In conventional Green's function methods the vertex function \ensuremath{\Gamma} is generally energy dependent. However, a model-space Green's function method where the vertex function is manifestly energy independent can be formulated using energy-independent effective interaction theories based on folded diagrams and/or similarity transformations. This is discussed in general and then illustrated for a 1p1h model-space Green's function applied to a solvable Lipkin many-fermion model. The poles of the conventional Green's function are obtained by solving a self-consistent Dyson equation and model space calculations may lead to unphysical poles. For the energy-independent model-space Green's function only the physical poles of the model problem are reproduced and are in satisfactory agreement with the exact excitation energies. \textcopyright{} 1996 The American Physical Society.In conventional Green's function methods the vertex function \ensuremath{\Gamma} is generally energy dependent. However, a model-space Green's function method where the vertex function is manifestly energy independent can be formulated using energy-independent effective interaction theories based on folded diagrams and/or similarity transformations. This is discussed in general and then illustrated for a 1p1h model-space Green's function applied to a solvable Lipkin many-fermion model. The poles of the conventional Green's function are obtained by solving a self-consistent Dyson equation and model space calculations may lead to unphysical poles. For the energy-independent model-space Green's function only the physical poles of the model problem are reproduced and are in satisfactory agreement with the exact excitation energies. \textcopyright{} 1996 The American Physical Society.

Physical Review CMar 1, 19960 citations

Some Analytic Properties of Green Functions and Self-Energy Parts for a System of Interacting Bosons

W. E. Parry, Roy E. Turner

Some analytic properties of the single-particle Green functions and proper self-energy parts for a system of interacting bosons at nonzero temperatures are derived. In particular, it is shown how to obtain the analytical continuations of simple functions of the proper self-energy parts, which can be obtained from perturbation theory at an infinite set of points along the imaginary energy axis, to the whole of the complex energy plane. This is useful in determining the poles of the Green functions.Some analytic properties of the single-particle Green functions and proper self-energy parts for a system of interacting bosons at nonzero temperatures are derived. In particular, it is shown how to obtain the analytical continuations of simple functions of the proper self-energy parts, which can be obtained from perturbation theory at an infinite set of points along the imaginary energy axis, to the whole of the complex energy plane. This is useful in determining the poles of the Green functions.

Journal of Mathematical PhysicsApr 1, 19630 citations

Green function and excitation of a singular oscillator

V. V. Dodonov, I.A. Malkin, Vladimir I. Man’ko

Physics Letters AJun 1, 197222 citations

Unified role of Green's function poles and zeros in correlated topological insulators

Andrea Blason, Michele Fabrizio

Green's function zeros, which can emerge only if correlation is strong, have been for long overlooked and believed to be devoid of any physical meaning, unlike Green's function poles. Here, we prove that Green's function zeros instead contribute on the same footing as poles to determine the topological character of an insulator. The key to the proof, worked out explicitly in two dimensions but easily extendable in three dimensions, is to express the topological invariant in terms of a quasiparticlethermal Green's function matrix ${G}_{*}(i\ensuremath{\epsilon},\mathbf{k})=1/[i\ensuremath{\epsilon}\ensuremath{-}{H}_{*}(\ensuremath{\epsilon},\mathbf{k})]$, with Hermitian ${H}_{*}(\ensuremath{\epsilon},\mathbf{k})$, by filtering out the positive-definite quasiparticle residue. In that way, the topological invariant is easily found to reduce to the Thouless, Kohmoto, Nightingale, and den Nijs formula for quasiparticles described by the noninteracting Hamiltonian ${H}_{*}(0,\mathbf{k})$ . Since the poles of the quasiparticle Green's function ${G}_{*}(\ensuremath{\epsilon},\mathbf{k})$ on the real frequency axis correspond to poles and zeros of the physical-particle Green's function $G(\ensuremath{\epsilon},\mathbf{k})$, both of them equally determine the topological character of an insulator.Green's function zeros, which can emerge only if correlation is strong, have been for long overlooked and believed to be devoid of any physical meaning, unlike Green's function poles. Here, we prove that Green's function zeros instead contribute on the same footing as poles to determine the topological character of an insulator. The key to the proof, worked out explicitly in two dimensions but easily extendable in three dimensions, is to express the topological invariant in terms of a quasiparticlethermal Green's function matrix ${G}_{*}(i\ensuremath{\epsilon},\mathbf{k})=1/[i\ensuremath{\epsilon}\ensuremath{-}{H}_{*}(\ensuremath{\epsilon},\mathbf{k})]$, with Hermitian ${H}_{*}(\ensuremath{\epsilon},\mathbf{k})$, by filtering out the positive-definite quasiparticle residue. In that way, the topological invariant is easily found to reduce to the Thouless, Kohmoto, Nightingale, and den Nijs formula for quasiparticles described by the noninteracting Hamiltonian ${H}_{*}(0,\mathbf{k})$. Since the poles of the quasiparticle Green's function ${G}_{*}(\ensuremath{\epsilon},\mathbf{k})$ on the real frequency axis correspond to poles and zeros of the physical-particle Green's function $G(\ensuremath{\epsilon},\mathbf{k})$, both of them equally determine the topological character of an insulator.

arXiv:2304.08180Physical review. B./Physical review. BSep 11, 202340 citations

{H}_{*}(0,\mathbf{k})

. Since the poles of the quasiparticle Green's function ${G}_{*}(\ensuremath{\epsilon},\mathbf{k})$ on the real frequency axis correspond to poles and zeros of the physical-particle Green's function $G(\ensuremath{\epsilon},\mathbf{k})$, both of them equally determine the topological character of an insulator.