Abstract
Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bb¯bb¯, bb¯τ+τ− and bb¯γγ decay channels with single-Higgs boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ− and bb¯ decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton–proton collisions at √s = 13 TeV and correspond to an integrated luminosity of 126–139 fb−1. The combination of the double-Higgs analyses sets an upper limit of μHH<2.4 at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling (λHHH), values outside the interval −0.4<κλ=(λHHH/λHHH SM)<6.3 are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles. In this relaxed scenario, the constraint becomes −1.4<κλ<6.1 at 95% CL.
Original language | English |
---|---|
Article number | 137745 |
Pages (from-to) | 1-20 |
Number of pages | 20 |
Journal | Physics Letters B |
Volume | 843 |
DOIs | |
Publication status | Published - 10 Aug 2023 |
Externally published | Yes |
Bibliographical note
Copyright the Author(s) 2023. Version archived for private and non-commercial use with the permission of the author/s and according to publisher conditions. For further rights please contact the publisher.Cite this
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In: Physics Letters B, Vol. 843, 137745, 10.08.2023, p. 1-20.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Constraints on the Higgs boson self-coupling from single- and double-Higgs production with the ATLAS detector using pp collisions at √s = 13 TeV
AU - The ATLAS Collaboration
AU - Aad, G.
AU - Abbott, B.
AU - Abeling, K.
AU - Abicht, N. J.
AU - Abidi, S. H.
AU - Aboulhorma, A.
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B. S.
AU - Adam Bourdarios, C.
AU - Adamczyk, L.
AU - Addepalli, S. V.
AU - Addison, M. J.
AU - Adelman, J.
AU - Adiguzel, A.
AU - Adye, T.
AU - Affolder, A. A.
AU - Afik, Y.
AU - Agaras, M. N.
AU - Agarwala, J.
AU - Aggarwal, A.
AU - Agheorghiesei, C.
AU - Ahmad, A.
AU - Ahmadov, F.
AU - Ahmed, W. S.
AU - Ahuja, S.
AU - Ai, X.
AU - Aielli, G.
AU - Aikot, A.
AU - Ait Tamlihat, M.
AU - Aitbenchikh, B.
AU - Aizenberg, I.
AU - Akbiyik, M.
AU - Åkesson, T. P.A.
AU - Akimov, A. V.
AU - Akiyama, D.
AU - Akolkar, N. N.
AU - Al Khoury, K.
AU - Alberghi, G. L.
AU - Albert, J.
AU - Albicocco, P.
AU - Albouy, G. L.
AU - Alderweireldt, S.
AU - Aleksa, M.
AU - Aleksandrov, I. N.
AU - Alexa, C.
AU - Alexopoulos, T.
AU - Alfonsi, F.
AU - Algren, M.
AU - Alhroob, M.
AU - Ali, B.
AU - Ali, H. M.J.
AU - Ali, S.
AU - Alibocus, S. W.
AU - Aliev, M.
AU - Alimonti, G.
AU - Alkakhi, W.
AU - Allaire, C.
AU - Allbrooke, B. M.M.
AU - Allen, J. F.
AU - Allendes Flores, C. A.
AU - Allport, P. P.
AU - Aloisio, A.
AU - Alonso, F.
AU - Alpigiani, C.
AU - Alvarez Estevez, M.
AU - Alvarez Fernandez, A.
AU - Alves Cardoso, M.
AU - Aly, M.
AU - Alviggi, M. G.
AU - Amaral Coutinho, Y.
AU - Ambler, A.
AU - Amelung, C.
AU - Amerl, M.
AU - Ames, C. G.
AU - Amidei, D.
AU - Amor Dos Santos, S. P.
AU - Amos, K. R.
AU - Ananiev, V.
AU - Anastopoulos, C.
AU - Andeen, T.
AU - Anders, J. K.
AU - Andrean, S. Y.
AU - Andreazza, A.
AU - Angelidakis, S.
AU - Angerami, A.
AU - Anisenkov, A. V.
AU - Annovi, A.
AU - Antel, C.
AU - Anthony, M. T.
AU - Antipov, E.
AU - Antonelli, M.
AU - Anulli, F.
AU - Aoki, M.
AU - Aoki, T.
AU - Aparisi Pozo, J. A.
AU - Aparo, M. A.
AU - Aperio Bella, L.
AU - Appelt, C.
AU - Apyan, A.
AU - Aranzabal, N.
AU - Arbiol Val, S. J.
AU - Arcangeletti, C.
AU - Arce, A. T.H.
AU - Arena, E.
AU - Arguin, J. F.
AU - Argyropoulos, S.
AU - Arling, J. H.
AU - Arnaez, O.
AU - Arnold, H.
AU - Artoni, G.
AU - Asada, H.
AU - Asai, K.
AU - Asai, S.
AU - Asbah, N. A.
AU - Assahsah, J.
AU - Assamagan, K.
AU - Astalos, R.
AU - Atashi, S.
AU - Atkin, R. J.
AU - Atkinson, M.
AU - Atmani, H.
AU - Atmasiddha, P. A.
AU - Augsten, K.
AU - Auricchio, S.
AU - Auriol, A. D.
AU - Austrup, V. A.
AU - Avolio, G.
AU - Axiotis, K.
AU - Azuelos, G.
AU - Babal, D.
AU - Bachacou, H.
AU - Bachas, K.
AU - Bachiu, A.
AU - Backman, F.
AU - Badea, A.
AU - Bagnaia, P.
AU - Bahmani, M.
AU - Bailey, A. J.
AU - Bailey, V. R.
AU - Baines, J. T.
AU - Baines, L.
