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@ARTICLE{Lu:910664,
author = {Lu, Bing-Nan and Li, Ning and Elhatisari, Serdar and Ma,
Yuan-Zhuo and Lee, Dean and Meißner, Ulf-G.},
title = {{P}erturbative {Q}uantum {M}onte {C}arlo {M}ethod for
{N}uclear {P}hysics},
journal = {Physical review letters},
volume = {128},
number = {24},
issn = {0031-9007},
address = {College Park, Md.},
publisher = {APS},
reportid = {FZJ-2022-04037},
pages = {242501},
year = {2022},
note = {We gratefully acknowledge funding by NSAF (Grant No.
U1930403), the Deutsche Forschungsgemeinschaft (DFG, German
Research Foundation) and the NSFC through the funds provided
to the Sino-German Collaborative Research Center TRR110
“Symmetries and the Emergence of Structure in QCD” (DFG
Project ID 196253076 - TRR 110, NSFC Grant No. 12070131001),
the Chinese Academy of Sciences (CAS) President’s
International Fellowship Initiative (PIFI) (Grant No.
2018DM0034), Volkswagen Stiftung (Grant No. 93562), the
European Research Council (ERC) under the European Union’s
Horizon 2020 research and innovation programme (grant
agreement No. 101018170) and the U.S. Department of Energy
(DE-SC0013365 and DE-SC0021152) and the Nuclear
Computational Low-Energy Initiative (NUCLEI) SciDAC-4
project (DE-SC0018083) and the Scientific and Technological
Research Council of Turkey (TUBITAK project no. 120F341) and
the National Natural Science Foundation of China under
Grants No. 12105106 and the China Postdoctoral Science
Foundation under Grants No. BX20200136 and 2020M682747.},
abstract = {While first order perturbation theory is routinely used in
quantum Monte Carlo (QMC) calculations, higher-order terms
present significant numerical challenges. We present a new
approach for computing perturbative corrections in
projection QMC calculations. We demonstrate the method by
computing nuclear ground state energies up to second order
for a realistic chiral interaction. We calculate the binding
energies of several light nuclei up to 16O by expanding the
Hamiltonian around the Wigner SU(4) limit and find good
agreement with data. In contrast to the natural ordering of
the perturbative series, we find remarkably large second
order energy corrections. This occurs because the perturbing
interactions break the symmetries of the unperturbed
Hamiltonian. Our method is free from the sign problem and
can be applied to QMC calculations for many-body systems in
nuclear physics, condensed matter physics, ultracold atoms,
and quantum chemistry.},
cin = {IAS-4},
ddc = {530},
cid = {I:(DE-Juel1)IAS-4-20090406},
pnm = {5111 - Domain-Specific Simulation Data Life Cycle Labs
(SDLs) and Research Groups (POF4-511) / DFG project
196253076 - TRR 110: Symmetrien und Strukturbildung in der
Quantenchromodynamik (196253076) / Nuclear Lattice
Simulations $(jara0015_20200501)$},
pid = {G:(DE-HGF)POF4-5111 / G:(GEPRIS)196253076 /
$G:(DE-Juel1)jara0015_20200501$},
typ = {PUB:(DE-HGF)16},
pubmed = {35776463},
UT = {WOS:000820702500005},
doi = {10.1103/PhysRevLett.128.242501},
url = {https://juser.fz-juelich.de/record/910664},
}