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@ARTICLE{Bulava:470529,
author = {Bulava, John and Hansen, Maxwell T. and Hansen, Michael W.
and Patella, Agostino and Tantalo, Nazario},
title = {{I}nclusive rates from smeared spectral densities in the
two-dimensional {O}(3) non-linear $σ$-model},
journal = {Journal of high energy physics},
volume = {07},
number = {7},
issn = {1029-8479},
address = {[Trieste]},
publisher = {SISSA},
reportid = {PUBDB-2021-04207, DESY-21-201. arXiv:2111.12774.
HU-EP-21/49},
pages = {034},
year = {2022},
note = {26 pages, 11 figures},
abstract = {This work employs the spectral reconstruction approach of
ref. [1] to determine an inclusive rate in the 1 + 1
dimensional O(3) non-linear σ-model, analogous to the QCD
part of e$^{+}$e$^{−}$ → hadrons. The Euclidean
two-point correlation function of the conserved current j is
computed using Monte Carlo lattice field theory simulations
for a variety of spacetime volumes and lattice spacings. The
spectral density of this correlator is related to the
inclusive rate for j → X in which all final states
produced by the external current are summed. The ill-posed
inverse problem of determining the spectral density from the
correlation function is made tractable through the
determination of smeared spectral densities in which the
desired density is convolved with a set of known smearing
kernels of finite width ϵ. The smooth energy dependence of
the underlying spectral density enables a controlled ϵ →
0 extrapolation in the inelastic region, yielding the
real-time inclusive rate without reference to individual
finite-volume energies or matrix elements. Systematic
uncertainties due to cutoff effects and residual
finite-volume effects are estimated and taken into account
in the final error budget. After taking the continuum limit,
the results are consistent with the known analytic rate to
within the combined statistical and systematic errors. Above
energies where 20-particle states contribute, the overall
precision is sufficient to discern the four-particle
contribution to the spectral density.},
keywords = {density: spectral (INSPIRE) / width: finite (INSPIRE) /
finite size: effect (INSPIRE) / density: correlation
function (INSPIRE) / dimension: 2 (INSPIRE) / current:
conservation law (INSPIRE) / O(3) (INSPIRE) / sigma model:
nonlinear (INSPIRE) / quantum chromodynamics (INSPIRE) /
Euclidean (INSPIRE) / lattice (INSPIRE) / lattice field
theory (INSPIRE) / statistical (INSPIRE) / continuum limit
(INSPIRE) / energy dependence (INSPIRE) / hadron (INSPIRE) /
Monte Carlo (INSPIRE) / Lattice Quantum Field Theory
(autogen) / Sigma Models (autogen)},
cin = {$Z_APR$ / $Z_ZPPT$},
ddc = {530},
cid = {$I:(DE-H253)Z_APR-20201126$ / $I:(DE-H253)Z_ZPPT-20210408$},
pnm = {611 - Fundamental Particles and Forces (POF4-611) / GRK
2575 - GRK 2575: Überdenken der Quantenfeldtheorie
(417533893)},
pid = {G:(DE-HGF)POF4-611 / G:(GEPRIS)417533893},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2111.12774},
howpublished = {arXiv:2111.12774},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2111.12774;\%\%$},
UT = {WOS:000821876500002},
doi = {10.1007/JHEP07(2022)034},
url = {https://bib-pubdb1.desy.de/record/470529},
}