )] 23

( )

( ) [( )( ) (

)( )(( ) )] 24

( )( )( ) First augmentation factor

( )( )(( ) ) First detritions factor

Module Numbered Five: The differential system of this model is now (Module number five)

( )

( ) [( )( ) (

)( )( )] 25

( )

( ) [( )( ) (

)( )( )] 26

( )

( ) [( )( ) (

)( )( )] 27

( )

( ) [( )( ) (

)( )(( ) )] 28

( )

( ) [( )( ) (

)( )(( ) )] 29

( )

( ) [( )( ) (

)( )(( ) )] 30

( )( )( ) First augmentation factor

( )( )(( ) ) First detritions factor

Module Numbered Six

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The differential system of this model is now (Module numbered Six)

( )

( ) [( )( ) (

)( )( )] 31

( )

( ) [( )( ) (

)( )( )] 32

( )

( ) [( )( ) (

)( )( )] 33

( )

( ) [( )( ) (

)( )(( ) )] 34

( )

( ) [( )( ) (

)( )(( ) )] 35

( )

( ) [( )( ) (

)( )(( ) )] 36

( )( )( ) First augmentation factor

Module Numbered Seven: The differential system of this model is now (SEVENTH MODULE)

( )

( ) [( )( ) (

)( )( )] 37

( )

( ) [( )( ) (

)( )( )] 38

( )

( ) [( )( ) (

)( )( )] 39

( )

( ) [( )( ) (

)( )(( ) )] 40

( )

( ) [( )( ) (

)( )(( ) )] 41

( )

( ) [( )( ) (

)( )(( ) )] 42

( )( )( ) First augmentation factor

Module Numbered Eight

GOVERNING EQUATIONS:

The differential system of this model is now

( )

( ) [( )( ) (

)( )( )] 43

( )

( ) [( )( ) (

)( )( )] 44

( )

( ) [( )( ) (

)( )( )] 45

( )

( ) [( )( ) (

)( )(( ) )] 46

( )

( ) [( )( ) (

)( )(( ) )] 47

( )

( ) [( )( ) (

)( )(( ) )] 48

Module Numbered Nine

GOVERNING EQUATIONS:

The differential system of this model is now

( )

( ) [( )( ) (

)( )( )] 49

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( )

( ) [( )( ) (

)( )( )]

50

( )

( ) [( )( ) (

)( )( )]

51

( )

( ) [( )( ) (

)( )(( ) )]

52

( )

( ) [( )( ) (

)( )(( ) )]

53

( )

( ) [( )( ) (

)( )(( ) )]

54

( )( )( ) First augmentation factor

( )( )(( ) ) First detrition factor

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

55

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

56

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

57

Where ( )( )( ) (

)( )( ) ( )( )( ) are first augmentation coefficients for

category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are second augmentation coefficient

for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third augmentation coefficient

for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fourth augmentation

coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth augmentation

coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth augmentation

coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are seventh augmentation coefficient for

1,2,3

( )( )( ) (

)( )( ) ( )( )( ) are eight augmentation coefficient for

1,2,3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth

augmentation coefficient for 1,2,3

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( )

( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

58

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

59

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

60

Where ( )( )( ) (

)( )( ) ( )( )( ) are first detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are second detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth detrition

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth detrition coefficients

for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth detrition coefficients

for category 1, 2 and 3

– ( )( )( ) – (

)( )( ) , – ( )( )( ) are seventh detrition coefficients for

category 1, 2 and 3

– ( )( )( ) – (

)( )( ) – ( )( )( ) are eight detrition coefficients for

category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth

detrition coefficients for category 1, 2 and 3

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

61

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

62

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

63

Where ( )( )( ) (

)( )( ) ( )( )( ) are first augmentation coefficients

for category 1, 2 and 3

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( )( )( ) , (

)( )( ) , ( )( )( ) are second augmentation coefficient

for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third augmentation coefficient

for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth augmentation

coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth augmentation

coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth augmentation

coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) , ( )( )( ) are seventh augmentation

coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are eight augmentation coefficient

for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth augmentation coefficient for

category 1, 2 and 3

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

64

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

65

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

66

( )( )( ) , (

)( )( ) , ( )( )( ) are first detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) , ( )( )( ) are second detrition coefficients for

category 1,2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third detrition coefficients

for category 1,2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth detrition

coefficients for category 1,2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth detrition

coefficients for category 1,2 and 3

( )( )( ) (

)( )( ) , ( )( )( ) are sixth detrition

coefficients for category 1,2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are seventh detrition coefficients

for category 1,2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are eight detrition coefficients for

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category 1,2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition coefficients for

category 1,2 and 3

( )( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

67

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

68

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

69

( )( )( ) , (

)( )( ) , ( )( )( ) are first augmentation coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) , ( )( )( ) are second augmentation

coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third augmentation

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) ( )( )( ) are fourth

augmentation coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth augmentation

coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are sixth augmentation

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are seventh augmentation

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are eight augmentation

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth augmentation coefficients

for category 1, 2 and 3

( )( )

[

( )( ) (

)( )( ) – ( )( )( ) – (

)( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

70

71

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( )( )

[ (

)( ) ( )( )( ) – (

)( )( ) – ( )( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

( )( )

[

( )( ) (

)( )( ) – ( )( )( ) – (

)( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

72

( )( )( ) (

)( )( ) ( )( )( ) are first detrition coefficients for

category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are second detrition coefficients

for category 1, 2 and 3

( )( )( ) (

)( )( ) , ( )( )( ) are third detrition coefficients for

category 1,2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth detrition

coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth detrition

coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are sixth detrition

coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) – ( )( )( ) are seventh detrition

coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are eight detrition coefficients

for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition coefficients for

category 1, 2 and 3

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

73

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

74

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

75

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

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( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) , (

)( )( ) ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth detrition coefficients

for category 1 2 3

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

76

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

77

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

78

– ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) , ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) , – (

)( )( ) , – ( )( )( )

– ( )( )( ) , – (

)( )( ) – ( )( )( )

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ISSN 2250-3153

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– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition coefficients

for category 1 2 3

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

79

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

80

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

81

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) are fourth augmentation

coefficients for category 1,2, and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth augmentation

coefficients for category 1,2,and 3

( )( )( ) (

)( )( ) ( )( )( ) are sixth augmentation

coefficients for category 1,2, 3

( )( )( ) , (

)( )( ) , ( )( )( ) are seventh

augmentation coefficients for category 1,2, 3

( )( )( ) , (

)( )( ) , ( )( )( ) are eighth augmentation

coefficients for category 1,2, 3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth augmentation

coefficients for category 1,2, 3

( )

( )

[

(

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

82

( )

( )

[

(

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

83

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( )

( )

[

(

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

84

– ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) are fourth detrition coefficients

for category 1,2, and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth detrition

coefficients for category 1,2, and 3

– ( )( )( ) , – (

)( )( ) – ( )( )( ) are sixth detrition

coefficients for category 1,2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are seventh detrition

coefficients for category 1,2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are eighth detrition

coefficients for category 1,2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition

coefficients for category 1,2, and 3

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

85

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

86

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

87

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ISSN 2250-3153

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( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) - are fourth

augmentation coefficients

( )( )( ) (

)( )( ) ( )( )( ) - fifth augmentation

coefficients

( )( )( ) , (

)( )( ) ( )( )( ) sixth augmentation

coefficients

( )( )( ) , (

)( )( ) , ( )( )( )

