1972
DOI: 10.1063/1.1666120
|View full text |Cite
|
Sign up to set email alerts
|

Exactly Soluble Model of Interacting Electrons

Abstract: We diagonalize a many-fermion Hamiltonian consisting of terms quadratic as well as quartic in the field operators. A dual spectrum of eigenstates is an interesting result. We also derive a formula for obtaining the free energy at finite temperature.

Help me understand this report

Search citation statements

Order By: Relevance

Paper Sections

Select...
3
1
1

Citation Types

0
15
0

Year Published

1974
1974
2019
2019

Publication Types

Select...
7
1

Relationship

0
8

Authors

Journals

citations
Cited by 13 publications
(15 citation statements)
references
References 6 publications
0
15
0
Order By: Relevance
“…This transformation was originally introduced by Mattis and Nam [54] to solve the following Hubbard-like model…”
Section: A Su (2) Heisenberg Magnetsmentioning
confidence: 99%
“…This transformation was originally introduced by Mattis and Nam [54] to solve the following Hubbard-like model…”
Section: A Su (2) Heisenberg Magnetsmentioning
confidence: 99%
“…The model is reduced to chain of spinless fermions (2) with the chemical potential U [13]. According to [13], the ground state degeneracy is dependent on whether κ = U τ (δ) > 4 or otherwise. In the thermodynamic limit there are zero energy Majorana states, they are realized in the interval |κ| ≤ 4.…”
Section: The Hofstadter Model Of Interacting Electronsmentioning
confidence: 99%
“…Such a criterion should connect the value of the gap of a topological insulator with the magnitude of the Coulomb repulsion between fermions. Taking into account the exact solution of fermion chain model [13], we calculate the stability of topological state in the Hofstadler model of interacting electrons. Result does not stripe geometry depend on the symmetry of the lattice, we believe that it is generic and can be applicable to different 2D topological insulators.…”
Section: Introductionmentioning
confidence: 99%
“…The Hubbard model with correlated hopping on a chain has been proposed and solved exactly in [3][4][5]. Mattic and Nam (MN) proposed modification of the Hubbard model for interacting electrons forming pairs, and solved it exactly in special point [6] (better known as the Kitaev point [7]). In contrast to traditional Hubbard model [1], the MN model describes topological states of interacting electrons [7][8][9], quantum topological phase transition between topological trivial and nontrivial phases.…”
Section: Introductionmentioning
confidence: 99%
“…In contrast to traditional Hubbard model [1], the MN model describes topological states of interacting electrons [7][8][9], quantum topological phase transition between topological trivial and nontrivial phases. In this context, it is interesting to discuss a new model, which is a modification [3,6], the exact solution of which takes place for arbitrary one-site interaction, correlated hopping and pairing.…”
Section: Introductionmentioning
confidence: 99%