AU - Baker, O. K.
AU - Bakos, E.
AU - Bakshi Gupta, D.
AU - Balakrishnan, V.
AU - Balasubramanian, R.
AU - Baldin, E. M.
AU - Balek, P.
AU - Ballabene, E.
AU - Balli, F.
AU - Baltes, L. M.
AU - Balunas, W. K.
AU - Balz, J.
AU - Banas, E.
AU - Bandieramonte, M.
AU - Bandyopadhyay, A.
AU - Bansal, S.
AU - Barak, L.
AU - Barakat, M.
AU - Barberio, E. L.
AU - Barberis, D.
AU - Barbero, M.
AU - Barel, M. Z.
AU - Barends, K. N.
AU - Barillari, T.
AU - Barisits, M. S.
AU - Barklow, T.
AU - Baron, P.
AU - Baron Moreno, D. A.
AU - Baroncelli, A.
AU - Barone, G.
AU - Barr, A. J.
AU - Barr, J. D.
AU - Barranco Navarro, L.
AU - Barreiro, F.
AU - Barreiro Guimarães da Costa, J.
AU - Barron, U.
AU - Barros Teixeira, M. G.
AU - Barsov, S.
AU - Bartels, F.
AU - Bartoldus, R.
AU - Barton, A. E.
AU - Bartos, P.
AU - Basan, A.
AU - Baselga, M.
AU - Bassalat, A.
AU - Basso, M. J.
AU - Basson, C. R.
AU - Bates, R. L.
AU - Batlamous, S.
AU - Batley, J. R.
AU - Batool, B.
AU - Battaglia, M.
AU - Battulga, D.
AU - Bauce, M.
AU - Bauer, M.
AU - Bauer, P.
AU - Bazzano Hurrell, L. T.
AU - Beacham, J. B.
AU - Beau, T.
AU - Beaucamp, J. Y.
AU - Beauchemin, P. H.
AU - Becherer, F.
AU - Bechtle, P.
AU - Beck, H. P.
AU - Becker, K.
AU - Beddall, A. J.
AU - Bednyakov, V. A.
AU - Bee, C. P.
AU - Beemster, L. J.
AU - Beermann, T. A.
AU - Begalli, M.
AU - Begel, M.
AU - Behera, A.
AU - Behr, J. K.
AU - Beirer, J. F.
AU - Beisiegel, F.
AU - Belfkir, M.
AU - Bella, G.
AU - Bellagamba, L.
AU - Bellerive, A.
AU - Bellos, P.
AU - Beloborodov, K.
AU - Benchekroun, D.
AU - Bendebba, F.
AU - Benhammou, Y.
AU - Benoit, M.
AU - Bensinger, J. R.
AU - Bentvelsen, S.
AU - Beresford, L.
AU - Beretta, M.
AU - Bergeaas Kuutmann, E.
AU - Berger, N.
AU - Bergmann, B.
AU - Beringer, J.
AU - Bernardi, G.
AU - Bernius, C.
AU - Bernlochner, F. U.
AU - Bernon, F.
AU - Berrocal Guardia, A.
AU - Berry, T.
AU - Berta, P.
AU - Berthold, A.
AU - Bertram, I. A.
AU - Bethke, S.
AU - Betti, A.
AU - Bevan, A. J.
AU - Shojaii, J.
N1 - Copyright the Author(s) 2023. Version archived for private and non-commercial use with the permission of the author/s and according to publisher conditions. For further rights please contact the publisher.
PY - 2023/8/10
Y1 - 2023/8/10
N2 - Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bb¯bb¯, bb¯τ+τ− and bb¯γγ decay channels with single-Higgs boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ− and bb¯ decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton–proton collisions at √s = 13 TeV and correspond to an integrated luminosity of 126–139 fb−1. The combination of the double-Higgs analyses sets an upper limit of μHH<2.4 at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling (λHHH), values outside the interval −0.4<κλ=(λHHH/λHHH SM)<6.3 are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles. In this relaxed scenario, the constraint becomes −1.4<κλ<6.1 at 95% CL.
AB - Constraints on the Higgs boson self-coupling are set by combining double-Higgs boson analyses in the bb¯bb¯, bb¯τ+τ− and bb¯γγ decay channels with single-Higgs boson analyses targeting the γγ, ZZ⁎, WW⁎, τ+τ− and bb¯ decay channels. The data used in these analyses were recorded by the ATLAS detector at the LHC in proton–proton collisions at √s = 13 TeV and correspond to an integrated luminosity of 126–139 fb−1. The combination of the double-Higgs analyses sets an upper limit of μHH<2.4 at 95% confidence level on the double-Higgs production cross-section normalised to its Standard Model prediction. Combining the single-Higgs and double-Higgs analyses, with the assumption that new physics affects only the Higgs boson self-coupling (λHHH), values outside the interval −0.4<κλ=(λHHH/λHHH SM)<6.3 are excluded at 95% confidence level. The combined single-Higgs and double-Higgs analyses provide results with fewer assumptions, by adding in the fit more coupling modifiers introduced to account for the Higgs boson interactions with the other Standard Model particles. In this relaxed scenario, the constraint becomes −1.4<κλ<6.1 at 95% CL.
UR - http://www.scopus.com/inward/record.url?scp=85164519627&partnerID=8YFLogxK
U2 - 10.1016/j.physletb.2023.137745
DO - 10.1016/j.physletb.2023.137745
M3 - Article
AN - SCOPUS:85164519627
SN - 0370-2693
VL - 843
SP - 1
EP - 20
JO - Physics Letters B
JF - Physics Letters B
M1 - 137745
ER -