( )( )( ) , (

)( )( ) , ( )( )( )

Eighth augmentation coefficients

( )( )( ) , (

)( )( ) , ( )( )( ) ninth augmentation

coefficients

( )( )

[ (

)( ) ( )( )( ) – (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

88

( )( )

[ (

)( ) ( )( )( ) – (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

89

( )( )

[ (

)( ) ( )( )( ) – (

)( )( ) – ( )( )( )

( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

90

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) are fourth detrition

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ISSN 2250-3153

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coefficients for category 1, 2, and 3

( )( )( ) , (

)( )( ) ( )( )( ) are fifth detrition

coefficients for category 1, 2, and 3

– ( )( )( ) , – (

)( )( ) – ( )( )( ) are sixth detrition

coefficients for category 1, 2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are seventh

detrition coefficients for category 1, 2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( )

are eighth detrition coefficients for category 1, 2, and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition

coefficients for category 1, 2, and 3

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

91

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

92

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

93

Where ( )( )( ) (

)( )( ) ( )( )( ) are first augmentation coefficients for

category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are second

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fourth

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are seventh

augmentation coefficient for category 1, 2 and 3

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ISSN 2250-3153

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( )( )( ) , (

)( )( ) , ( )( )( )

are eighth augmentation coefficient for 1,2,3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth

augmentation coefficient for 1,2,3

( )( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

]

94

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

Where ( )( )( ) (

)( )( ) ( )( )( ) are first detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are second

detrition coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third detrition

coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth

detrition coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth detrition

coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth detrition

coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( )

are seventh detrition coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are eighth

detrition coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition

coefficients for category 1, 2 and 3

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( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

95

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

( )

( )

[ (

)( ) ( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

Where ( )( )( ) (

)( )( ) ( )( )( ) are first augmentation coefficients

for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are second

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fourth

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are seventh

augmentation coefficient for 1,2,3

( )( )( ) , (

)( )( ) , ( )( )( ) are eighth

augmentation coefficient for 1,2,3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth

augmentation coefficient for 1,2,3

( )( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

]

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( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

Where ( )( )( ) (

)( )( ) ( )( )( ) are first detrition coefficients for

category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are second

detrition coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third

detrition coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth

detrition coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth

detrition coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , – ( )( )( ) are sixth detrition

coefficients for category 1, 2 and 3

– ( )( )( ) – (

)( )( ) , – ( )( )( ) are seventh detrition

coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are eighth

detrition coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth detrition

coefficients for category 1, 2 and 3

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

96

( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

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( )

( )

[

( )( ) (

)( )( ) ( )( )( ) (

)( )( )

( )( )( ) (

)( )( ) ( )( )( )

( )( )( ) (

)( )( ) ( )( )( ) ]

Where ( )( )( ) (

)( )( ) ( )( )( ) are first augmentation coefficients

for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are second

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fourth

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fifth

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth

augmentation coefficient for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are Seventh

augmentation coefficient for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are eighth

augmentation coefficient for 1,2,3

( )( )( ) , (

)( )( ) , ( )( )( ) are ninth

augmentation coefficient for 1,2,3

( )( )

[

( )( ) (

)( )( ) ( )( )( ) – (

)( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

]

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

( )( )

[ (

)( ) ( )( )( ) (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( )

– ( )( )( ) – (

)( )( ) – ( )( )( ) ]

Where ( )( )( ) (

)( )( ) ( )( )( ) are first detrition coefficients for

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category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are second

detrition coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are third

detrition coefficients for category 1, 2 and 3

( )( )( ) (

)( )( ) ( )( )( ) are fourth

detrition coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are fifth

detrition coefficients for category 1, 2 and 3

( )( )( ) , (

)( )( ) , ( )( )( ) are sixth

detrition coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are seventh detrition

coefficients for category 1, 2 and 3

– ( )( )( ) – (

)( )( ) , – ( )( )( ) are eighth

detrition coefficients for category 1, 2 and 3

– ( )( )( ) , – (

)( )( ) , – ( )( )( ) are ninth

detrition coefficients for category 1, 2 and 3

Where we suppose

(A) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(B) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )( ) ( )

( ) ( )( ) ( )

( )

97

(C) ( )( ) ( ) ( )

( )

( )( ) ( ) ( )

( )

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

98

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )( ) (

)( )( ) ( )( ) ( )( )

99

With the Lipschitz condition, we place a restriction on the behavior of functions

( )( )(

) and( )( )( ) (

) and ( ) are points belonging to the interval

[( )( ) ( )

( )] . It is to be noted that ( )( )( ) is uniformly continuous. In the

eventuality of the fact, that if ( )( ) then the function (

)( )( ) , the first augmentation coefficient attributable to terrestrial organisms, would be absolutely continuous.

Definition of ( )( ) ( )

( ) : 100

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(D) ( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

Definition of ( )( ) ( )

( ) :

(E) There exists two constants ( )( ) and ( )

( ) which together

with ( )( ) ( )

( ) ( )( ) and ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

101

Where we suppose

(F) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(G) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

102

( )( )( ) ( )

( ) ( )( ) ( )

( ) 103

(H) ( )( ) ( ) ( )

( ) 104

( )( ) (( ) ) ( )

( ) 105

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

106

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( ) 107

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( ) 108

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient attributable to terrestrial organisms, would be absolutely continuous.

Definition of ( )( ) ( )

( ) :

(I) ( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

109

Definition of ( )( ) ( )

( ) :

There exists two constants ( )( ) and ( )

( ) which together

with ( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( )

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satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) 110

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) 111

Where we suppose

(J) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )( ) ( )

( ) ( )( ) ( )

( )

112

( )( ) ( ) ( )

( )

( )( ) ( ) ( )

( )

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

113

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )(

) ( )( )( ) ( )

( ) ( )( )

114

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) And ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient would be absolutely continuous.

Definition of ( )( ) ( )

( ) :

(K) ( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

115

There exists two constants There exists two constants ( )( ) and ( )

( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

116

Where we suppose

( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(L) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

117

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Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )(( ) ) ( )

( ) ( )( ) ( )

( )

(M) ( )( ) ( ) ( )

( )

( )( ) (( ) ) ( )

( )

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

118

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

119

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient would be

absolutely continuous.

Definition of ( )( ) ( )

( ) :

( )( ) ( )

( ) are positive constants

( )( )

( )( ) ( )

( )

( )( )

120

Definition of ( )( ) ( )

( ) :

(N) There exists two constants ( )( ) and ( )

( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

121

Where we suppose

( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(O) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )(( ) ) ( )

( ) ( )( ) ( )

( )

122

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(P) ( )( ) ( ) ( )

( )

( )( ) ( ) ( )

( )

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

123

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

124

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient would be

absolutely continuous.

