Exponential decay of correlation functions in many-electron systems
arXiv:1002.0772 · doi:10.1063/1.3409395
Abstract
For a class of tight-binding many-electron models on hyper-cubic lattices the equal-time correlation functions at non-zero temperature are proved to decay exponentially in the distance between the center of positions of the electrons and the center of positions of the holes. The decay bounds hold in any space dimension in the thermodynamic limit if the interaction is sufficiently small depending on temperature. The proof is based on the U(1)-invariance property and volume-independent perturbative bounds of the finite dimensional Grassmann integrals formulating the correlation functions.
52 pages, minor changes, final version, to appear in J. Math. Phys
References in corpus (5)
- Decay of Superconducting and Magnetic Correlations in One- and Two-Dimensional Hubbard Models
- Determinant Bounds and the Matsubara UV Problem of Many-Fermion Systems
- Does the Hubbard Model Show Superconductivity?
- Positivity and Convergence in Fermionic Quantum Field Theory
- A rigorous treatment of the perturbation theory for many-electron systems
Cited by in corpus (5)
- Superconducting phase in the BCS model with imaginary magnetic field
- Renormalization group analysis of multi-band many-electron systems at half-filling
- Superconducting phase in the BCS model with imaginary magnetic field. III. Non-vanishing free dispersion relations
- A Bayesian Mark Interaction Model for Analysis of Tumor Pathology Images
- The zero-temperature limit of the free energy density in many-electron systems at half-filling