Abstract
A search is presented for the pair production of higgsinos χ˜ in gauge-mediated supersymmetry models, where the lightest neutralinos χ˜1 0 decay into a light gravitino G˜ in association with either a Higgs h or a Z boson. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb−1 of proton–proton collisions at a centre-of-mass energy of s=13TeV. It targets final states in which a Higgs boson decays into a photon pair, while the other Higgs or Z boson decays into a bb¯ pair, with missing transverse momentum associated with the two gravitinos. Search regions dependent on the amount of missing transverse momentum are defined by the requirements that the diphoton mass should be consistent with the mass of the Higgs boson, and the bb¯ mass with the mass of the Higgs or Z boson. The main backgrounds are estimated with data-driven methods using the sidebands of the diphoton mass distribution. No excesses beyond Standard Model expectations are observed and higgsinos with masses up to 320GeV are excluded, assuming a branching fraction of 100% for χ˜1 0→hG˜. This analysis excludes higgsinos with masses of 130GeV for branching fractions to hG˜ as low as 36%, thus providing complementarity to previous ATLAS searches in final states with multiple leptons or multiple b-jets, targeting different decays of the electroweak bosons.
Original language | English |
---|---|
Article number | 138938 |
Pages (from-to) | 1-24 |
Number of pages | 24 |
Journal | Physics Letters B |
Volume | 856 |
DOIs | |
Publication status | Published - Sept 2024 |
Externally published | Yes |
Bibliographical note
Copyright the Author(s) 2024. 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. 856, 138938, 09.2024, p. 1-24.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Search for pair-produced higgsinos decaying via Higgs or Z bosons to final states containing a pair of photons and a pair of b-jets 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 - Abusleme Hoffman, A. C.
AU - Acharya, B. S.
AU - Adam Bourdarios, C.
AU - Adamczyk, L.
AU - Adamek, 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 - 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, A.
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 - 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 - Antrim, D. J.A.
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 - Arcangeletti, C.
AU - Arce, A. T.H.
AU - Arena, E.
AU - Arguin, J. F.
AU - Argyropoulos, S.
AU - Arling, J. H.
AU - Armbruster, A. J.
AU - Arnaez, O.
AU - Arnold, H.
AU - Arrubarrena Tame, Z. P.
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 - Atlay, N. B.
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 - Bakalis, C.
AU - Baker, O. K.
AU - Bakos, E.
AU - Bakshi Gupta, D.
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 - Barbour, G.
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 - 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 - Belyaev, N. L.
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 - Berry, T.
AU - Berta, P.
AU - Berthold, A.
AU - Bertram, I. A.
AU - Bethke, S.
AU - Shojaii, J.
N1 - Copyright the Author(s) 2024. 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 - 2024/9
Y1 - 2024/9
N2 - A search is presented for the pair production of higgsinos χ˜ in gauge-mediated supersymmetry models, where the lightest neutralinos χ˜1 0 decay into a light gravitino G˜ in association with either a Higgs h or a Z boson. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb−1 of proton–proton collisions at a centre-of-mass energy of s=13TeV. It targets final states in which a Higgs boson decays into a photon pair, while the other Higgs or Z boson decays into a bb¯ pair, with missing transverse momentum associated with the two gravitinos. Search regions dependent on the amount of missing transverse momentum are defined by the requirements that the diphoton mass should be consistent with the mass of the Higgs boson, and the bb¯ mass with the mass of the Higgs or Z boson. The main backgrounds are estimated with data-driven methods using the sidebands of the diphoton mass distribution. No excesses beyond Standard Model expectations are observed and higgsinos with masses up to 320GeV are excluded, assuming a branching fraction of 100% for χ˜1 0→hG˜. This analysis excludes higgsinos with masses of 130GeV for branching fractions to hG˜ as low as 36%, thus providing complementarity to previous ATLAS searches in final states with multiple leptons or multiple b-jets, targeting different decays of the electroweak bosons.
AB - A search is presented for the pair production of higgsinos χ˜ in gauge-mediated supersymmetry models, where the lightest neutralinos χ˜1 0 decay into a light gravitino G˜ in association with either a Higgs h or a Z boson. The search is performed with the ATLAS detector at the Large Hadron Collider using 139 fb−1 of proton–proton collisions at a centre-of-mass energy of s=13TeV. It targets final states in which a Higgs boson decays into a photon pair, while the other Higgs or Z boson decays into a bb¯ pair, with missing transverse momentum associated with the two gravitinos. Search regions dependent on the amount of missing transverse momentum are defined by the requirements that the diphoton mass should be consistent with the mass of the Higgs boson, and the bb¯ mass with the mass of the Higgs or Z boson. The main backgrounds are estimated with data-driven methods using the sidebands of the diphoton mass distribution. No excesses beyond Standard Model expectations are observed and higgsinos with masses up to 320GeV are excluded, assuming a branching fraction of 100% for χ˜1 0→hG˜. This analysis excludes higgsinos with masses of 130GeV for branching fractions to hG˜ as low as 36%, thus providing complementarity to previous ATLAS searches in final states with multiple leptons or multiple b-jets, targeting different decays of the electroweak bosons.
UR - http://www.scopus.com/inward/record.url?scp=85201411999&partnerID=8YFLogxK
U2 - 10.1016/j.physletb.2024.138938
DO - 10.1016/j.physletb.2024.138938
M3 - Article
AN - SCOPUS:85201411999
SN - 0370-2693
VL - 856
SP - 1
EP - 24
JO - Physics Letters B
JF - Physics Letters B
M1 - 138938
ER -