Definition of ( )( ) ( )

( ) :

( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

125

Definition of ( )( ) ( )

( ) :

There exists two constants ( )( ) and ( )

( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

126

Where we suppose

( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(Q) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )(( ) ) ( )

( ) ( )( ) ( )

( )

127

(R) ( )( ) ( ) ( )

( )

( )( ) (( ) ) ( )

( )

Definition of ( )( ) ( )

( ) :

128

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Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient would be

absolutely continuous.

Definition of ( )( ) ( )

( ) :

( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

129

Definition of ( )( ) ( )

( ) :

There exists two constants ( )( ) and ( )

( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

130

Where we suppose

(S) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(T) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )( ) ( )

( ) ( )( ) ( )

( )

131

(U) ( )( ) ( ) ( )

( )

( )( ) (( ) ) ( )

( )

Definition of ( )

( ) ( )( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants

and

132

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

133

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( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the first augmentation coefficient , would be absolutely continuous.

Definition of ( )( ) ( )

( ) :

(V) ( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

134

Definition of ( )( ) ( )

( ) :

(W) There exists two constants ( )( ) and ( )

( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

135

Where we suppose

A. ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

136

B. The functions ( )( ) (

)( ) are positive continuous increasing and bounded

Definition of ( )( ) ( )

( ):

137

( )( )( ) ( )

( ) ( )( )

138

( )( )(( ) ) ( )

( ) ( )( ) ( )

( ) 139

C. ( )( ) ( ) ( )

( )

140

( )( ) (( ) ) ( )

( ) 141

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants and

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

142

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

143

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

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and ( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the eighth augmentation coefficient , would be absolutely continuous.

Definition of ( )( ) ( )

( ) :

D. ( )( ) ( )

( ) are positive constants

( )( )

( )( ) ( )

( )

( )( )

144

Definition of ( )( ) ( )

( ) : E. There exists two constants ( )

( ) and ( )( ) which together with

( )( ) ( )

( ) ( )( )

( )( ) and the constants ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

Satisfy the inequalities

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

145

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

146

Where we suppose

(X) ( )( ) (

)( ) ( )( ) ( )

( ) ( )( ) (

)( )

(Y) The functions ( )( ) (

)( ) are positive continuous increasing and bounded.

Definition of ( )( ) ( )

( ):

( )( )( ) ( )

( ) ( )( )

( )( )( ) ( )

( ) ( )( ) ( )

( )

146A

(Z) ( )( ) ( ) ( )

( )

( )( ) ( ) ( )

( )

Definition of ( )( ) ( )

( ) :

Where ( )( ) ( )

( ) ( )( ) ( )

( ) are positive constants

and

They satisfy Lipschitz condition:

( )( )(

) ( )( )( ) ( )

( ) ( )( )

( )( )(( )

) ( )( )(( ) ) ( )

( ) ( ) ( ) ( )( )

With the Lipschitz condition, we place a restriction on the behavior of functions ( )( )(

)

and( )( )( ) . (

) and ( ) are points belonging to the interval [( )( ) ( )

( )] . It

is to be noted that ( )( )( ) is uniformly continuous. In the eventuality of the fact, that if

( )( ) then the function (

)( )( ) , the ninth augmentation coefficient attributable to, would be absolutely continuous.

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Definition of ( )( ) ( )

( ) :

(AA) ( )( ) ( )

( ) are positive constants

( )

( )

( )( ) ( )

( )

( )( )

Definition of ( )( ) ( )

( ) : (BB) There exists two constants ( )

( ) and ( )( ) which together with

( )( ) ( )

( ) ( )( ) ( )

( ) and the constants

( )( ) (

)( ) ( )( ) (

)( ) ( )( ) ( )

( ) satisfy the inequalities

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

( )( )

( )( ) (

)( ) ( )( ) ( )

( ) ( )( )

Theorem 1: if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the conditions

Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

147

Theorem 2 : if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the conditions

Definition of ( ) ( )

( ) ( )( ) ( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

148

Theorem 3 : if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the conditions

( ) ( )( ) ( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

149

Theorem 4 : if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the

conditions

Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

150

Theorem 5 : if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the

conditions

151

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Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

Theorem 6 : if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the

conditions

Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

152

Theorem 7: if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the conditions Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

153

Theorem 8: if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the conditions Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

153

A

Theorem 9: if the conditions (A)-(E) above are fulfilled, there exists a solution satisfying the

conditions

Definition of ( ) ( ) :

( ) ( )( )

( )( ) , ( )

( ) ( )( ) ( )( ) , ( )

153

B

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

154

( ) ( )

( )

( ) ( )

( ) 155

( ) ( )

( ) ( )( ) 156

( ) ( )

( ) ( )( ) 157

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By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

158

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof:

Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

159

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

160

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof:

Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By 161

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( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions

which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

162

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions

which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

163

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( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof:

Consider operator ( ) defined on the space of sextuples of continuous functions

which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

164

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

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By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

165

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

166

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

Proof: Consider operator ( ) defined on the space of sextuples of continuous functions which satisfy

166A

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( ) ( )

( )

( ) ( )

( )

( ) ( )

( ) ( )( )

( ) ( )

( ) ( )( )

By

( ) ∫ [( )

( ) ( ( )) (( )( )

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

( ) ∫ [( )

( ) ( ( )) (( )( ) (

)( )( ( ( )) ( ))) ( ( ))] ( )

Where ( ) is the integrand that is integrated over an interval ( )

The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

167

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 1

168

Analogous inequalities hold also for

The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( ) ( ( )

( ) )

( )( )( )( )

( )( ) ( ( )( ) )

169

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From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

170

Analogous inequalities hold also for

The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

171

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

172

Analogous inequalities hold also for

The operator ( ) maps the space of functions satisfying into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

173

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 4

174

The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 5

175

The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

176

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( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 6

Analogous inequalities hold also for

177

(a) The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

178

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 7

179 The operator ( ) maps the space of functions satisfying Equations into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

180

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 8

Analogous inequalities hold also for

181

(b) The operator ( ) maps the space of functions satisfying 34,35,36 into itself .Indeed it is obvious that

( ) ∫ [( )

( ) ( ( )

( ) ( )( ) ( ))]

( )

( ( )( ) )

( )( )( )( )

( )( ) ( ( )( ) )

From which it follows that

( ( ) ) ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )]

( ) is as defined in the statement of theorem 9

Analogous inequalities hold also for

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It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

182

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

183

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

184

In order that the operator ( ) transforms the space of sextuples of functions satisfying Equations into itself

The operator ( ) is a contraction with respect to the metric

(( ( ) ( )) ( ( ) ( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

185

Indeed if we denote

Definition of : ( ) ( )( )

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses it follows

| ( ) ( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) (( ( ) ( ) ( ) ( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

186

Remark 1: The fact that we supposed ( )( ) (

)( ) depending also on can be considered as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( ) and hypothesis can replaced by a usual Lipschitz condition.

Remark 2: There does not exist any where ( ) ( )

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From 19 to 24 it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 3: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

187

Remark 4: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

188

Remark 5: If is bounded from below and (( )( ) ( ( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )( ( ) ) ( ) ( )( )

189

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) ( ( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

190

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

191

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

192

In order that the operator ( ) transforms the space of sextuples of functions satisfying Equations into itself

193

The operator ( ) is a contraction with respect to the metric 194

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((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of : ( ) ( )( )

195

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

196

Where ( ) represents integrand that is integrated over the interval

From the hypotheses it follows

197

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows 198

Remark 6: The fact that we supposed ( )( ) (

)( ) depending also on can be considered as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

199

Remark 7: There does not exist any where ( ) ( )

it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

200

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 8: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

201

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If is bounded, the same property follows for and respectively.

