Abstract
A search is performed for localized excesses in the low-mass dijet invariant mass distribution, targeting a hypothetical new particle decaying into two jets and produced in association with either a high transverse momentum photon or a jet. The search uses the full Run 2 data sample from LHC proton-proton collisions collected by the ATLAS experiment at a center-of-mass energy of 13 TeV during 2015-2018. Two variants of the search are presented for each type of initial-state radiation: one that makes no jet flavor requirements and one that requires both of the jets to have been identified as containing Formula Presented-hadrons. No excess is observed relative to the Standard Model prediction, and the data are used to set upper limits on the production cross section for a benchmark Formula Presented model and, separately, for generic, beyond the Standard Model scenarios which might produce a Gaussian-shaped contribution to dijet invariant mass distributions. The results extend the current constraints on dijet resonances to the mass range between 200 and 650 GeV.
Original language | English |
---|---|
Article number | 032002 |
Pages (from-to) | 032002-1-032002-30 |
Number of pages | 30 |
Journal | Physical Review D |
Volume | 110 |
Issue number | 3 |
DOIs | |
Publication status | Published - 1 Aug 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: Physical Review D, Vol. 110, No. 3, 032002, 01.08.2024, p. 032002-1-032002-30.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Search for low-mass resonances decaying into two jets and produced in association with a photon or a jet at √s =13 TeV with the ATLAS detector
AU - ATLAS Collaboration
AU - Filmer, E. K.
AU - Grant, C. M.
AU - Jackson, P.
AU - Kong, A. X.Y.
AU - Pandya, H. D.
AU - Potti, H.
AU - Ruggeri, T. A.
AU - Saha, S.
AU - Ting, E. X.L.
AU - White, M. J.
AU - Gingrich, D. M.
AU - Lindon, J. H.
AU - Nishu, N.
AU - Pinfold, J. L.
AU - Cakir, O.
AU - Canbay, A. C.
AU - Yildiz, H. Duran
AU - Kuday, S.
AU - Turk Cakir, I.
AU - Sultansoy, S.
AU - Adam Bourdarios, C.
AU - Arnaez, O.
AU - Berger, N.
AU - Brahimi, N.
AU - Castillo, F. L.
AU - Cavaliere, T.
AU - Costanza, F.
AU - Delmastro, M.
AU - Di Ciaccio, L.
AU - Hryn’ova, T.
AU - Koletsou, I.
AU - Levêque, J.
AU - Lewis, D. J.
AU - Little, J. D.
AU - Lorenzo Martinez, N.
AU - Sauvan, E.
AU - Wu, Z.
AU - Bernardi, G.
AU - Bomben, M.
AU - Li, A.
AU - Li, T.
AU - Marchiori, G.
AU - Nakkalil, K.
AU - Shen, Q.
AU - Zhang, Y.
AU - Chekanov, S.
AU - Hopkins, W. H.
AU - Hoya, J.
AU - Luongo, N. A.
AU - Metcalfe, J.
AU - Mete, A. S.
AU - Paramonov, A.
AU - Proudfoot, J.
AU - Van Gemmeren, P.
AU - Wamorkar, T.
AU - Wang, R.
AU - Zhang, J.
AU - Cheu, E.
AU - Cui, Z.
AU - Ghosh, A.
AU - Johns, K. A.
AU - Lampl, W.
AU - Lindley, R. E.
AU - Loch, P.
AU - Rutherfoord, J. P.
AU - Sardain, J.
AU - Varnes, E. W.
AU - Zhou, H.
AU - Zhou, Y.
AU - Bakshi Gupta, D.
AU - Burghgrave, B.
AU - Cardenas, J. C.J.
AU - De, K.
AU - Farbin, A.
AU - Hadavand, H. K.
AU - Myers, A. J.
AU - Ozturk, N.
AU - Usai, G.
AU - White, A.
AU - Angelidakis, S.
AU - Fassouliotis, D.
AU - Fountas, L.
AU - Gkialas, I.
AU - Kourkoumelis, C.
AU - Alexopoulos, T.
AU - Drivas-Koulouris, I.
AU - Gazis, E. N.
AU - Kitsaki, C.
AU - Maltezos, S.
AU - Perganti, M.
AU - Andeen, T.
AU - Burton, C. D.
AU - Choi, K.
AU - Onyisi, P. U.E.
AU - Panchal, D. K.
AU - Tost, M.
AU - Wang, C.
AU - Huseynov, N.
AU - Agaras, M. N.
AU - Berrocal Guardia, A.
AU - Bosman, M.
AU - Carlotto, J. I.
AU - Casado, M. P.
AU - Castillo Garcia, L.
AU - Epari, S.
AU - Fernandez Martinez, P.
AU - Gautam, V.
AU - Grinstein, S.
AU - Harrison, J.
AU - Jimenez Pena, J.
AU - Juste Rozas, A.
AU - Korolkov, I.
AU - Mamuzic, J.
AU - Martinez, M.
AU - Martinez Suarez, P.
AU - Mir, L. M.
AU - Montejo Berlingen, J.
AU - Oliveira Correa, G.
AU - Orlando, N.
AU - Pacheco Pages, A.
AU - Padilla Aranda, C.
AU - Qin, Y.
AU - Riu, I.
AU - Sonay, A.
AU - Terzo, S.
AU - Barreiro Guimarães da Costa, J.
AU - Cai, Y.
AU - Chu, X.
AU - Cui, H.
AU - Fan, Y.
AU - Fang, Y.
AU - Guo, F.
AU - He, M.
