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@ARTICLE{Nghiem:902441,
author = {Nghiem, H. T. M. and Costi, Theodoulos},
title = {{S}elf-energy method for time-dependent spectral functions
of the {A}nderson impurity model within the time-dependent
numerical renormalization group approach},
journal = {Physical review / B},
volume = {104},
number = {20},
issn = {1098-0121},
address = {Woodbury, NY},
publisher = {Inst.},
reportid = {FZJ-2021-04263},
pages = {205113},
year = {2021},
abstract = {The self-energy method for quantum impurity models
expresses the correlation part of the self-energy in terms
of the ratio of two Green's functions and allows for a more
accurate calculation of equilibrium spectral functions than
is possible directly from the one-particle Green's function
[Bulla et al., J. Phys.: Condens. Matter 10, 8365 (1998)],
for example, within the numerical renormalization group
method. In addition, the self-energy itself is a central
quantity required in the dynamical mean field theory of
strongly correlated lattice models. Here, we show how to
generalize the self-energy method to the time-dependent
situation for the prototype model of strong correlations,
the Anderson impurity model. We use the equation-of-motion
method to obtain closed expressions for the local Green's
function in terms of a time-dependent correlation
self-energy, with the latter being given as a ratio of a
one-particle time-dependent Green's function and a
higher-order correlation function. We benchmark this
self-energy approach to time-dependent spectral functions
against the direct approach within the time-dependent
numerical renormalization group method. The self-energy
approach improves the accuracy of time-dependent spectral
function calculations, and the closed-form expressions for
the Green's function allow for a clear picture of the time
evolution of spectral features at the different
characteristic time scales. The self-energy approach is of
potential interest also for other quantum impurity solvers
for real-time evolution, including time-dependent density
matrix renormalization group and continuous-time quantum
Monte Carlo techniques.},
cin = {IAS-3},
ddc = {530},
cid = {I:(DE-Juel1)IAS-3-20090406},
pnm = {5213 - Quantum Nanoscience (POF4-521)},
pid = {G:(DE-HGF)POF4-5213},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000719865400004},
doi = {10.1103/PhysRevB.104.205113},
url = {https://juser.fz-juelich.de/record/902441},
}