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A measurement of the Higgs boson mass and width via its decay to two bosons is presented. Proton-proton collision data collected by the CMS experiment, corresponding to an integrated luminosity of at a center-of-mass energy of 13 TeV, is used. The invariant mass distribution of four leptons in the on-shell Higgs boson decay is used to measure its mass and constrain its width. This yields the most precise single measurement of the Higgs boson mass to date, , and an upper limit on the width at 95% confidence level. A combination of the on- and off-shell Higgs boson production decaying to four leptons is used to determine the Higgs boson width, assuming that no new virtual particles affect the production, a premise that is tested by adding new heavy particles in the gluon fusion loop model. This result is combined with a previous CMS analysis of the off-shell Higgs boson production with decay to two leptons and two neutrinos, giving a measured Higgs boson width of , in agreement with the standard model prediction of 4.1 MeV. The strength of the off-shell Higgs boson production is also reported. The scenario of no off-shell Higgs boson production is excluded at a confidence level corresponding to 3.8 standard deviations. © 2025 CERN, for the CMS Collaboration2025CERN
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- Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
Title:
Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production
Abstract Since the discovery of the Higgs boson in 2012, detailed studies of its properties have been ongoing. Besides its mass, its width—related to its lifetime—is an important parameter. One way to determine this quantity is to measure its off-shell production, where the Higgs boson mass is far away from its nominal value, and relating it to its on-shell production, where the mass is close to the nominal value. Here we report evidence for such off-shell contributions to the production cross-section of two Z bosons with data from the CMS experiment at the CERN Large Hadron Collider. We constrain the total rate of the off-shell Higgs boson contribution beyond the Z boson pair production threshold, relative to its standard model expectation, to the interval [0.0061, 2.0] at the 95% confidence level. The scenario with no off-shell contribution is excluded at a p -value of 0.0003 (3.6 standard deviations). We measure the width of the Higgs boson as $${{{\varGamma }}}_{{{{{{\rm{H}}}}}}}={3.2}_{-1.7}^{+2.4}\,{{{{{\rm{MeV}}}}}}$$ Γ H = 3.2 − 1.7 + 2.4 MeV , in agreement with the standard model expectation of 4.1 MeV. In addition, we set constraints on anomalous Higgs boson couplings to W and Z boson pairs.
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- PAR ID:
- 10420362
- Author(s) / Creator(s):
- Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Chatterjee, S.; Damanakis, K.; Dragicevic, M.; Del Valle, A. Escalante; Frühwirth, R.; Jeitler, M.; Krammer, N.; Lechner, L.; Liko, D.; Mikulec, I.; Paulitsch, P.; Pitters, F. M.; Schieck, J.; Schöfbeck, R.; Schwarz, D.; Templ, S.more » ; Waltenberger, W.; Wulz, C.