Measurement of the H → γγ and H → ZZ* → 4l cross-sections in pp collisions at √s = 13.6 TeV with the ATLAS detector
The inclusive Higgs boson production cross-section is measured in the di-photon and the ZZ* → 4l decay channels using 31.4 and 29.0 fb-1 of pp collision data respectively, collected with the ATLAS detector at a centre-of-mass energy of √s = 13.6 TeV. To reduce the model dependence, the measurement i...
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| Main Authors: | , , , , , , , , , , , , , , , , , , , , , , , |
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| Corporate Author: | |
| Format: | Article (Journal) |
| Language: | English |
| Published: |
24 January 2024
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| In: |
The European physical journal. C, Particles and fields
Year: 2024, Volume: 84, Pages: 1-34 |
| ISSN: | 1434-6052 |
| DOI: | 10.1140/epjc/s10052-023-12130-5 |
| Online Access: | Verlag, lizenzpflichtig, Volltext: https://doi.org/10.1140/epjc/s10052-023-12130-5 |
| Author Notes: | ATLAS Collaboration* |
MARC
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| 245 | 1 | 0 | |a Measurement of the H → γγ and H → ZZ* → 4l cross-sections in pp collisions at √s = 13.6 TeV with the ATLAS detector |c ATLAS Collaboration* |
| 246 | 3 | 0 | |a sqrt |
| 246 | 3 | 3 | |a Measurement of the H → gamma gamma and H → ZZ * → 4 l cross-sections in proton-proton collisions at square root s = 13.6 TeV with the ATLAS detector |
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| 500 | |a *ATLAS Collaboration: G. Aad, L.M. Baltes, F. Bartels, M.M. Czurylo, F. Del Rio, S.J. Dittmeier, M. Dunford, S. Franchino, T. Junkermann, M. Klassen, T. Mkrtchyan, P.S. Ott, D.F. Rassloff, S. Rodriguez Bosca, C. Sauer, A. Schoening, H.-C. Schultz-Coulon, V. Sothilingam, R. Stamen, P. Starovoitov, L. Vigani, S.M. Weber, M. Wessels, J. Zinsser [und sehr viele weitere Personen] | ||
| 500 | |a Im Titel steht der Buchstabe s unter dem Wurzelsymbol | ||
| 500 | |a Gesehen am 09.08.2024 | ||
| 520 | |a The inclusive Higgs boson production cross-section is measured in the di-photon and the ZZ* → 4l decay channels using 31.4 and 29.0 fb-1 of pp collision data respectively, collected with the ATLAS detector at a centre-of-mass energy of √s = 13.6 TeV. To reduce the model dependence, the measurement in each channel is restricted to a particle-level phase space that closely matches the channel’s detector-level kinematic selection, and it is corrected for detector effects. These measured fiducial cross-sections are $$\sigma _{\textrm{fid},\gamma \gamma } = $$ $$76^{+14}_{-13}$$ fb, and $$\sigma _{\textrm{fid},4 \ell } =$$ $$2.80\, \pm \, 0.74$$ fb, in agreement with the corresponding Standard Model predictions of $$67.6 \pm 3.7 $$ fb and $$3.67 \pm 0.19 $$ fb. Assuming Standard Model acceptances and branching fractions for the two channels, the fiducial measurements are extrapolated to the full phase space yielding total cross-sections of $$\sigma (pp \rightarrow H) = 67^{+12}_{-11}$$ pb and $$46 \pm 12$$ pb at 13.6 $$\text {TeV}$$from the di-photon and $$ZZ^* \rightarrow 4 \ell $$measurements respectively. The two measurements are combined into a total cross-section measurement of $$\sigma (pp \rightarrow H)= 58.2 \pm 8.7$$ pb, to be compared with the Standard Model prediction of $$\sigma (pp \rightarrow H)_\textrm{SM} = 59.9 \pm 2.6 $$ pb. | ||
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