Abstract
A search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (bb¯) and the other decays to WW*, ZZ*, or τ+τ−, with in each case a final state with ℓ+ℓ−+ neutrinos (ℓ = e, μ). The analysis targets separately the gluon-gluon fusion and vector boson fusion production modes. Data recorded by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 140 fb−1, are used in this analysis. Events are selected to have exactly two b-tagged jets and two leptons with opposite electric charge and missing transverse momentum in the final state. These events are classified using multivariate analysis algorithms to separate the HH events from other Standard Model processes. No evidence of the signal is found. The observed (expected) upper limit on the cross-section for non-resonant Higgs boson pair production is determined to be 9.7 (16.2) times the Standard Model prediction at 95% confidence level. The Higgs boson self-interaction coupling parameter κλ and the quadrilinear coupling parameter κ2V are each separately constrained by this analysis to be within the ranges [−6.2, 13.3] and [−0.17, 2.4], respectively, at 95% confidence level, when all other parameters are fixed.
Original language | English |
---|---|
Article number | 37 |
Pages (from-to) | 1-47 |
Number of pages | 48 |
Journal | Journal of High Energy Physics |
Volume | 2024 |
Issue number | 2 |
DOIs | |
Publication status | Published - Feb 2024 |
Externally published | Yes |
Bibliographical note
Copyright the Author(s). 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.Keywords
- Hadron-Hadron Scattering
- Higgs Physics
- Proton-Proton Scattering
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In: Journal of High Energy Physics, Vol. 2024, No. 2, 37, 02.2024, p. 1-47.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Search for non-resonant Higgs boson pair production in the 2b + 2ℓ + ETmiss final state in pp collisions at √s = 13 TeV with the ATLAS detector
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 - Aktas, S.
AU - Al Khoury, K.
AU - Alberghi, G. L.
AU - Albert, J.
AU - Albicocco, P.
AU - Albouy, G. L.
AU - Alderweireldt, S.
AU - Alegria, Z. L.
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 - Alviggi, M. G.
AU - Aly, M.
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 - 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 - Baer, T. M.
AU - Bagnaia, P.
AU - Bahmani, M.
AU - Bahner, D.
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 - 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 - Shojaii, J.
N1 - Copyright the Author(s). 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 - 2024/2
Y1 - 2024/2
N2 - A search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (bb¯) and the other decays to WW*, ZZ*, or τ+τ−, with in each case a final state with ℓ+ℓ−+ neutrinos (ℓ = e, μ). The analysis targets separately the gluon-gluon fusion and vector boson fusion production modes. Data recorded by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 140 fb−1, are used in this analysis. Events are selected to have exactly two b-tagged jets and two leptons with opposite electric charge and missing transverse momentum in the final state. These events are classified using multivariate analysis algorithms to separate the HH events from other Standard Model processes. No evidence of the signal is found. The observed (expected) upper limit on the cross-section for non-resonant Higgs boson pair production is determined to be 9.7 (16.2) times the Standard Model prediction at 95% confidence level. The Higgs boson self-interaction coupling parameter κλ and the quadrilinear coupling parameter κ2V are each separately constrained by this analysis to be within the ranges [−6.2, 13.3] and [−0.17, 2.4], respectively, at 95% confidence level, when all other parameters are fixed.
AB - A search for non-resonant Higgs boson pair (HH) production is presented, in which one of the Higgs bosons decays to a b-quark pair (bb¯) and the other decays to WW*, ZZ*, or τ+τ−, with in each case a final state with ℓ+ℓ−+ neutrinos (ℓ = e, μ). The analysis targets separately the gluon-gluon fusion and vector boson fusion production modes. Data recorded by the ATLAS detector in proton-proton collisions at a centre-of-mass energy of 13 TeV at the Large Hadron Collider, corresponding to an integrated luminosity of 140 fb−1, are used in this analysis. Events are selected to have exactly two b-tagged jets and two leptons with opposite electric charge and missing transverse momentum in the final state. These events are classified using multivariate analysis algorithms to separate the HH events from other Standard Model processes. No evidence of the signal is found. The observed (expected) upper limit on the cross-section for non-resonant Higgs boson pair production is determined to be 9.7 (16.2) times the Standard Model prediction at 95% confidence level. The Higgs boson self-interaction coupling parameter κλ and the quadrilinear coupling parameter κ2V are each separately constrained by this analysis to be within the ranges [−6.2, 13.3] and [−0.17, 2.4], respectively, at 95% confidence level, when all other parameters are fixed.
KW - Hadron-Hadron Scattering
KW - Higgs Physics
KW - Proton-Proton Scattering
UR - http://www.scopus.com/inward/record.url?scp=85190958560&partnerID=8YFLogxK
U2 - 10.1007/JHEP02(2024)037
DO - 10.1007/JHEP02(2024)037
M3 - Article
AN - SCOPUS:85190958560
SN - 1029-8479
VL - 2024
SP - 1
EP - 47
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 2
M1 - 37
ER -