-E.; Chekhovsky, V.; Litomin, A.; Makarenko, V.; Darwish, M. R.; De Wolf, E. A.; Janssen, T.; Kello, T.; Lelek, A.; Sfar, H. Rejeb; Van Mechelen, P.; Van Putte, S.; Van Remortel, N.; Bols, E. S.; D’Hondt, J.; De Moor, A.; Delcourt, M.; El Faham, H.; Lowette, S.; Moortgat, S.; Morton, A.; Müller, D.; Sahasransu, A. R.; Tavernier, S.; Van Doninck, W.; Vannerom, D.; Beghin, D.; Bilin, B.; Clerbaux, B.; De Lentdecker, G.; Favart, L.; Kalsi, A. K.; Lee, K.; Mahdavikhorrami, M.; Makarenko, I.; Paredes, S.; Pétré, L.; Popov, A.; Postiau, N.; Starling, E.; Thomas, L.; Bemden, M. 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C.; Nabili, S.; Palmer, C.; Seidel, M.; Skuja, A.; Wang, L.; Wong, K.; Abercrombie, D.; Andreassi, G.; Bi, R.; Busza, W.; Cali, I. A.; Chen, Y.; D’Alfonso, M.; Eysermans, J.; Freer, C.; Ceballos, G. Gomez; Goncharov, M.; Harris, P.; Hu, M.; Klute, M.; Kovalskyi, D.; Krupa, J.; Lee, Y.-J.; Long, K.; Mironov, C.; Paus, C.; Rankin, D.; Roland, C.; Roland, G.; Shi, Z.; Stephans, G. S.; Wang, J.; Wang, Z.; Wyslouch, B.; Chatterjee, R. M.; Evans, A.; Hiltbrand, J.; Jain, Sh.; Joshi, B. M.; Krohn, M.; Kubota, Y.; Mans, J.; Revering, M.; Rusack, R.; Saradhy, R.; Schroeder, N.; Strobbe, N.; Wadud, M. A.; Bloom, K.; Bryson, M.; Chauhan, S.; Claes, D. R.; Fangmeier, C.; Finco, L.; Golf, F.; Joo, C.; Kravchenko, I.; Reed, I.; Siado, J. E.; Snow, G. R.; Tabb, W.; Wightman, A.; Yan, F.; Zecchinelli, A. G.; Agarwal, G.; Bandyopadhyay, H.; Hay, L.; Iashvili, I.; Kharchilava, A.; McLean, C.; Nguyen, D.; Pekkanen, J.; Rappoccio, S.; Williams, A.; Alverson, G.; Barberis, E.; Haddad, Y.; Han, Y.; Hortiangtham, A.; Krishna, A.; Li, J.; Lidrych, J.; Madigan, G.; Marzocchi, B.; Morse, D. M.; Nguyen, V.; Orimoto, T.; Parker, A.; Skinnari, L.; Tishelman-Charny, A.; Wamorkar, T.; Wang, B.; Wisecarver, A.; Wood, D.; Bhattacharya, S.; Bueghly, J.; Chen, Z.; Gilbert, A.; Gunter, T.; Hahn, K. A.; Liu, Y.; Odell, N.; Schmitt, M. H.; Velasco, M.; Band, R.; Bucci, R.; Cremonesi, M.; Das, A.; Dev, N.; Goldouzian, R.; Hildreth, M.; Anampa, K. Hurtado; Jessop, C.; Lannon, K.; Lawrence, J.; Loukas, N.; Lutton, D.; Mariano, J.; Marinelli, N.; Mcalister, I.; McCauley, T.; Mcgrady, C.; Mohrman, K.; Moore, C.; Musienko, Y.; Ruchti, R.; Townsend, A.; Wayne, M.; Zarucki, M.; Zygala, L.; Bylsma, B.; Durkin, L. S.; Francis, B.; Hill, C.; Ornelas, M. Nunez; Wei, K.; Winer, B. L.; Yates, B. R.; Addesa, F. M.; Bonham, B.; Das, P.; Dezoort, G.; Elmer, P.; Frankenthal, A.; Greenberg, B.; Haubrich, N.; Higginbotham, S.; Kalogeropoulos, A.; Kopp, G.; Kwan, S.; Lange, D.; Marlow, D.; Mei, K.; Ojalvo, I.; Olsen, J.; Stickland, D.; Tully, C.; Malik, S.; Norberg, S.; Bakshi, A. S.; Barnes, V. E.; Chawla, R.; Das, S.; Gutay, L.; Jones, M.; Jung, A. W.; Kondratyev, D.; Koshy, A. M.; Liu, M.; Negro, G.; Neumeister, N.; Paspalaki, G.; Piperov, S.; Purohit, A.; Schulte, J. F.; Stojanovic, M.; Thieman, J.; Wang, F.; Xiao, R.; Xie, W.; Dolen, J.; Parashar, N.; Acosta, D.; Baty, A.; Carnahan, T.; Decaro, M.; Dildick, S.; Ecklund, K. M.; Freed, S.; Gardner, P.; Geurts, F. J.; Kumar, A.; Li, W.; Padley, B. P.; Redjimi, R.; Rotter, J.; Shi, W.; Leiton, A. G.; Yang, S.; Zhang, L.; Zhang, Y.; Bodek, A.; de Barbaro, P.; Demina, R.; Dulemba, J. L.; Fallon, C.; Ferbel, T.; Galanti, M.; Garcia-Bellido, A.; Hindrichs, O.; Khukhunaishvili, A.; Ranken, E.; Taus, R.; Van