Remark 9: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

202

Remark 10: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

203

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

204

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

205

206

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

207

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

208

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

209

In order that the operator ( ) transforms the space of sextuples of functions satisfying Equations into itself

210

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

211

Indeed if we denote

Definition of :( ( ) ( ) ) ( )(( ) ( ))

212

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

213

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( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses it follows

| ( ) ( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

214

Remark 11: The fact that we supposed ( )( ) (

)( ) depending also on can be considered as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

215

Remark 12: There does not exist any where ( ) ( )

it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

216

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 13: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

217

Remark 14: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

218

Remark 15: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

219

Then

( )

( )( )( ) which leads to 220

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(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

221

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

222

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

223

In order that the operator ( ) transforms the space of sextuples of functions satisfying

Equations into itself

224

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( ))

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses on Equations it follows

225

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

226

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Remark 16: The fact that we supposed ( )( ) (

)( ) depending also on can be considered

as not conformal with the reality, however we have put this hypothesis ,in order that we can

postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and

respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

227

Remark 17: There does not exist any where ( ) ( )

it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

228

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 18: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

229

Remark 19: If bounded, from below, the same property holds for The proof is

analogous with the preceding one. An analogous property is true if is bounded from below.

230

Remark 20: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

231

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

37 to 42

232

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Analogous inequalities hold also for

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

233

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

234

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

235

In order that the operator ( ) transforms the space of sextuples of functions satisfying

Equations into itself

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( ))

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses on it follows

236

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

237

Remark 21: The fact that we supposed ( )( ) (

)( ) depending also on can be considered

as not conformal with the reality, however we have put this hypothesis ,in order that we can

postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

238

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then it suffices to consider that ( )( ) (

)( ) depend only on and

respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

Remark 22: There does not exist any where ( ) ( )

it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

239

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 23: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

240

Remark 24: If bounded, from below, the same property holds for The proof is

analogous with the preceding one. An analogous property is true if is bounded from below.

241

Remark 25: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

242

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

Analogous inequalities hold also for

243

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

244

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( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

245

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

246

In order that the operator ( ) transforms the space of sextuples of functions satisfying

Equations into itself

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( ))

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses it follows

247

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

248

Remark 26: The fact that we supposed ( )( ) (

)( ) depending also on can be considered

as not conformal with the reality, however we have put this hypothesis ,in order that we can

postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of

If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and

respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

249

Remark 27: There does not exist any where ( ) ( )

it results

250

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( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 28: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

251

Remark 29: If bounded, from below, the same property holds for The proof is

analogous with the preceding one. An analogous property is true if is bounded from below.

252

Remark 30: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) :

Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

253

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

254

Analogous inequalities hold also for

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

255

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

256

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

257

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In order that the operator ( ) transforms the space of sextuples of functions satisfying Equations into itself

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( )) It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses on it follows

258

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

259

Remark 31: The fact that we supposed ( )( ) (

)( ) depending also on can be considered as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

260

Remark 32: There does not exist any where ( ) ( ) it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

261

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 33: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )

( ))

( )

( )(( )( ))

(

)( )

In the same way , one can obtain

262

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(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively. Remark 34: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

263

Remark 35: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) : Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

264

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations

265

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

266

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

267

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

268

In order that the operator ( ) transforms the space of sextuples of functions satisfying Equations into itself

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

269

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( ))

270

It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

271

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( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses it follows

272

|( )( ) ( )

( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( ) ( )

( )( )( )) ((( )

( ) ( )( ) ( )

( ) ( )( )))

And analogous inequalities for . Taking into account the hypothesis the result follows

273

Remark 36: The fact that we supposed ( )( ) (

)( ) depending also on can be considered as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

274

Remark 37 There does not exist any where ( ) ( ) it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

275

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 38: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

276

Remark 39: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

277

Remark 40: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then Definition of ( )( ) : Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

278

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Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ( ) ) (

)( )

279

It is now sufficient to take ( )

( )

( )( ) ( )

( )

( )( ) and to choose

( )( ) ( )

( ) large to have

279A

( )( )

( )( ) [( )( ) (( )

( ) )

(( )( )

)

] ( )( )

( )( )

( )( ) [(( )( )

) (

( )( )

)

( )( )] ( )

( )

In order that the operator ( ) transforms the space of sextuples of functions satisfying 39,35,36 into itsel

The operator ( ) is a contraction with respect to the metric

((( )( ) ( )

( )) (( )( ) ( )

( )))

| ( )( )

( )( )| ( )( )

| ( )( )

( )( )| ( )( )

Indeed if we denote

Definition of ( ) ( ) : ( ( ) ( ) ) ( )(( ) ( )) It results

| ( )

( )

| ∫ ( )( )

|

( )

( )| ( )( ) ( ) ( )( ) ( ) ( )

∫ ( )( )|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )( )(

( ) ( ))|

( )

( )| ( )( ) ( ) ( )( ) ( )

( )

( )( )(

( ) ( )) (

)( )( ( )

( )) ( )( ) ( ) ( )( ) ( ) ( )

Where ( ) represents integrand that is integrated over the interval

From the hypotheses on 45,46,47,28 and 29 it follows

|( )( ) ( )| ( )( )

( )( ) (( )( ) (

)( ) ( )( )

( )( )( )

( )) ((( )( ) ( )

( ) ( )( ) ( )

( )))

And analogous inequalities for . Taking into account the hypothesis (39,35,36) the result follows

Remark 41: The fact that we supposed ( )( ) (

)( ) depending also on can be considered

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as not conformal with the reality, however we have put this hypothesis ,in order that we can postulate condition necessary to prove the uniqueness of the solution bounded by

( )( ) ( )( ) ( )

( ) ( )( ) respectively of If instead of proving the existence of the solution on , we have to prove it only on a compact

then it suffices to consider that ( )( ) (

)( ) depend only on and respectively on ( )( ) and hypothesis can replaced by a usual Lipschitz condition.

Remark 42: There does not exist any where ( ) ( )

From 99 to 44 it results

( ) [ ∫ {(

)( ) ( )( )( ( ( )) ( ))} ( )

]

( ) ( (

)( ) ) for

Definition of (( )( ))

(( )

( )) (( )

( ))

:

Remark 43: if is bounded, the same property have also . indeed if

( )( ) it follows

(( )

( )) (

)( ) and by integrating

(( )( ))

( )( )(( )

( )) (

)( )

In the same way , one can obtain

(( )( ))

( )( )(( )

( )) (

)( )

If is bounded, the same property follows for and respectively.

Remark 44: If bounded, from below, the same property holds for The proof is analogous with the preceding one. An analogous property is true if is bounded from below.