AU - Huang, X.
AU - Huang, Y.
AU - Jia, X.
AU - Li, M.
AU - Li, S.
AU - Li, Z.
AU - Liang, S.
AU - Liang, Z.
AU - Liu, B.
AU - Liu, P.
AU - Lou, X.
AU - Lu, G.
AU - Mohammed, A. F.
AU - Sha, Q.
AU - Shan, L. Y.
AU - Shi, X.
AU - Tariq, K.
AU - Wang, S.
AU - Wang, W.
AU - Xin, S.
AU - Xu, D.
AU - Yang, X.
AU - Ye, J.
AU - Yu, C.
AU - Zeng, H.
AU - Zhai, M.
AU - Zhang, K.
AU - Zhang, P.
AU - Zhuang, X.
AU - Chen, X.
AU - Feng, M.
AU - Li, H.
AU - Pang, H.
AU - Xia, M.
AU - Xu, Y.
AU - Che, Y.
AU - Chen, H.
AU - Chen, S. J.
AU - De Maria, A.
AU - Han, L.
AU - Jia, Z.
AU - Jin, S.
AU - Lucio Alves, F. L.
AU - Min, T.
AU - Wang, X.
AU - Wang, Y.
AU - Xia, L.
AU - Xu, Z.
AU - Ye, H.
AU - Zhang, L.
AU - Zheng, J.
AU - Liu, Y.
AU - Wu, M.
AU - Ran, K.
AU - Bakos, E.
AU - Beemster, L. J.
AU - Jovicevic, J.
AU - Maksimovic, V.
AU - Sijacki, Dj
AU - Vranjes, N.
AU - Vranjes Milosavljevic, M.
AU - Živković, L.
AU - Aakvaag, E.
AU - Buanes, T.
AU - Eigen, G.
AU - Fomin, N.
AU - Hassan, S.
AU - Hellesund, S.
AU - Huiberts, S. K.
AU - Lipniacka, A.
AU - Martin dit Latour, B.
AU - Stugu, B.
AU - Traeet, A.
AU - Beringer, J.
AU - Calafiura, P.
AU - Cerutti, F.
AU - Chan, J.
AU - Ciocio, A.
AU - Dyckes, G. I.
AU - Einsweiler, K.
AU - Ene, I.
AU - Fortman, A. W.
AU - Foti, M. G.
AU - Gagnon, L. G.
AU - Garcia-Sciveres, M.
AU - Gonzalez Renteria, C.
AU - Gray, H. M.
AU - Haber, C.
AU - Han, S.
AU - Heim, T.
AU - Hu, M.
AU - Ju, X.
AU - Le Pottier, L. T.
AU - Leggett, C.
AU - Marshall, Z.
AU - Mironova, M.
AU - Nachman, B. P.
AU - Ottino, G. J.
AU - Pagan Griso, S.
AU - Pettee, M.
AU - Pianori, E.
AU - Rastogi, A.
AU - Reynolds, E.
AU - Roberts, B. R.
AU - Shapiro, M.
AU - Stanislaus, B.
AU - Thompson, E. A.
AU - Tsulaia, V.
AU - Wagner, J. M.
AU - Wang, H.
AU - Xiong, J.
AU - Yamazaki, T.
AU - Yao, W. M.
AU - Zhang, Z.
AU - Varni, C.
AU - Yeo, B. K.
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 - 2024/8/1
Y1 - 2024/8/1
N2 - A search is performed for localized excesses in the low-mass dijet invariant mass distribution, targeting a hypothetical new particle decaying into two jets and produced in association with either a high transverse momentum photon or a jet. The search uses the full Run 2 data sample from LHC proton-proton collisions collected by the ATLAS experiment at a center-of-mass energy of 13 TeV during 2015-2018. Two variants of the search are presented for each type of initial-state radiation: one that makes no jet flavor requirements and one that requires both of the jets to have been identified as containing Formula Presented-hadrons. No excess is observed relative to the Standard Model prediction, and the data are used to set upper limits on the production cross section for a benchmark Formula Presented model and, separately, for generic, beyond the Standard Model scenarios which might produce a Gaussian-shaped contribution to dijet invariant mass distributions. The results extend the current constraints on dijet resonances to the mass range between 200 and 650 GeV.
AB - A search is performed for localized excesses in the low-mass dijet invariant mass distribution, targeting a hypothetical new particle decaying into two jets and produced in association with either a high transverse momentum photon or a jet. The search uses the full Run 2 data sample from LHC proton-proton collisions collected by the ATLAS experiment at a center-of-mass energy of 13 TeV during 2015-2018. Two variants of the search are presented for each type of initial-state radiation: one that makes no jet flavor requirements and one that requires both of the jets to have been identified as containing Formula Presented-hadrons. No excess is observed relative to the Standard Model prediction, and the data are used to set upper limits on the production cross section for a benchmark Formula Presented model and, separately, for generic, beyond the Standard Model scenarios which might produce a Gaussian-shaped contribution to dijet invariant mass distributions. The results extend the current constraints on dijet resonances to the mass range between 200 and 650 GeV.
UR - http://www.scopus.com/inward/record.url?scp=85201290432&partnerID=8YFLogxK
U2 - 10.1103/PhysRevD.110.032002
DO - 10.1103/PhysRevD.110.032002
M3 - Article
AN - SCOPUS:85201290432
SN - 2470-0029
VL - 110
SP - 032002-1-032002-30
JO - Physical Review D
JF - Physical Review D
IS - 3
M1 - 032002
ER -