Onsem, G. P.; Goulianos, K.; Chiarito, B.; Chou, J. P.; Gershtein, Y.; Halkiadakis, E.; Hart, A.; Heindl, M.; Karacheban, O.; Laflotte, I.; Lath, A.; Montalvo, R.; Nash, K.; Osherson, M.; Salur, S.; Schnetzer, S.; Somalwar, S.; Stone, R.; Thayil, S. A.; Thomas, S.; Wang, H.; Acharya, H.; Delannoy, A. G.; Fiorendi, S.; Holmes, T.; Spanier, S.; Bouhali, O.; Dalchenko, M.; Delgado, A.; Eusebi, R.; Gilmore, J.; Huang, T.; Kamon, T.; Kim, H.; Luo, S.; Malhotra, S.; Mueller, R.; Overton, D.; Rathjens, D.; Safonov, A.; Akchurin, N.; Damgov, J.; Hegde, V.; Lamichhane, K.; Lee, S. W.; Mengke, T.; Muthumuni, S.; Peltola, T.; Volobouev, I.; Wang, Z.; Whitbeck, A.; Appelt, E.; Greene, S.; Gurrola, A.; Johns, W.; Melo, A.; Padeken, K.; Romeo, F.; Sheldon, P.; Tuo, S.; Velkovska, J.; Arenton, M. W.; Cardwell, B.; Cox, B.; Cummings, G.; Hakala, J.; Hirosky, R.; Joyce, M.; Ledovskoy, A.; Li, A.; Neu, C.; Lara, C. E.; Tannenwald, B.; White, S.; Poudyal, N.; Banerjee, S.; Black, K.; Bose, T.; Dasu, S.; De Bruyn, I.; Everaerts, P.; Galloni, C.; He, H.; Herndon, M.; Herve, A.; Hussain, U.; Lanaro, A.; Loeliger, A.; Loveless, R.; Sreekala, J. Madhusudanan; Mallampalli, A.; Mohammadi, A.; Pinna, D.; Savin, A.; Shang, V.; Sharma, V.; Smith, W. H.; Teague, D.; Trembath-Reichert, S.; Vetens, W. « less
- Date Published:
- Journal Name:
- Nature Physics
- Volume:
- 18
- Issue:
- 11
- ISSN:
- 1745-2473
- Page Range / eLocation ID:
- 1329 to 1334
- Format(s):
- Medium: X
- Sponsoring Org:
- National Science Foundation
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Bargieła, Piotr; Buccioni, Federico; Caola, Fabrizio; Devoto, Federica; von Manteuffel, Andreas; Tancredi, Lorenzo (, The European Physical Journal C)Abstract In this paper we consider signal-background interference effects in Higgs-mediated diphoton production at the LHC. After reviewing earlier works that show how to use these effects to constrain the Higgs boson total decay width, we provide predictions beyond NLO accuracy for the interference and related observables, and study the impact of QCD radiative corrections on the Higgs width determination. In particular, we use the so-called soft-virtual approximation to estimate interference effects at NNLO in QCD. The inclusion of these effects reduces the NNLO prediction for the total Higgs cross-section in the diphoton channel by about 1.7%. We study in detail the impact of QCD corrections on the Higgs-boson line-shape and its implications for the Higgs boson width extraction. In particular, we find that the shift of the Higgs resonance peak arising from interference effects gets reduced by about 30% with respect to the NLO prediction. Assuming an experimental resolution of about 150 $$\textrm{MeV}$$ on interference-induced modifications of the Higgs-boson line-shape, our NNLO analysis shows that one could constrain the Higgs-boson total width to about 10–20 times its Standard Model value.more » « less
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Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Ambrogi, F.; Bergauer, T.; Dragicevic, M.; Erö, J.; Escalante Del Valle, A.; Frühwirth, R.; Jeitler, M.; et al (, Journal of High Energy Physics)null (Ed.)A bstract A search for standard model Higgs bosons (H) produced with transverse momentum ( p T ) greater than 450 GeV and decaying to bottom quark-antiquark pairs ( $$ \mathrm{b}\overline{\mathrm{b}} $$ b b ¯ ) is performed using proton-proton collision data collected by the CMS experiment at the LHC at $$ \sqrt{s} $$ s = 13 TeV. The data sample corresponds to an integrated luminosity of 137 fb − 1 . The search is inclusive in the Higgs boson production