Remark 45: If is bounded from below and (( )( ) (( )( ) )) (

)( ) then

Definition of ( )( ) : Indeed let be so that for

( )( ) (

)( )(( )( ) ) ( ) ( )( )

Then

( )

( )( )( ) which leads to

(( )( )( )( )

) ( )

If we take such that

it results

(( )( )( )( )

)

By taking now sufficiently small one sees that is

unbounded. The same property holds for if ( )( ) (( )( ) ) (

)( )

We now state a more precise theorem about the behaviors at infinity of the solutions of equations 37 to 92

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Behavior of the solutions of equation

Theorem If we denote and define

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

(a) )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

280

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) :

(b) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( ) and ( )

( )( ( )) ( )

( ) ( )

( )( )

281

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the equations

( )( )( ( ))

( )

( ) ( ) ( )( ) and ( )

( )( ( )) ( )

( ) ( ) ( )( )

282

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(c) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

283

and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

are defined

284

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

where ( )( ) is defined by equation

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

285

( ( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

286

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( )( ) ( )

(( )( ) ( )( )) 287

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( )) 288

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

289

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )( ) ( )

( )( )( ) (

)( )

( )( ) (

)( ) ( )( )

290

Behavior of the solutions of equation

Theorem 2: If we denote and define

291

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

(d) )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

292

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( ) 293

( )( ) (

)( ) ( )( ) (

)( )(( ) ) ( )( )(( ) ) ( )

( ) 294

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : 295

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots 296

(e) of the equations ( )( )( ( ))

( )

( ) ( ) ( )( ) 297

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and 298

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : 299

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the 300

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( ) 301

and ( )( )( ( ))

( )

( ) ( ) ( )( ) 302

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :- 303

(f) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by 304

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) 305

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

306

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) 307

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and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

308

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) 309

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

310

( )( ) is defined by equation

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( ) 311

( ( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

312

( )( ) ( )

(( )( ) ( )( )) 313

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( )) 314

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

315

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):- 316

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

317

( )( ) ( )

( )( )( ) (

)( )

( )( ) (

)( ) ( )( )

318

Behavior of the solutions

Theorem 3: If we denote and define

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

(a) )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )(( ) ) ( )

( )

319

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

(b) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

320

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and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :-

(c) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

321

and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) and ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

( )( ) is defined by equation

322

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( ) 323

( ( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

324

( )( ) ( )

(( )( ) ( )( )) 325

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( )) 326

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

327

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )( ) ( )

( )( )( ) (

)( )

328

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( )( ) (

)( ) ( )( )

Behavior of the solutions of equation Theorem: If we denote and define Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) :

(d) ( )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )(( ) ) ( )( )(( ) ) ( )

( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) :

(e) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

329

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(f) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

and ( )( )

( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

330

and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

331

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

where ( )( ) is defined by equation

332

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

333

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(( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) )

334

( )( ) ( )

(( )( ) ( )( ))

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

335

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

336

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )

( ) ( )( )( )

( ) ( )( )

( )( ) (

)( ) ( )( )

337

Behavior of the solutions of equation Theorem 2: If we denote and define Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) :

(g) ( )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )(( ) ) ( )( )(( ) ) ( )

( )

338

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) : (h) By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

339

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(i) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

340

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and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

341

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

where ( )( ) is defined by equation

342

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

343

(( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) )

344

( )( ) ( )

(( )( ) ( )( ))

345

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

346

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

347

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )

( ) ( )( )( )

( ) ( )( )

( )( ) (

)( ) ( )( )

348

Behavior of the solutions of equation Theorem 2: If we denote and define Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) :

(j) ( )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

349

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( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )(( ) ) ( )( )(( ) ) ( )

( ) Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) ( ) ( ) :

(k) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

350

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(l) If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

351

and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

352

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( )

where ( )( ) is defined by equation

353

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

354

(( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) )

355

( )( ) ( )

(( )( ) ( )( ))

356

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

357

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( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

358

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )( ) ( )

( )( )( ) (

)( )

( )( ) (

)( ) ( )( )

359

360

Behavior of the solutions of equation Theorem 2: If we denote and define Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) :

( )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( ) ( )

( ) ( )( ) (

)( ) ( )( )(( ) ) (

)( )(( ) ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) : By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the roots of the equations

( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

361

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) :

By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

If we define ( )( ) ( )

( ) ( )( ) ( )

( ) by ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

362

and analogously ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

363

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and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( ) where ( )

( ) is defined by equation

364

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

365

(( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

366

( )( ) ( )

(( )( ) ( )( ))

367

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

368

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

369

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )( ) ( )

( )( )( ) (

)( )

( )( ) (

)( ) ( )( )

370

Behavior of the solutions of equation Theorem 2: If we denote and define

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : (m) ( )

( ) ( )( ) ( )

( ) ( )( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( ) ( )

( ) ( )( ) (

)( ) ( )( )(( ) ) (

)( )(( ) ) ( )( )

371

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) :

(n) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

372

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Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(o) If we define ( )

( ) ( )( ) ( )

( ) ( )( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and analogously ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( )

374

Then the solution of global equations satisfies the inequalities

(( )( ) ( )( )) ( )

( )( ) where ( )

( ) is defined by equation

375

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

376

( ( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

377

( )( ) ( )

(( )( ) ( )( ))

378

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

379

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

380

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):- 381

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Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )( ) ( )

( )( )( ) (

)( )

( )( ) (

)( ) ( )( )

Behavior of the solutions of equation 37 to 92 Theorem 2: If we denote and define Definition of ( )

( ) ( )( ) ( )

( ) ( )( ) :

(p) )( ) ( )

( ) ( )( ) ( )

( ) four constants satisfying

( )( ) (

)( ) ( )( ) (

)( )( ) ( )( )( ) ( )

( )

( )( ) (

)( ) ( )( ) (

)( )(( ) ) ( )( )(( ) ) ( )

( )

382

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( ) ( ) :

(q) By ( )( ) ( )

( ) and respectively ( )( ) ( )

( ) the roots of the

equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( ) and

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) : By ( )

( ) ( )( ) and respectively ( )

( ) ( )( ) the

roots of the equations ( )( )( ( ))

( )

( ) ( ) ( )( )

and ( )( )( ( ))

( )

( ) ( ) ( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) :-

(r) If we define ( )

( ) ( )( ) ( )

( ) ( )( ) by

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

and ( )( )

( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and analogously

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) ( )( )

and ( )( )

( )( ) ( )

( ) ( )( ) ( )

( ) ( )( ) ( )

( ) where ( )( ) ( )

( ) are defined by 59 and 69 respectively

Then the solution of 99,20,44,22,23 and 44 satisfies the inequalities

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(( )( ) ( )( )) ( )

( )( )

where ( )( ) is defined by equation 45

( )( ) (( )( ) ( )( )) ( )

( )( ) ( )( )

( ( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ))

( )( ) ( )( )

( )( ) )

( )( ) ( )

(( )( ) ( )( ))

( )( ) ( )( ) ( )

( )( ) (( )( ) ( )( ))

( )( )

( )( )(( )( ) ( )( ))

[ ( )( ) ( )( ) ]

( )( ) ( )

( )( )

( )( )(( )( ) ( )( ) ( )( ))[ (( )( ) ( )( )) ( )( ) ]

( )( )

Definition of ( )( ) ( )

( ) ( )( ) ( )

( ):-

Where ( )( ) ( )

( )( )( ) (

)( )

( )( ) ( )

( ) ( )( )

( )

( ) ( )( )( )

( ) ( )( )

( )( ) (

)( ) ( )( )

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )( ) ( )

( ) :-

(a) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

383

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In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )( ) ( )( ) ( )

( )

384

(b) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

385

(c) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem.

