Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector
A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded b...
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| Vydáno v: | European Physical Journal C Ročník 82; číslo 8 |
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| Hlavní autoři: | , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , , |
| Médium: | Journal Article |
| Jazyk: | angličtina |
| Vydáno: |
Berlin/Heidelberg
Springer Berlin Heidelberg
2022
Springer Springer Nature B.V Springer Nature |
| Témata: | |
| ISSN: | 1434-6044, 1434-6052, 1431-5858, 1434-6052 |
| On-line přístup: | Získat plný text |
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| Abstract | A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying
W
or
Z
boson. The dataset delivered by the LHC at a centre-of-mass energy of
and recorded by the ATLAS detector corresponds to an integrated luminosity of 139
fb
-
1
. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of
WW
,
WZ
and
ZZ
production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the
(
W
/
Z
)
Z
(
→
c
c
¯
)
process and 3.8 (4.6) standard deviations for the
(
W
/
Z
)
W
(
→
c
q
)
process. The
(
W
/
Z
)
H
(
→
c
c
¯
)
search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of
, corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier
|
κ
c
|
<
8.5
(
12.4
)
, at the 95% confidence level. A combination with the ATLAS
(
W
/
Z
)
H
,
H
→
b
b
¯
analysis is performed, allowing the ratio
κ
c
/
κ
b
to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. |
|---|---|
| AbstractList | A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of √ s = 13 TeV and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb −1 . Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW , WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the ( W / Z ) Z (→ cc ¯) process and 3.8 (4.6) standard deviations for the ( W / Z ) W (→ cq ) process. The ( W / Z ) H (→ cc ¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of 125 GeV, corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κ c | <8.5 (12.4), at the 95% confidence level. A combination with the ATLAS ( W / Z ) H , H → bb ¯ a analysis is performed, allowing the ratio κ c / κ b to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton- proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of root s = 13 TeV and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb(-1). Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(-> c (c) over bar) process and 3.8 (4.6) standard deviations for the (W/Z)W(-> cq) process. The (WIZ)H(-> c (c) over bar) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model crosssection times branching fraction for a Higgs boson with a mass of 125 GeV, corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier vertical bar k(c)vertical bar < 8.5 (12.4), at the 95% confidence level. A combination with the ATLAS (W/Z)H, H -> b<(b)over bar> analysis is performed, allowing the ratio k(c)/k(b) to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb-1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(→cc¯) process and 3.8 (4.6) standard deviations for the (W/Z)W(→cq) process. The (W/Z)H(→cc¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of , corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc|<8.5(12.4), at the 95% confidence level. A combination with the ATLAS (W/Z)H,H→bb¯ analysis is performed, allowing the ratio κc/κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of [InlineEquation not available: see fulltext.] and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb-1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/ Z) Z(→ cc¯) process and 3.8 (4.6) standard deviations for the (W/ Z) W(→ cq) process. The (W/ Z) H(→ cc¯) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of [InlineEquation not available: see fulltext.], corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |κc|<8.5(12.4), at the 95% confidence level. A combination with the ATLAS (W/ Z) H, H→ bb¯ analysis is performed, allowing the ratio κc/ κb to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. © 2022, The Author(s). A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton- proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of root s = 13 TeV and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb(-1). Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the (W/Z)Z(-> c A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton-proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of [Formula omitted] and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 [Formula omitted]. