Pinning of Fermionic Occupation Numbers

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Pinning of Fermionic Occupation Numbers Christian Schilling ETH Zürich in collaboration with M.Christandl, D.Ebler, D.Gross Phys. Rev. Lett. 110, 040404 (2013)

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Pinning of Fermionic Occupation Numbers. Christian Schilling ETH Zürich. in collaboration with M.Christandl , D.Ebler , D.Gross. Phys. Rev . Lett . 110 , 040404 (2013). Outline. Motivation Generalized Pauli Constraints Application to Physics Pinning Analysis - PowerPoint PPT Presentation

Transcript of Pinning of Fermionic Occupation Numbers

Page 1: Pinning of Fermionic Occupation  Numbers

Pinning of Fermionic Occupation Numbers

Christian SchillingETH Zürich

in collaboration with

M.Christandl, D.Ebler, D.Gross

Phys. Rev. Lett. 110, 040404 (2013)

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Outline

1) Motivation

2) Generalized Pauli Constraints

3) Application to Physics

4) Pinning Analysis

5) Physical Relevance of Pinning

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1) MotivationPauli’s exclusion principle (1925):

`no two identical fermions in

the same quantum state’

mathematically:

relevant when

Aufbau principle for atoms

(quasi-) pinned by(quasi-) pinned by

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`quantum states of identical

fermions are antisymmetric’

strengthened by Dirac & Heisenberg in (1926):

implications for occupation numbers ?

further constraints beyond

but only relevant if (quasi-) pinned (?)

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mathematical objects ?

N-fermion states

1-particle reduced density operator

natural occupationnumbers

partial trace

translate antisymmetry of

to 1-particle picture

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Q: Which 1-RDO are possible?

2) Generalized Pauli Constraints

(Fermionic Quantum Marginal Problem)

describe this set

unitary equivalence:

only natural occupation numbers relevant

A:

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0

1

1

Pauli exclusion principle[A.Klyachko., CMP 282, p287-322, 2008][A.Klyachko, J.Phys 36, p72-86, 2006]

Polytope

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polytope

intersection offinitely many half

spaces

=

facet:

half space:

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Example: N = 3 & d= 6

[Borland&Dennis, J.Phys. B, 5,1, 1972]

[Ruskai, Phys. Rev. A, 40,45, 2007]

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Position of relevant states(e.g. ground state) ?

or here ? (pinning)

here ?

point on boundary :

kinematical constraints

generalization of:

decayimpossible

0

1

1

3) Application to Physics

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N non-interacting fermions:

effectively 1-particle problem

with solution

with

N-particle picture: 1-particle picture:

( )

( )

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Pauli exclusion principle constraints

exactly pinned!

0

1

1

Slaterdeterminants

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requirements for non-trivial model?

N identical fermions with coupling parameter

analytical solvable:

depending on

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Hamiltonian:

diagonalization of

length scales:

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Now: Fermions

restrict to

ground state: [Z.Wang et al., arXiv 1108.1607, 2011]

if non-interacting

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properties of :

depends only on i.e. on

non-trivial duality

weak-interacting

from now on :

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`Boltzmann distribution law’:

hierarchy:

Thanks toJürg Fröhlich

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too difficult/ not known yet

instead: check w.r.t

4) Pinning Analysis

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relevant as long as

lower bound on pinning order

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relevant as long as

quasi-pinning

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moreover :

larger ?

- quasi-pinningposter by Daniel Ebler

excitations ?first few still quasi-pinned

weaker with increasing excitation

quasi-pinning a ground state effect !?

quasi-pinnig only for weak interaction ?

No!:

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saturated by :

Implication for corresponding ?

5) Physical Relevance of Pinning

Physical Relevance of Pinning ?

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generalization of:

stable:

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Selection Rule:

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Example:

Pinning of

dimension

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Application: Improvement of Hartree-Fock

approximate unknown ground state

Hartree-Fock

much better:

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Conclusions

antisymmetry of translated to 1-particle picture

Generalized Pauli constraints

study of fermion – model with coupling

Pauli constraints pinned up to corrections

Generalized Pauli constraints pinned up to corrections

improve Hartree-Focke.g.

Pinning is physically relevant

Fermionic Ground States simpler than appreciated (?)

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Outlook

Hubbard model

Quantum Chemistry: Atoms

Physical & mathematical Intuition

for Pinning

HOMO-LUMO-

gap

Strongly correlated Fermions

Antisymmetry Energy Minimization

generic for:

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Thank you!