Particular case :

If ( )( ) (

)( ) ( )( ) ( )

( ) and in this case ( )( ) ( )

( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

386

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

387

Definition of ( ) :- ( )

388

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It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

389

From which one obtains

Definition of ( )( ) ( )

( ) :-

(d) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

390

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

391

From which we deduce ( )( ) ( )( ) ( )

( ) 392

(e) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

393

(f) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

394

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

395

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

396

Now, using this result and replacing it in global equations we get easily the result stated in the theorem.

Particular case :

If ( )( ) (

)( ) ( )( ) ( )

( ) and in this case ( )( ) ( )

( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( )

397

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Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( )

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

398

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

399

From which one obtains

(a) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

400

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

Definition of ( )( ) :-

From which we deduce ( )( ) ( )( ) ( )

( )

401

(b) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

402

(c) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

403

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In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem.

Particular case :

If ( )( ) (

)( ) ( )( ) ( )

( ) and in this case ( )( ) ( )

( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( )

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( )

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

From which one obtains Definition of ( )

( ) ( )( ) :-

(d) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )

( ) ( )( ) ( )( )

404

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )( ) ( )( ) ( )

( )

405

(e) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

406

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( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

(f) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem. Particular case : If (

)( ) ( )( ) ( )

( ) ( )( ) and in this case ( )

( ) ( )( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if (

)( ) ( )( ) ( )

( ) ( )( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

407

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )

( ) ( )( ) :-

(g) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

408

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( )( ) ( )( ) ( )

( )

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )( ) ( )( ) ( )

( )

409

(h) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

410

(i) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem. Particular case : If (

)( ) ( )( ) ( )

( ) ( )( ) and in this case ( )

( ) ( )( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

411

Proof : From global equations we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

Definition of ( ) :- ( )

It follows

412

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(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )( ) ( )

( ) :-

(j) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )

( ) ( )( ) ( )( )

413

(k) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

414

(l) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem. Particular case : If (

)( ) ( )( ) ( )

( ) ( )( ) and in this case ( )

( ) ( )( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

415

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( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

Proof : From global equations we obtain ( )

( )

( ) (( )( ) (

)( ) ( )( )( ))

( )( )( )

( ) ( )( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )( )( ( ))

( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )( ) ( )

( ) :-

For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

416

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )

( ) ( )( ) ( )( )

417

If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

418

If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

419

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In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem. Particular case : If (

)( ) ( )( ) ( )

( ) ( )( ) and in this case ( )

( ) ( )( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then ( )( ) ( )

( )if in addition

( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important consequence of the relation

between ( )( ) and ( )

( ) and definition of ( )( )

420

Proof : From global equations we obtain ( )

( )

( ) (( )( ) (

)( ) ( )( )( )) (

)( )( ) ( ) ( )

( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )

( )( ( )) ( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )( ) ( )

( ) :-

(m) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

( )( ) ( )( ) ( )

( )

421

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )( ) ( )( ) ( )

( )

422

(n) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

423

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( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

(o) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in global equations we get easily the result stated in the theorem. Particular case :

If ( )( ) (

)( ) ( )( ) ( )

( ) and in this case ( )( ) ( )

( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if (

)( ) ( )( ) ( )

( ) ( )( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

424

Proof : From 99,20,44,22,23,44 we obtain

( )

( )

( ) (( )( ) (

)( ) ( )( )( ))

( )( )( )

( ) ( )( ) ( )

Definition of ( ) :- ( )

It follows

(( )( )( ( ))

( )

( ) ( ) ( )( ))

( )

(( )( )( ( ))

( )

( ) ( ) ( )( ))

From which one obtains

Definition of ( )( ) ( )

( ) :-

(p) For ( )( )

( )

( ) ( )( )

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

424A

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( )( ) ( )( ) ( )

( )

In the same manner , we get

( )( ) ( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

, ( )( ) ( )( ) ( )( )

( )( ) ( )( )

From which we deduce ( )( ) ( )( ) ( )

( )

(q) If ( )( ) ( )

( )

( )

( ) we find like in the previous case,

( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

( )( ) ( )( )( )( )

[ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

(r) If ( )( ) ( )

( ) ( )( )

, we obtain

( )( ) ( )( )

( )( ) ( )( )( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( ) [ ( )( )(( )( ) ( )( )) ]

( )( )

And so with the notation of the first part of condition (c) , we have

Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

In a completely analogous way, we obtain Definition of ( )( ) :-

( )( ) ( )( ) ( )

( ), ( )( ) ( )

( )

Now, using this result and replacing it in 99, 20,44,22,23, and 44 we get easily the result stated in the theorem. Particular case :

If ( )( ) (

)( ) ( )( ) ( )

( ) and in this case ( )( ) ( )

( ) if in addition

( )( ) ( )

( ) then ( )( ) ( )( ) and as a consequence ( ) ( )

( ) ( ) this also

defines ( )( ) for the special case .

Analogously if ( )( ) (

)( ) ( )( ) ( )

( ) and then

( )( ) ( )

( )if in addition ( )( ) ( )

( ) then ( ) ( )( ) ( ) This is an important

consequence of the relation between ( )( ) and ( )

( ) and definition of ( )( )

We can prove the following

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ,

425

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( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations 426

( )( )(

)( ) ( )( )( )

( ) 427

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) 428

( )( )(

)( ) ( )( )( )

( ) , 429

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

430

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

431

We can prove the following

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

432

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

433

Theorem If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

434

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( )( )(

)( ) ( )( )( )

( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) (

)( )( )( ) ( )

( )( )( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )

( ) ( )( ) as defined by equation are satisfied , then the system

435

Theorem : If ( )( ) (

)( ) are independent on , and the conditions with the notations

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) (

)( )( )( ) ( )

( )( )( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation are satisfied , then the system

436

Theorem : If ( )( ) (

)( ) are independent on , and the conditions (with the notations

45,46,27,28)

( )( )(

)( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( )(

)( ) ( )( )( )

( ) ,

( )( )(

)( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( ) ( )( )( )

( )

( )( ) ( )

( ) as defined by equation 45 are satisfied , then the system

436A

( )( ) [(

)( ) ( )( )( )] 437

( )( ) [(

)( ) ( )( )( )] 438

( )( ) [(

)( ) ( )( )( )] 439

( )( ) (

)( ) ( )( )( ) 440

( )( ) (

)( ) ( )( )( ) 441

( )( ) (

)( ) ( )( )( ) 442

has a unique positive solution , which is an equilibrium solution for the system

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( )( ) [(

)( ) ( )( )( )] 443

( )( ) [(

)( ) ( )( )( )] 444

( )( ) [(

)( ) ( )( )( )] 445

( )( ) (

)( ) ( )( )( ) 446

( )( ) (

)( ) ( )( )( ) 447

( )( ) (

)( ) ( )( )( ) 448

has a unique positive solution , which is an equilibrium solution

( )( ) [(

)( ) ( )( )( )] 449

( )( ) [(

)( ) ( )( )( )] 450

( )( ) [(

)( ) ( )( )( )] 451

( )( ) (

)( ) ( )( )( ) 452

( )( ) (

)( ) ( )( )( ) 453

( )( ) (

)( ) ( )( )( ) 454

has a unique positive solution , which is an equilibrium solution

( )( ) [(

)( ) ( )( )( )]