mode. Highly Lorentz-boosted Higgs bosons decaying to $$ \mathrm{b}\overline{\mathrm{b}} $$ b b ¯ are reconstructed as single large-radius jets, and are identified using jet substructure and a dedicated b tagging technique based on a deep neural network. The method is validated with Z → $$ \mathrm{b}\overline{\mathrm{b}} $$ b b ¯ decays. For a Higgs boson mass of 125 GeV, an excess of events above the background assuming no Higgs boson production is observed with a local significance of 2.5 standard deviations ( σ ), while the expectation is 0.7. The corresponding signal strength and local significance with respect to the standard model expectation are μ H = 3 . 7 ± 1 . 2(stat) $$ {}_{-0.7}^{+0.8} $$ − 0.7 + 0.8 (syst) $$ {}_{-0.5}^{+0.8} $$ − 0.5 + 0.8 (theo) and 1 . 9 σ . Additionally, an unfolded differential cross section as a function of Higgs boson p T for the gluon fusion production mode is presented, assuming the other production modes occur at the expected rates.more » « less
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Sirunyan, A. M.; Tumasyan, A.; Adam, W.; Andrejkovic, J. W.; Bergauer, T.; Chatterjee, S.; Dragicevic, M.; Valle, A. Escalante; Frühwirth, R.; Jeitler, M.; et al (, The European Physical Journal C)null (Ed.)Abstract Production cross sections of the Higgs boson are measured in the $${\mathrm{H}} \rightarrow {\mathrm{Z}} {\mathrm{Z}} \rightarrow 4\ell $$ H → Z Z → 4 ℓ ( $$\ell ={\mathrm{e}},{{{\upmu }}_{\mathrm{}}^{\mathrm{}}} $$ ℓ = e , μ ) decay channel. A data sample of proton–proton collisions at a center-of-mass energy of 13 $$\,\text {Te}\text {V}$$ Te , collected by the CMS detector at the LHC and corresponding to an integrated luminosity of 137 $$\,\text {fb}^{-1}$$ fb - 1 is used. The signal strength modifier $$\mu $$ μ , defined as the ratio of the Higgs boson production rate in the $$4\ell $$ 4 ℓ channel to the standard model (SM) expectation, is measured to be $$\mu =0.94 \pm 0.07 \,\text {(stat)} ^{+0.09}_{-0.08} \,\text {(syst)} $$ μ = 0.94 ± 0.07 (stat) - 0.08 + 0.09 (syst) at a fixed value of $$m_{{\mathrm{H}}} = 125.38\,\text {Ge}\text {V} $$ m H = 125.38 Ge . The signal strength modifiers for the individual Higgs boson production modes are also reported. The inclusive fiducial cross section for the $${\mathrm{H}} \rightarrow 4\ell $$ H → 4 ℓ process is measured to be $$2.84^{+0.23}_{-0.22} \,\text {(stat)} ^{+0.26}_{-0.21} \,\text {(syst)} \,\text {fb} $$ 2 . 84 - 0.22 + 0.23 (stat) - 0.21 + 0.26 (syst) fb , which is compatible with the SM prediction of $$2.84 \pm 0.15 \,\text {fb} $$ 2.84 ± 0.15 fb for the same fiducial region. Differential cross sections as a function of the transverse momentum and rapidity of the Higgs boson, the number of associated jets, and the transverse momentum of the leading associated jet are measured. A new set of cross section measurements in mutually exclusive categories targeted to identify production mechanisms and kinematical features of the events is presented. The results are in agreement with the SM predictions.more » « less
