% IMPORTANT: The following is UTF-8 encoded. This means that in the presence
% of non-ASCII characters, it will not work with BibTeX 0.99 or older.
% Instead, you should use an up-to-date BibTeX implementation like “bibtex8” or
% “biber”.
@ARTICLE{Bulava:473389,
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 $\sigma$-model},
reportid = {PUBDB-2022-00012, arXiv:2111.12774. DESY-21-201.
HU-EP-21/49},
year = {2021},
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 $\sigma$-model, analogous to the
QCD part of ${e}^+{e}^- \rightarrow \rm {hadrons}$. 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 $j \rightarrow {\rm X}$ 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 $\epsilon$.
The smooth energy dependence of the underlying spectral
density enables a controlled $\epsilon \to 0$ extrapolation
in the inelastic region, yielding the real-time inclusive
rate without reference to individual finite-volume energies
or matrix elements. Systematic uncertainties due 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)},
cin = {$Z_ZPPT$},
cid = {$I:(DE-H253)Z_ZPPT-20210408$},
pnm = {611 - Fundamental Particles and Forces (POF4-611)},
pid = {G:(DE-HGF)POF4-611},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)25},
eprint = {2111.12774},
howpublished = {arXiv:2111.12774},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2111.12774;\%\%$},
doi = {10.3204/PUBDB-2022-00012},
url = {https://bib-pubdb1.desy.de/record/473389},
}