455

( )( ) [(

)( ) ( )( )( )] 456

( )( ) [(

)( ) ( )( )( )]

457

( )( ) (

)( ) ( )( )(( ))

458

( )( ) (

)( ) ( )( )(( ))

459

( )( ) (

)( ) ( )( )(( ))

460

has a unique positive solution , which is an equilibrium solution

( )( ) [(

)( ) ( )( )( )]

461

( )( ) [(

)( ) ( )( )( )]

462

( )( ) [(

)( ) ( )( )( )]

463

( )( ) (

)( ) ( )( )( )

464

( )( ) (

)( ) ( )( )( )

465

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( )( ) (

)( ) ( )( )( )

466

has a unique positive solution , which is an equilibrium solution

( )( ) [(

)( ) ( )( )( )]

467

( )( ) [(

)( ) ( )( )( )]

468

( )( ) [(

)( ) ( )( )( )]

469

( )( ) (

)( ) ( )( )( )

470

( )( ) (

)( ) ( )( )( )

471

( )( ) (

)( ) ( )( )( )

472

has a unique positive solution , which is an equilibrium solution

( )( ) [(

)( ) ( )( )( )]

473

( )( ) [(

)( ) ( )( )( )]

474

( )( ) [(

)( ) ( )( )( )]

475

( )( ) (

)( ) ( )( )( )

476

( )( ) (

)( ) ( )( )( )

477

( )( ) (

)( ) ( )( )( )

478

( )( ) [(

)( ) ( )( )( )]

479

( )( ) [(

)( ) ( )( )( )]

480

( )( ) [(

)( ) ( )( )( )]

481

( )( ) (

)( ) ( )( )( )

482

( )( ) (

)( ) ( )( )( )

483

( )( ) (

)( ) ( )( )( )

484

( )( ) [(

)( ) ( )( )( )]

484A

( )( ) [(

)( ) ( )( )( )]

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( )( ) [(

)( ) ( )( )( )]

( )( ) (

)( ) ( )( )( )

( )( ) (

)( ) ( )( )( )

( )( ) (

)( ) ( )( )( )

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

485

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

486

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

487

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

488

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

489

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

490

Proof: (a) Indeed the first two equations have a nontrivial solution if

491

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( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

Proof: (a) Indeed the first two equations have a nontrivial solution if ( ) (

)( )( )( ) ( )

( )( )( ) (

)( )( )( )( ) (

)( )( )( )( )

( )( )( )(

)( )( )

492

Proof:

(a) Indeed the first two equations have a nontrivial solution if

( ) ( )( )(

)( ) ( )( )( )

( ) ( )( )(

)( )( ) ( )( )(

)( )( )

( )( )( )(

)( )( )

492

A

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

493

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

first equations

494

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

495

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

496

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

497

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

498

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first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

499

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

500

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

501

Definition and uniqueness of :-

After hypothesis ( ) ( ) and the functions ( )( )( ) being increasing, it follows

that there exists a unique for which (

) . With this value , we obtain from the three

first equations

( )( )

[( )( ) (

)( )( )]

, ( )( )

[( )( ) (

)( )( )]

501

A

(c) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( ) must be replaced by their values from 96. It is easy to see that is a decreasing function in taking into account the hypothesis ( ) ( ) it follows that there exists a unique

such that ( )

502

(d) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

503

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Where in ( )( ) must be replaced by their values from 96. It is easy to see

that is a decreasing function in taking into account the hypothesis ( ) ( ) it

follows that there exists a unique such that (( )

)

504

(a) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( ) must be replaced by their values from 96. It is easy to see that

is a decreasing function in taking into account the hypothesis ( ) ( ) it follows

that there exists a unique such that (( )

)

505

(b) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( )( ) must be replaced by their values from 96. It is easy to see

that is a decreasing function in taking into account the hypothesis ( ) ( ) it

follows that there exists a unique such that (( )

)

506

(c) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( )( ) must be replaced by their values from 96. It is easy to see

that is a decreasing function in taking into account the hypothesis ( ) ( ) it

follows that there exists a unique such that (( )

)

507

(d) By the same argument, the equations admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( )( ) must be replaced by their values from 96. It is easy to see

that is a decreasing function in taking into account the hypothesis ( ) ( ) it

follows that there exists a unique such that ( )

508

(e) By the same argument, the equations admit solutions if ( ) (

)( )( )( ) ( )

( )( )( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( ) Where in ( )( ) must be replaced by their values from 96. It is easy to see that is a decreasing function in taking into account the hypothesis ( ) ( ) it follows that there exists a unique

such that ( )

509

(f) By the same argument, the equations admit solutions if

510

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( ) ( )( )(

)( ) ( )( )( )

( ) [(

)( )( )( )( ) (

)( )( )( )( )] (

)( )( )( )( )( )

Where in ( )( ) must be replaced by their values from 96. It is easy to see that is a decreasing function in taking into account the hypothesis ( ) ( ) it follows that there exists a unique

such that ( )

(g) By the same argument, the equations 92,93 admit solutions if

( ) ( )( )(

)( ) ( )( )( )

( )

[( )( )(

)( )( ) ( )( )(

)( )( )] ( )( )( )(

)( )( )

Where in ( )( ) must be replaced by their values from 96. It is easy to see

that is a decreasing function in taking into account the hypothesis ( ) ( ) it

follows that there exists a unique such that (( )

)

Finally we obtain the unique solution

( ) ,

( ) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

( )( )

[( )( ) (

)( )( )] ,

( )( )

[( )( ) (

)( )( )]

Obviously, these values represent an equilibrium solution

511

Finally we obtain the unique solution

(( )

) , (

) and 512

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

513

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )] 514

Obviously, these values represent an equilibrium solution

Finally we obtain the unique solution

(( )

) , (

) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

Obviously, these values represent an equilibrium solution of global equations

515

Finally we obtain the unique solution

( ) ,

( ) and

516

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( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

Obviously, these values represent an equilibrium solution of global equations

517

Finally we obtain the unique solution

(( )

) , (

) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

518

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

Obviously, these values represent an equilibrium solution of global equations

519

Finally we obtain the unique solution

(( )

) , (

) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

520

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

Obviously, these values represent an equilibrium solution of global equations

521

Finally we obtain the unique solution

(( ) ) ,

( ) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

522

Finally we obtain the unique solution

(( ) ) ,

( ) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

523

Finally we obtain the unique solution of 89 to 99

(( )

) , (

) and

( )( )

[( )( ) (

)( )( )]

,

( )( )

[( )( ) (

)( )( )]

523

A

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( )( )

[( )( ) (

)( )(( ) )] ,

( )( )

[( )( ) (

)( )(( ) )]

ASYMPTOTIC STABILITY ANALYSIS

Theorem 4: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( )

524

Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

525

((

)( ) ( )( )) ( )

( ) ( )( )

526

((

)( ) ( )( )) ( )

( ) ( )( )

