Abstract
A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at √s = 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb, tt¯, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion.
Original language | English |
---|---|
Article number | 118 |
Pages (from-to) | 1-46 |
Number of pages | 47 |
Journal | Journal of High Energy Physics |
Volume | 2024 |
Issue number | 4 |
DOIs | |
Publication status | Published - Apr 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
- Beyond Standard Model
- Exotics
- Hadron-Hadron Scattering
- Particle and Resonance Production
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In: Journal of High Energy Physics, Vol. 2024, No. 4, 118, 04.2024, p. 1-46.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Combination of searches for heavy spin-1 resonances using 139 fb−1 of proton-proton collision data at √s = 13 TeV with the ATLAS detector
AU - The ATLAS collaboration
AU - Aad, G.
AU - Aakvaag, E.
AU - Abbott, B.
AU - Abeling, K.
AU - Abicht, N. J.
AU - Abidi, S. H.
AU - Aboelela, M.
AU - Aboulhorma, A.
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B. S.
AU - Ackermann, A.
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 - Amirie, K. J.
AU - Amor Dos Santos, S. P.
AU - Amos, K. R.
AU - An, S.
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 - 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 - Astrand, K. S.V.
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 - Bai, K.
AU - Bailey, A. J.
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 - 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 - Bates, R. L.
AU - Batlamous, S.
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 - Benkendorfer, K. C.
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 - Bethke, S.
AU - Betti, A.
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 - 2024/4
Y1 - 2024/4
N2 - A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at √s = 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb, tt¯, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion.
AB - A combination of searches for new heavy spin-1 resonances decaying into different pairings of W, Z, or Higgs bosons, as well as directly into leptons or quarks, is presented. The data sample used corresponds to 139 fb−1 of proton-proton collisions at √s = 13 TeV collected during 2015–2018 with the ATLAS detector at the CERN Large Hadron Collider. Analyses selecting quark pairs (qq, bb, tt¯, and tb) or third-generation leptons (τν and ττ) are included in this kind of combination for the first time. A simplified model predicting a spin-1 heavy vector-boson triplet is used. Cross-section limits are set at the 95% confidence level and are compared with predictions for the benchmark model. These limits are also expressed in terms of constraints on couplings of the heavy vector-boson triplet to quarks, leptons, and the Higgs boson. The complementarity of the various analyses increases the sensitivity to new physics, and the resulting constraints are stronger than those from any individual analysis considered. The data exclude a heavy vector-boson triplet with mass below 5.8 TeV in a weakly coupled scenario, below 4.4 TeV in a strongly coupled scenario, and up to 1.5 TeV in the case of production via vector-boson fusion.
KW - Beyond Standard Model
KW - Exotics
KW - Hadron-Hadron Scattering
KW - Particle and Resonance Production
UR - http://www.scopus.com/inward/record.url?scp=85200616166&partnerID=8YFLogxK
U2 - 10.1007/JHEP04(2024)118
DO - 10.1007/JHEP04(2024)118
M3 - Article
AN - SCOPUS:85200616166
SN - 1029-8479
VL - 2024
SP - 1
EP - 46
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 4
M1 - 118
ER -