Intrinsic Semi Conductor Materials

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    Intrinsicemi-conductor

    Materials

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    Introduction

    Intrinsic semiconductors aresemiconductors which do not contain

    impurities. They do contain electrons as

    well as holes. The electron densityequals the hole density since the

    thermal activation of an electron from

    the valence band to the conduction bandyields a free electron in the conduction

    band as well as a free hole in the

    valence band.

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    Introduction

    Intrinsic by denition means natural orinherent, and intrinsic semiconductors

    are the bulk properties of the

    semiconductor material itself, not thoseof dopants or impurities. Silicon and

    germanium are the two most commonly

    used eamples of intrinsicsemiconductors, as they are elementalsemiconductors and were some of the

    rst widely studied and usedsemiconductors.

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    Semiconductor Structure

    The electronic structure ofsemiconductors are the foundation of

    their unique properties. Themechanisms which make

    semiconductors their own class ofmaterial is based on the electricalstructure, which dictates the core

    properties of semiconductors.

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    The most well known electricconductors are metals. !etals are able

    to carry an electric "ow because of

    their available free electrons that canpass from one atom to the net. This

    enables the electric "ow #which is

    merely composed of electrons "owingacross a substance$ to travel through

    the length of the metal.

    Semiconductor Structure

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    Semiconductors work in a verydi%erent manner. &ll intrinsicsemiconductors are group 14

    elements, and thusly only have 'valence ( electrons available forbonding in their outermost shell.

    )ecause of these ' electrons, group*' elements like Silicon are able to

    form crystal lattice structures

    composed of countless atoms of that

    Semiconductor Structure

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    Semiconductor Structure

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    Band Theory

    !etals and semiconductors have aunique property that separates them

    from non+conductive insulators. In

    metals and insulators, the di%erencebetween energy orbitals are so small

    that electrons can be ecited from lower

    energy orbitals to higher energy levels.These small orbital energy di%erences

    are referred to as bands.

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    Band Theory

    nlike the discrete energy levels thatyou are taught about in beginning

    chemistry, these bands are so close

    together in energy that it takes a verysmall amount of energy to promoteelectrons to these higher band levels.

    The higher energy level that thevalence electrons can be ecited to isreferred to as the conduction band,

    because the electrons in this band are

    free to carry an electric current.

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    Band Theory

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    Hole Conduction

    )y denition, an electron hole isthe opposite of an electron. It

    represents the lack of an electronwhere an electron could potentially

    be situated or previously wassituated in an otherwise full

    electron shell. In this case,electron holes result from electrons

    leaving their place in the lattice

    structure .

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    Hole Conduction

    -nce heat is put into thesemiconductor and electrons begin

    continually crossing into the

    conduction band, hole conductionbegins constantly moving electronsacross the semiconductor, addingto the overall electron "ow. This

    increases the conductive ability ofthe semiconductor, constantly

    allowing new electrons to cross into

    the conduction gap.

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    Hole Conduction

    lectron holes have an important rolein increasing the conductive abilitiesof semiconductors. /ole conduction

    rst requires an electron toeperience ecitation in order to leave

    its valence band to the conduction

    band. -nce the valence electron hasleft, neighboring electrons are pulledinto the electron holes, lling eisting

    electron holes while creating newneighboring ones.

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