527

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

528

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

529

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

530

ASYMPTOTIC STABILITY ANALYSIS

Theorem 4: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable

531

Proof: Denote

Definition of :-

,

532

( )( )

(

) ( )( ) ,

( )( )

( ( )

) 533

taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

534

((

)( ) ( )( )) ( )

( ) ( )( )

535

((

)( ) ( )( )) ( )

( ) ( )( )

536

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((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

537

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

538

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

539

ASYMPTOTIC STABILITY ANALYSIS

Theorem 4: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

540

Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

541

((

)( ) ( )( )) ( )

( ) ( )( )

542

((

)( ) ( )( )) ( )

( ) ( )( )

543

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

544

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

545

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

546

ASYMPTOTIC STABILITY ANALYSIS

Theorem 4: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

547

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

(( )

)

548

Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

549

((

)( ) ( )( )) ( )

( ) ( )( )

550

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((

)( ) ( )( )) ( )

( ) ( )( )

551

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

552

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

553

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

554

ASYMPTOTIC STABILITY ANALYSIS

Theorem 5: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

555

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

556

Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

557

((

)( ) ( )( )) ( )

( ) ( )( )

558

((

)( ) ( )( )) ( )

( ) ( )( )

559

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

560

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

561

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

562

ASYMPTOTIC STABILITY ANALYSIS

Theorem 6: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

563

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

564

Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

565

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((

)( ) ( )( )) ( )

( ) ( )( )

566

((

)( ) ( )( )) ( )

( ) ( )( )

567

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

568

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

569

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

570

ASYMPTOTIC STABILITY ANALYSIS Theorem 7: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable. Proof: Denote

571

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

572

Then taking into account equations and neglecting the terms of power 2, we obtain from

((

)( ) ( )( )) ( )

( ) ( )( )

573

((

)( ) ( )( )) ( )

( ) ( )( )

574

((

)( ) ( )( )) ( )

( ) ( )( )

575

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

576

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

578

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

579

Obviously, these values represent an equilibrium solution ASYMPTOTIC STABILITY ANALYSIS Theorem 8: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable. Proof: Denote

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

580

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Then taking into account equations and neglecting the terms of power 2, we obtain

((

)( ) ( )( )) ( )

( ) ( )( )

581

((

)( ) ( )( )) ( )

( ) ( )( )

582

((

)( ) ( )( )) ( )

( ) ( )( )

583

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

584

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

585

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

586

ASYMPTOTIC STABILITY ANALYSIS Theorem 9: If the conditions of the previous theorem are satisfied and if the functions

( )( ) (

)( ) Belong to ( )( ) then the above equilibrium point is asymptotically stable.

Proof: Denote

586A

Definition of :-

,

(

)( )

(

) ( )( ) ,

( )( )

( ( )

)

Then taking into account equations 89 to 99 and neglecting the terms of power 2, we obtain from 99 to 44

((

)( ) ( )( )) ( )

( ) ( )( )

586B

((

)( ) ( )( )) ( )

( ) ( )( )

586 C

((

)( ) ( )( )) ( )

( ) ( )( )

586 D

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

586 E

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

586 F

((

)( ) ( )( )) ( )

( ) ∑ ( ( )( ) )

586

G

The characteristic equation of this system is 587

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(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

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((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

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((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

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((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

+

(( )( ) ( )( ) ( )

( )) (( )( ) ( )( ) ( )

( ))

[((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )]

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( ) ( )( ) ( )

( ))( )( )

( )( )( )

( ) )

((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( ))

((( )( )) ( (

)( ) ( )( ) ( )

( ) ( )( )) ( )( )) ( )

( )

(( )( ) ( )( ) ( )

( )) (( )( )( )

( ) ( )

( )( )( )( )

( ) )

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((( )( ) ( )( ) ( )

( )) ( ) ( ) ( )

( ) ( ) ( ) )

And as one sees, all the coefficients are positive. It follows that all the roots have negative real part,

and this proves the theorem.

References

(1) Z-Theory and its applications by Sir Allan Zade

(2) ^ Abraham Pais, Inward Bound: Of Matter and Forces in the Physical World ISBN 0-19-

851997-4. Pais recounts how his astonishment at the rapidity with which Feynman could

calculate using his method. Feynman's method is now part of the standard methods for

physicists.

(3) ^ Newton, T.D.; Wigner, E.P. (1949). "Localized states for elementary particles". Reviews of

Modern Physics 21 (3): 400–

406. Bibcode 1949RvMP...21..400N.doi:10.1103/RevModPhys.21.400.

(4) Weinberg, S. Quantum Field Theory, Vols. I to III, 2000, Cambridge University Press:

Cambridge, UK.

(5) Feynman, R.P. (2001) [1964]. The Character of Physical Law. MIT Press. ISBN 0-262-56003-

8.

(6) Feynman, R.P. (2006) [1985]. QED: The Strange Theory of Light and Matter. Princeton

University Press. ISBN 0-691-12575-9.

(7) Gribbin, J. (1998). Q is for Quantum: Particle Physics from A to Z. Weidenfeld &

Nicolson. ISBN 0-297-81752-3.

(8) Schumm, Bruce A. (2004) Deep Down Things. Johns Hopkins Univ. Press. Chpt. 4.

(9) Bogoliubov, N.; Shirkov, D. (1982). Quantum Fields. Benjamin-Cummings. ISBN 0-8053-

0983-7.

(10) Frampton, P.H. (2000). Gauge Field Theories. Frontiers in Physics (2nd ed.). Wiley.

(11) Greiner, W; Müller, B. (2000). Gauge Theory of Weak Interactions. Springer. ISBN 3-540-

67672-4.

(12) Itzykson, C.; Zuber, J.-B. (1980). Quantum Field Theory. McGraw-Hill. ISBN 0-07-032071-3.

(13) Kane, G.L. (1987). Modern Elementary Particle Physics. Perseus Books. ISBN 0-201-11749-5.

(14) Kleinert, H.; Schulte-Frohlinde, Verena (2001). Critical Properties of φ4-Theories. World

Scientific. ISBN 981-02-4658-7.

(15) Kleinert, H. (2008). Multivalued Fields in Condensed Matter, Electrodynamics, and

Gravitation. World Scientific. ISBN 978-981-279-170-2.

(16) Loudon, R (1983). The Quantum Theory of Light. Oxford University Press. ISBN 0-19-

851155-8.

(17) Mandl, F.; Shaw, G. (1993). Quantum Field Theory. John Wiley & Sons. ISBN [[Special:

BookSources/00471941867|00471941867]].

(18) Peskin, M.; Schroeder, D. (1995). An Introduction to Quantum Field Theory. Westview

Press. ISBN 0-201-50397-2.

(19) Ryder, L.H. (1985). Quantum Field Theory. Cambridge University Press. ISBN 0-521-33859-

X.

(20) Srednicki, Mark (2007) Quantum Field Theory. Cambridge Univ. Press.

(21) Yndurain, F.J. (1996). Relativistic Quantum Mechanics and Introduction to Field Theory (1st

Ed.). Springer. ISBN 978-3-540-60453-2.

(22) Zee, A. (2003). Quantum Field Theory in a Nutshell. Princeton University Press. ISBN 0-691-

01019-6.

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