% 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{Arco:602032,
author = {Arco, F. and Heinemeyer, S. and Mühlleitner, M. and
Radchenko, K.},
title = {{S}ensitivity to triple {H}iggs couplings via di-{H}iggs
production in the 2{HDM} at the ({HL}-){LHC}},
journal = {The European physical journal / C},
volume = {83},
number = {11},
issn = {1434-6044},
address = {Heidelberg},
publisher = {Springer},
reportid = {PUBDB-2024-00480, arXiv:2212.11242. DESY-22-203.
IFT-UAM/CSIC-22-073. KA-TP-30-2022},
pages = {1019},
year = {2023},
note = {43 pages, 26 figures},
abstract = {An important task of the LHC is the investigation of the
Higgs-boson sector. Of particular interest is the
reconstruction of the Higgs potential, i.e. the measurement
of the Higgs self-couplings. Based on previous analyses,
within the 2-Higgs-Doublet Model (2HDM) type I, we analyze
several two-dimensional benchmark planes that are over large
parts in agreement with all theoretical and experimental
constraints. For these planes we evaluate di-Higgs
production cross sections at the (HL-)LHC with a
center-of-mass energy of $14 \,\, \textrm{TeV}$ at
next-to-leading order in the heavy top-quark limit with the
code HPAIR. We investigate in particular the process $gg
\rightarrow hh$, with h being the Higgs boson discovered at
the LHC with a mass of about $125 \,\, \textrm{GeV}$. The
top box diagram of the loop-mediated gluon fusion process
into Higgs pairs interferes with the s-channel exchange of
the two ${\mathcal{C}\mathcal{P}}$-even 2HDM Higgs bosons h
and H. The latter two involve the triple Higgs couplings
(THCs) $\lambda _{hhh}$ and $\lambda _{hhH}$, respectively,
possibly making them accessible at the HL-LHC. Depending on
the size of the involved top-Yukawa and THCs as well as on
the mass of H, the contribution of the s-channel H diagram
can be dominating or be highly suppressed. We find regions
of the allowed parameter space in which the di-Higgs
production cross section can differ by many standard
deviations from its SM prediction, indicating possible
access to deviations in $\lambda _{hhh}$ from the SM value
$\lambda _{\textrm{SM}}$ and/or contributions involving
$\lambda _{hhH}$. The sensitivity to the beyond-the-SM (BSM)
THC $\lambda _{hhH}$ is further analyzed employing the
$m_{hh}$ distributions. We demonstrate how a possible
measurement of $\lambda _{hhH}$ depends on the various
experimental uncertainties. Depending on the underlying
parameter space, the HL-LHC may have the option not only to
detect BSM THCs, but also to provide a first rough
measurement of their sizes.},
keywords = {Higgs particle: doublet: 2 (INSPIRE) / potential: Higgs
(INSPIRE) / coupling: Higgs (INSPIRE) / top: coupling
(INSPIRE) / Higgs particle: pair production (INSPIRE) /
gluon: fusion (INSPIRE) / sensitivity (INSPIRE) / CERN LHC
Coll: upgrade (INSPIRE) / numerical calculations (INSPIRE) /
new physics (INSPIRE)},
cin = {T},
ddc = {530},
cid = {I:(DE-H253)T-20120731},
pnm = {611 - Fundamental Particles and Forces (POF4-611) / DFG
project G:(GEPRIS)390833306 - EXC 2121: Quantum Universe
(390833306) / HIDDeN - Hunting Invisibles: Dark sectors,
Dark matter and Neutrinos (860881)},
pid = {G:(DE-HGF)POF4-611 / G:(GEPRIS)390833306 /
G:(EU-Grant)860881},
experiment = {EXP:(DE-MLZ)NOSPEC-20140101},
typ = {PUB:(DE-HGF)16},
eprint = {2212.11242},
howpublished = {arXiv:2212.11242},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2212.11242;\%\%$},
UT = {WOS:001100008300001},
doi = {10.1140/epjc/s10052-023-12193-4},
url = {https://bib-pubdb1.desy.de/record/602032},
}