CERN Accelerating science

CERN Document Server 1,869 records found  1 - 10nextend  jump to record: Search took 0.77 seconds. 
1.
Search for Higgs boson decays into a pair of pseudoscalar particles in the $\gamma\gamma\tau_{\text{had}}\tau_{\text{had}}$ final state using $pp$ collisions at $\sqrt{s}=13$ TeV with the ATLAS detector / ATLAS Collaboration
A search for exotic decays of the 125 GeV Higgs boson into a pair of new spin-0 particles, $H \to aa$, where one decays into a photon pair and the other into a $\tau$-lepton pair, is presented. [...]
arXiv:2412.14046 ; CERN-EP-2024-323.
- 2024 - 37 p, 37.
Fulltext - Previous draft version - Fulltext
2.
High-precision measurement of the W boson mass with the CMS experiment at the LHC / CMS Collaboration
In the standard model of particle physics, the masses of the carriers of the weak interaction, the W and Z bosons, are uniquely related. [...]
arXiv:2412.13872 ; CMS-SMP-23-002 ; CERN-EP-2024-308 ; CMS-SMP-23-002-003.
- 2024 - 73 p, 73.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
3.
Search for heavy neutral resonances decaying to tau lepton pairs in proton-proton collisions at $ \sqrt{s} = $ 13 TeV / CMS Collaboration
A search for heavy neutral gauge bosons (Z') decaying into a pair of tau leptons is performed in proton-proton collisions at $ \sqrt{s}= $ 13 TeV at the CERN LHC. [...]
arXiv:2412.04357 ; CMS-EXO-21-016 ; CERN-EP-2024-292 ; CMS-EXO-21-016-003.
- 2024 - 43.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
4.
Model-agnostic search for dijet resonances with anomalous jet substructure in proton-proton collisions at $ \sqrt{s} $ = 13 TeV / CMS Collaboration
This paper presents a model-agnostic search for narrow resonances in the dijet final state in the mass range 1.8-6 TeV. [...]
arXiv:2412.03747 ; CMS-EXO-22-026 ; CERN-EP-2024-291 ; CMS-EXO-22-026-003.
- 2024 - 55.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
5.
Precision calibration of calorimeter signals in the ATLAS experiment using an uncertainty-aware neural network / ATLAS Collaboration
The ATLAS experiment at the Large Hadron Collider explores the use of modern neural networks for a multi-dimensional calibration of its calorimeter signal defined by clusters of topologically connected cells (topo-clusters). [...]
arXiv:2412.04370 ; CERN-EP-2024-317.
- 2024 - 72.
Fulltext - Previous draft version - Fulltext
6.
Measurement of the inclusive WZ production cross section in pp collisions at $ \sqrt{s}= $ 13.6 TeV / CMS Collaboration
The inclusive WZ production cross section is measured in proton-proton collisions at a centre-of-mass energy of 13.6 TeV, using data collected during 2022 with the CMS detector, corresponding to an integrated luminosity of 34.7 fb$ ^{-1} $. [...]
arXiv:2412.02477 ; CMS-SMP-24-005 ; CERN-EP-2024-293 ; CMS-SMP-24-005-003.
- 2024 - 45.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
7.
An implementation of neural simulation-based inference for parameter estimation in ATLAS / ATLAS Collaboration
Neural simulation-based inference is a powerful class of machine-learning-based methods for statistical inference that naturally handles high-dimensional parameter estimation without the need to bin data into low-dimensional summary histograms. [...]
arXiv:2412.01600 ; CERN-EP-2024-305.
- 2024 - 49.
Fulltext - Previous draft version - Fulltext
8.
Measurement of off-shell Higgs boson production in the $H^*\rightarrow ZZ\rightarrow 4\ell$ decay channel using a neural simulation-based inference technique in 13 TeV $pp$ collisions with the ATLAS detector / ATLAS Collaboration
A measurement of off-shell Higgs boson production in the $H^*\to ZZ\to 4\ell$ decay channel is presented. [...]
arXiv:2412.01548 ; CERN-EP-2024-298.
- 2024 - 65.
Fulltext - Previous draft version - Fulltext
9.
Search for heavy neutral Higgs bosons A and H in the $ {\mathrm{t}\overline{\mathrm{t}}} $Z channel in proton-proton collisions at 13 TeV / CMS Collaboration
A direct search for new heavy neutral Higgs bosons A and H in the $ {\mathrm{t}\overline{\mathrm{t}}} \mathrm{Z} $ channel is presented, targeting the process $ \mathrm{p}\mathrm{p}\to\mathrm{A}\to\mathrm{Z}\mathrm{H} $ with $ \mathrm{H}\to{\mathrm{t}\overline{\mathrm{t}}} $. [...]
arXiv:2412.00570 ; CMS-B2G-23-006 ; CERN-EP-2024-301 ; CMS-B2G-23-006-003.
- 2024 - 43.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext
10.
Proton reconstruction with the TOTEM Roman pot detectors for high-$ \beta^* $ LHC data / CMS and TOTEM Collaboration
The TOTEM Roman pot detectors are used to reconstruct the transverse momentum of scattered protons and to estimate the transverse location of the primary interaction. [...]
arXiv:2411.19749 ; CMS-SMP-23-006 ; CERN-EP-2024-273 ; TOTEM-2024-002 ; CMS-SMP-23-006-003.
- 2024 - 58.
Additional information for the analysis - CMS AuthorList - Fulltext - Fulltext

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16 Smith, B A
2 Smith, B B
14 Smith, B C
6 Smith, B D
12 Smith, B E
2 Smith, B G
1 Smith, B G R
29 Smith, B H
45 Smith, B J
1 Smith, B K
2 Smith, B M
3 Smith, B R
1 Smith, B S
7 Smith, B T
64 Smith, B.
19 Smith, B.C.
1 Smith, BC
1 Smith, BT
1 Smith, Barbara Herrnstein
1 Smith, Barbara M
2 Smith, Barry
8 Smith, Ben
235 Smith, Ben Campbell
5 Smith, Benjamin
1 Smith, Benjamin David
1 Smith, Benjamin H
2 Smith, Benjamin P
1 Smith, Bennett
1 Smith, Bennett E
3 Smith, Bernard
15 Smith, Beverly J
1 Smith, Björn
1 Smith, Bob
1 Smith, Bonnie
2 Smith, Brad
5 Smith, Bradford L
1 Smith, Bradley
1 Smith, Bradley D
1 Smith, Brena
1 Smith, Brent
1 Smith, Brent M
1 Smith, Brett
17 Smith, Brian
22 Smith, Brian J
4 Smith, Brian J.
2 Smith, Brian L
1 Smith, Brian R
2 Smith, Brian Robert
4 Smith, Brian T
8 Smith, Britton
25 Smith, Britton D
1 Smith, Bruce
1 Smith, Bruce C
2 Smith, Bryan
1 Smith, Bryan C
1 Smith, Bryan L
2 Smith, Bryan T
4 Smith, Bud
17 Smith, Bud E
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