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the [Formula omitted] process and 3.8 (4.6) standard deviations for the [Formula omitted] process. The [Formula omitted] search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of [Formula omitted], corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier [Formula omitted], at the 95% confidence level. A combination with the ATLAS [Formula omitted] analysis is performed, allowing the ratio [Formula omitted] to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of $\sqrt{s}$ = 13 TeV and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb-1. Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW, WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the $(W/Z)Z( → c\bar{c})$ process and 3.8 (4.6) standard deviations for the $(W/Z)W(→cq)$ process. The $(W/Z)Z( → c\bar{c})$ search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of 125 GeV, corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier |$k_c$| < 8.5 (12.4), at the 95% confidence level. A combination with the ATLAS $(W/Z)H,H → b\bar{b}$ analysis is performed, allowing the ratio $k_c/k_b$ to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. A search for the Higgs boson decaying into a pair of charm quarks is presented. The analysis uses proton–proton collisions to target the production of a Higgs boson in association with a leptonically decaying W or Z boson. The dataset delivered by the LHC at a centre-of-mass energy of and recorded by the ATLAS detector corresponds to an integrated luminosity of 139 fb - 1 . Flavour-tagging algorithms are used to identify jets originating from the hadronisation of charm quarks. The analysis method is validated with the simultaneous measurement of WW , WZ and ZZ production, with observed (expected) significances of 2.6 (2.2) standard deviations above the background-only prediction for the ( W / Z ) Z ( → c c ¯ ) process and 3.8 (4.6) standard deviations for the ( W / Z ) W ( → c q ) process. The ( W / Z ) H ( → c c ¯ ) search yields an observed (expected) upper limit of 26 (31) times the predicted Standard Model cross-section times branching fraction for a Higgs boson with a mass of , corresponding to an observed (expected) constraint on the charm Yukawa coupling modifier | κ c | < 8.5 ( 12.4 ) , at the 95% confidence level. A combination with the ATLAS ( W / Z ) H , H → b b ¯ analysis is performed, allowing the ratio κ c / κ b to be constrained to less than 4.5 at the 95% confidence level, smaller than the ratio of the b- and c-quark masses, and therefore determines the Higgs-charm coupling to be weaker than the Higgs-bottom coupling at the 95% confidence level. |
| Audience | Academic |
| Author | Walkowiak, W. Raine, J. A. Lucotte, A. Rendel, M. B. Madriz, R. G. Oreamuno Introzzi, G. Zanzi, D. Pan, J. Gao, Y. Codina, E. Perez Strom, D. M. Li, C.-Q. Yang, Z. Ezhilov, A. Fabbri, L. Falke, P. J. Emerman, A. Aguilar-Saavedra, J. A. Carminati, L. Cantero, J. Hsu, S.-C. Pedro, R. Agullo, P. Martinez Meyer, C. Luise, I. Navarro, J. E. García Diaz, M. A. Dudarev, A. Booth, C. D. Atmani, H. Borissov, G. Kajomovitz, E. Brüers, B. Yang, Y. Lyons, H. Catmore, J. R. Asimakopoulou, E. M. Calafiura, P. Garg, R. B. Gonzalez-Sevilla, S. Korn, A. Shaheen, R. Gama, R. Goncalves Pogrebnyak, I. Sauerburger, F. Bhopatkar, V. S. Simpson, E. L. Hessey, N. P. Schaefer, D. Tnourji, A. Trofymov, A. Zhang, S. Zhukov, K. Golubkov, D. Kang, N. J. Krüger, H. Kupfer, T. Heidorn, W. D. Hamdaoui, H. Gazis, E. N. Batley, J. R. Vokac, P. Hawkings, R. J. Busch, E. L. Melo, A. H. Yang, X. Kim, Y. K. Levin, D. Ronzani, M. Tu, Y. Schwarz, T. A. Ward, R. J. Lehmann, K. Calace, N. Zoccoli, A. Raskina, V. Jia, J. Viehhauser, G. H. A. Pettee, M. Cameron, D. Tariq, K. Ambroz, L. Veloso, F. Zhang, R. Fisc |
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S. orcidid: 0000-0003-3024-587X surname: Bhopatkar fullname: Bhopatkar, V. S. organization: High Energy Physics Division, Argonne National Laboratory – sequence: 256 givenname: R. surname: Bi fullname: Bi, R. organization: Department of Physics and Astronomy, University of Pittsburgh – sequence: 260 givenname: R. orcidid: 0000-0002-2079-5344 surname: Bielski fullname: Bielski, R. organization: Institute for Fundamental Science, University of Oregon – sequence: 307 givenname: R. orcidid: 0000-0001-9683-7101 surname: Bouquet fullname: Bouquet, R. organization: Université de Paris, CNRS/IN2P3, AstroParticule et Cosmologie – sequence: 313 givenname: N. orcidid: 0000-0003-0992-3509 surname: Brahimi fullname: Brahimi, N. organization: School of Physics and Astronomy, Shanghai