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Cite: MLA FormatTumasyan, A., Adam, W., Andrejkovic, J. W., Bergauer, T., Chatterjee, S., Damanakis, K., Dragicevic, M., Del Valle, A. Escalante, Frühwirth, R., Jeitler, M., Krammer, N., Lechner, L., Liko, D., Mikulec, I., Paulitsch, P., Pitters, F. M., Schieck, J., Schöfbeck, R., Schwarz, D., Templ, S., Waltenberger, W., Wulz, C.-E., Chekhovsky, V., Litomin, A., Makarenko, V., Darwish, M. R., De Wolf, E. A., Janssen, T., Kello, T., Lelek, A., Sfar, H. Rejeb, Van Mechelen, P., Van Putte, S., Van Remortel, N., Bols, E. S., D’Hondt, J., De Moor, A., Delcourt, M., El Faham, H., Lowette, S., Moortgat, S., Morton, A., Müller, D., Sahasransu, A. R., Tavernier, S., Van Doninck, W., Vannerom, D., Beghin, D., Bilin, B., Clerbaux, B., De Lentdecker, G., Favart, L., Kalsi, A. K., Lee, K., Mahdavikhorrami, M., Makarenko, I., Paredes, S., Pétré, L., Popov, A., Postiau, N., Starling, E., Thomas, L., Bemden, M. 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Cite: BibTeX Format@article{osti_10420362,
place = {Country unknown/Code not available}, title = {Measurement of the Higgs boson width and evidence of its off-shell contributions to ZZ production}, url = {https://par.nsf.gov/biblio/10420362}, DOI = {10.1038/s41567-022-01682-0}, abstractNote = {Abstract Since the discovery of the Higgs boson in 2012, detailed studies of its properties have been ongoing. Besides its mass, its width—related to its lifetime—is an important parameter. One way to determine this quantity is to measure its off-shell production, where the Higgs boson mass is far away from its nominal value, and relating it to its on-shell production, where the mass is close to the nominal value. Here we report evidence for such off-shell contributions to the production cross-section of two Z bosons with data from the CMS experiment at the CERN Large Hadron Collider. We constrain the total rate of the off-shell Higgs boson contribution beyond the Z boson pair production threshold, relative to its standard model expectation, to the interval [0.0061, 2.0] at the 95% confidence level. The scenario with no off-shell contribution is excluded at a p -value of 0.0003 (3.6 standard deviations). We measure the width of the Higgs boson as $${{{\varGamma }}}_{{{{{{\rm{H}}}}}}}={3.2}_{-1.7}^{+2.4}\,{{{{{\rm{MeV}}}}}}$$ Γ H = 3.2 − 1.7 + 2.4 MeV , in agreement with the standard model expectation of 4.1 MeV. In addition, we set constraints on anomalous Higgs boson couplings to W and Z boson pairs.}, journal = {Nature Physics}, volume = {18}, number = {11}, author = {Tumasyan, A. and Adam, W. and Andrejkovic, J. W. and Bergauer, T. and Chatterjee, S. and Damanakis, K. and Dragicevic, M. and Del Valle, A. Escalante and Frühwirth, R. and Jeitler, M. and Krammer, N. and Lechner, L. and Liko, D. and Mikulec, I. and Paulitsch, P. and Pitters, F. M. and Schieck, J. and Schöfbeck, R. and Schwarz, D. and Templ, S. and Waltenberger, W. and Wulz, C.-E. and Chekhovsky, V. and Litomin, A. and Makarenko, V. and Darwish, M. R. and De Wolf, E. A. and Janssen, T. and Kello, T. and Lelek, A. and Sfar, H. Rejeb and Van Mechelen, P. and Van Putte, S. and Van Remortel, N. and Bols, E. S. and D’Hondt, J. and De Moor, A. and Delcourt, M. and El Faham, H. and Lowette, S. and Moortgat, S. and Morton, A. and Müller, D. and Sahasransu, A. R. and Tavernier, S. and Van Doninck, W. and Vannerom, D. and Beghin, D. and Bilin, B. and Clerbaux, B. and De Lentdecker, G. and Favart, L. and Kalsi, A. K. and Lee, K. and Mahdavikhorrami, M. and Makarenko, I. and Paredes, S. and Pétré, L. and Popov, A. and Postiau, N. and Starling, E. and Thomas, L. and Bemden, M. 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