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Excitation spectrum and staggering transformations in lattice quantum models
Paulo A Faria da Veiga1, Michael O'Carroll, Ricardo Schor
1Departamento de Matemática, ICMC-USP, Caixa Postal 668, 13560-970 São Carlos, São Paulo, Brazil. veiga@icmc.sc.usp.br
Physical Review. E, Statistical, Nonlinear, and Soft Matter Physics
|September 21, 2002
Summary
This study analyzes the energy-momentum spectrum of various lattice Hamiltonians. It reveals that bound states can exist below or above the two-particle band, depending on interaction type and lattice dimension.
Area of Science:
- Condensed Matter Physics
- Quantum Field Theory
- Statistical Mechanics
Background:
- Investigating excitation spectra in diverse lattice Hamiltonian systems is crucial for understanding fundamental physical phenomena.
- Lattice Hamiltonians model systems ranging from quantum field theories to classical spin systems.
Purpose of the Study:
- To analyze the energy-momentum excitation spectrum of various lattice Hamiltonian operators.
- To determine the conditions for the existence of bound states in relation to the two-particle band.
Main Methods:
- Utilized a lattice version of the Bethe-Salpeter equation to determine the two-particle spectrum.
- Employed a nonrelativistic single-particle lattice Schrödinger Hamiltonian with a delta potential for analysis.
- Applied a staggering transformation to relate attractive and repulsive interaction cases.
Main Results:
- The low-lying spectrum consistently features a one-particle state and a two-particle band.
- Bound states can appear below (attractive interaction) or above (repulsive interaction) the two-particle band.
- The existence of these bound states is linked to the lattice dimension and interaction character.
Conclusions:
- The study provides a unified framework for understanding bound state formation in diverse lattice systems.
- The findings offer insights into the behavior of quantum and classical systems on a lattice.
- The connection to single-particle Schrödinger Hamiltonians simplifies the interpretation of complex many-body phenomena.