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

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

2 Outline 1)Motivation 2)Generalized Pauli Constraints 3)Application to Physics 4)Pinning Analysis 5)Physical Relevance of Pinning

3 1) Motivation Pauli’s exclusion principle (1925): `no two identical fermions in the same quantum state’ mathematically: relevant when Aufbau principle for atoms (quasi-) pinned by

4 `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 (?)

5 mathematical objects ? N-fermion states 1-particle reduced density operator natural occupation numbers partial trace translate antisymmetry of to 1-particle picture

6 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:A:

7 0 1 1 Pauli exclusion principle [A.Klyachko., CMP 282, p287-322, 2008] [A.Klyachko, J.Phys 36, p72-86, 2006] Polytope

8 polytope intersection of finitely many half spaces = facet: half space:

9 Example: N = 3 & d= 6 [Borland&Dennis, J.Phys. B, 5,1, 1972] [Ruskai, Phys. Rev. A, 40,45, 2007]

10 Position of relevant states (e.g. ground state) ? or here ? (pinning) here ? point on boundary : kinematical constraints generalization of: decay impossible 0 1 1 3) Application to Physics

11 N non-interacting fermions: effectively 1-particle problem with solution with N-particle picture: 1-particle picture: ( )

12 Pauli exclusion principle constraints exactly pinned! 0 1 1 Slater determinants

13 requirements for non-trivial model? N identical fermions with coupling parameter analytical solvable: depending on

14 Hamiltonian: diagonalization of length scales:

15 Now: Fermions restrict to ground state: [Z.Wang et al., arXiv 1108.1607, 2011] if non-interacting

16 properties of : depends only on i.e. on non-trivial duality weak-interacting from now on :

17 `Boltzmann distribution law’: hierarchy: Thanks to Jürg Fröhlich

18 too difficult/ not known yet instead: check w.r.t 4) Pinning Analysis

19 relevant as long as lower bound on pinning order

20 relevant as long as quasi-pinning

21 moreover : larger ? - quasi-pinning poster 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!:

22 saturated by : Implication for corresponding ? 5) Physical Relevance of Pinning Physical Relevance of Pinning ?

23 generalization of: stable:

24

25 Selection Rule:

26 Example: Pinning of dimension

27 Application: Improvement of Hartree-Fock approximate unknown ground state Hartree-Fock much better:

28 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-Fock e.g. Pinning is physically relevant Fermionic Ground States simpler than appreciated (?)

29 Outlook Hubbard model Quantum Chemistry: Atoms Physical & mathematical Intuition for Pinning HOMO- LUMO- gap Strongly correlated Fermions Antisymmetry Energy Minimization generic for:

30 Thank you!


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