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@ARTICLE{Hayrapetyan:646497,
author = {Hayrapetyan, Aram and others},
collaboration = {{CMS Collaboration}},
title = {{S}earch for a new resonance decaying to a {H}iggs boson
and a scalar boson in events with two b jets and two {Z}
bosons in proton-proton collisions at $\sqrt{s}$ = 13.6
{T}e{V}},
reportid = {PUBDB-2026-00884, arXiv:2602.18223. CMS-B2G-24-022.
CERN-EP-2026-020},
year = {2026},
note = {Submitted to Physical Review D. All figures and tables can
be found at
http://cms-results.web.cern.ch/cms-results/public-results/publications/B2G-24-022
(CMS Public Pages)},
abstract = {A search is performed for a new resonance X decaying into
either a pair of Higgs bosons (HH) or into a Higgs boson and
a new scalar boson Y (HY), using proton-proton collision
data collected at $\sqrt{s}$ = 13 TeV, corresponding to an
integrated luminosity of 138 fb$^{-1}$. This study performs
a comprehensive exploitation of the bbZZ events,
encompassing the following decay topologies. One H candidate
is identified through its decay into a bottom
quark-antiquark pair, while the other H or the Y candidate
is selected through its decay into a pair of Z bosons. One Z
boson is required to decay leptonically and the other, to
decay into a pair of quarks or neutrinos. Events of interest
are categorized based on the Lorentz boosts of the
hadronically decaying H and Z bosons. Machine-learning-based
discriminants, together with the reconstructed resonance
mass, are employed across the different categories to
separate signal from backgrounds, and their corresponding
distributions are included in a simultaneous fit. No
significant deviations from the standard model predictions
are observed. Upper limits at the 95\% confidence level are
set on the HH and HY production cross sections. For resonant
HH production, the upper limit on the cross section of pp
$\to$ HH production is 1 pb for a high-mass resonance. For
HY production, the upper limit on the cross section of the
process pp $\to$ X $\to$ bbZZ is approximately 5 fb for a
high-mass resonance. This is comparable to the sensitivity
achieved in other analyses, which focus on H decays to
$γγ$ or $ττ$ and Y decays into a pair of bottom quarks
or massive vector bosons.},
cin = {CMS},
cid = {I:(DE-H253)CMS-20120731},
pnm = {611 - Fundamental Particles and Forces (POF4-611) /
HIDSS-0002 - DASHH: Data Science in Hamburg - Helmholtz
Graduate School for the Structure of Matter
$(2019_IVF-HIDSS-0002)$ / DFG project G:(GEPRIS)390833306 -
EXC 2121: Das Quantisierte Universum II (390833306)},
pid = {G:(DE-HGF)POF4-611 / $G:(DE-HGF)2019_IVF-HIDSS-0002$ /
G:(GEPRIS)390833306},
experiment = {EXP:(DE-H253)LHC-Exp-CMS-20150101},
typ = {PUB:(DE-HGF)25},
eprint = {2602.18223},
howpublished = {arXiv:2602.18223},
archivePrefix = {arXiv},
SLACcitation = {$\%\%CITATION$ = $arXiv:2602.18223;\%\%$},
url = {https://bib-pubdb1.desy.de/record/646497},
}