Jiao Tong University, Key Laboratory for Particle Astrophysics and Cosmology (MOE), SKLPPC, Tsung-Dao Lee Institute – sequence: 343 givenname: A. G. orcidid: 0000-0001-8355-9237 surname: Buckley fullname: Buckley, A. G. organization: SUPA-School of Physics and Astronomy, University of Glasgow – sequence: 363 givenname: A. R. orcidid: 0000-0002-5458-5564 surname: Buzykaev fullname: Buzykaev, A. R. organization: Budker Institute of Nuclear Physics and NSU, SB RAS, Novosibirsk State University – sequence: 399 givenname: J. C. J. orcidid: 0000-0002-6511-7096 surname: Cardenas fullname: Cardenas, J. C. J. organization: Department of Physics, University of Texas at Arlington – sequence: 420 givenname: V. Castillo orcidid: 0000-0002-8245-1790 surname: Gimenez fullname: Gimenez, V. Castillo organization: Instituto de Física Corpuscular (IFIC), Centro Mixto Universidad de Valencia-CSIC – sequence: 449 givenname: S. V. orcidid: 0000-0002-4034-2326 surname: Chekulaev fullname: Chekulaev, S. V. organization: TRIUMF – sequence: 467 givenname: E. orcidid: 0000-0002-8772-0961 surname: Cheremushkina fullname: Cheremushkina, E. organization: Deutsches Elektronen-Synchrotron DESY – sequence: 485 givenname: L. 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A. organization: Department of Physics, University of Michigan – sequence: 2262 givenname: S. orcidid: 0000-0002-0190-7558 surname: Sharma fullname: Sharma, S. organization: Deutsches Elektronen-Synchrotron DESY – sequence: 2303 givenname: S. orcidid: 0000-0002-2438-3785 surname: Sinha fullname: Sinha, S. organization: School of Physics, University of the Witwatersrand – sequence: 2328 givenname: R. orcidid: 0000-0001-7430-7599 surname: Sobie fullname: Sobie, R. organization: Department of Physics and Astronomy, University of Victoria, Institute of Particle Physics (IPP) – sequence: 2348 givenname: R. orcidid: 0000-0003-0124-3410 surname: Soualah fullname: Soualah, R. organization: University of Sharjah – sequence: 2349 givenname: A. M. orcidid: 0000-0002-2210-0913 surname: Soukharev fullname: Soukharev, A. M. organization: Budker Institute of Nuclear Physics and NSU, SB RAS, Novosibirsk State University – sequence: 2394 givenname: S. orcidid: 0000-0001-7582-6227 surname: Stonjek fullname: Stonjek, S. organization: Max-Planck-Institut für Physik (Werner-Heisenberg-Institut) – sequence: 2419 givenname: S. orcidid: 0000-0003-2340-748X surname: Sultansoy fullname: Sultansoy, S. organization: Division of Physics, TOBB University of Economics and Technology – sequence: 2420 givenname: T. orcidid: 0000-0002-2685-6187 surname: Sumida fullname: Sumida, T. organization: Faculty of Science, Kyoto University – sequence: 2449 givenname: S. Tapia orcidid: 0000-0002-3659-7270 surname: Araya fullname: Araya, S. Tapia organization: Department of Physics and Astronomy, Iowa State University – sequence: 2461 givenname: G. N. orcidid: 0000-0002-1831-4871 surname: Taylor fullname: Taylor, G. N. organization: School of Physics, University of Melbourne – sequence: 2467 givenname: J. 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| OpenAccessLink | https://www.proquest.com/docview/2703667125?pq-origsite=%requestingapplication% |
| PQID | 2703667125 |
| PQPubID | 2034659 |
| ParticipantIDs | swepub_primary_oai_portal_research_lu_se_publications_b1dd928f_1037_46a6_a268_25778df67c54 swepub_primary_oai_DiVA_org_uu_483888 swepub_primary_oai_DiVA_org_su_209259 swepub_primary_oai_DiVA_org_kth_317031 osti_scitechconnect_1886924 proquest_journals_2703667125 gale_infotracacademiconefile_A716934422 gale_incontextgauss_ISR_A716934422 springer_journals_10_1140_epjc_s10052_022_10588_3 |
| PublicationCentury | 2000 |
| PublicationDate | 2022 |
| PublicationDateYYYYMMDD | 2022-01-01 |
| PublicationDate_xml | – year: 2022 text: 2022 |
| PublicationDecade | 2020 |
| PublicationPlace | Berlin/Heidelberg |
| PublicationPlace_xml | – name: Berlin/Heidelberg – name: Heidelberg – name: United States |
| PublicationSubtitle | Particles and Fields |
| PublicationTitle | European Physical Journal C |
| PublicationTitleAbbrev | Eur. Phys. J. C |
| PublicationYear | 2022 |
| Publisher | Springer Berlin Heidelberg Springer Springer Nature B.V Springer Nature |
| Publisher_xml | – name: Springer Berlin Heidelberg – name: Springer – name: Springer Nature B.V – name: Springer Nature |
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| Title | Direct constraint on the Higgs–charm coupling from a search for Higgs boson decays into charm quarks with the ATLAS detector |
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