Abstract
A search for new-physics resonances decaying into a lepton and a jet performed by the ATLAS experiment is presented. Scalar leptoquarks pair-produced in pp collisions at √s = 13 TeV at the Large Hadron Collider are considered using an integrated luminosity of 139 fb−1, corresponding to the full Run 2 dataset. They are searched for in events with two electrons or two muons and two or more jets, including jets identified as arising from the fragmentation of c- or b-quarks. The observed yield in each channel is consistent with the Standard Model background expectation. Leptoquarks with masses below 1.8 TeV and 1.7 TeV are excluded in the electron and muon channels, respectively, assuming a branching ratio into a charged lepton and a quark of 100%, with minimal dependence on the quark flavour. Upper limits on the aforementioned branching ratio are also given as a function of the leptoquark mass.
Original language | English |
---|---|
Article number | 112 |
Pages (from-to) | 1-44 |
Number of pages | 45 |
Journal | Journal of High Energy Physics |
Volume | 2020 |
Issue number | 10 |
DOIs | |
Publication status | Published - Oct 2020 |
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 (experiments)
- Particle and resonance production
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In: Journal of High Energy Physics, Vol. 2020, No. 10, 112, 10.2020, p. 1-44.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Search for pairs of scalar leptoquarks decaying into quarks and electrons or muons in √s = 13 TeV pp collisions with the ATLAS detector
AU - The ATLAS collaboration
AU - Aad, G.
AU - Abbott, B.
AU - Abbott, D. C.
AU - Abed Abud, A.
AU - Abeling, K.
AU - Abhayasinghe, D. K.
AU - Abidi, S. H.
AU - AbouZeid, O. S.
AU - Abraham, N. L.
AU - Abramowicz, H.
AU - Abreu, H.
AU - Abulaiti, Y.
AU - Acharya, B. S.
AU - Achkar, B.
AU - Adam, L.
AU - Adam Bourdarios, C.
AU - Adamczyk, L.
AU - Adamek, L.
AU - Adelman, J.
AU - Adersberger, M.
AU - Adiguzel, A.
AU - Adorni, S.
AU - Adye, T.
AU - Affolder, A. A.
AU - Afik, Y.
AU - Agapopoulou, C.
AU - Agaras, M. N.
AU - Aggarwal, A.
AU - Agheorghiesei, C.
AU - Aguilar-Saavedra, J. A.
AU - Ahmad, A.
AU - Ahmadov, F.
AU - Ahmed, W. S.
AU - Ai, X.
AU - Aielli, G.
AU - Akatsuka, S.
AU - Akbiyik, M.
AU - Åkesson, T. P.A.
AU - Akilli, E.
AU - Akimov, A. V.
AU - Al Khoury, K.
AU - Alberghi, G. L.
AU - Albert, J.
AU - Alconada Verzini, M. J.
AU - Alderweireldt, S.
AU - Aleksa, M.
AU - Aleksandrov, I. N.
AU - Alexa, C.
AU - Alexopoulos, T.
AU - Alfonsi, A.
AU - Alfonsi, F.
AU - Alhroob, M.
AU - Ali, B.
AU - Ali, S.
AU - Aliev, M.
AU - Alimonti, G.
AU - Allaire, C.
AU - Allbrooke, B. M.M.
AU - Allen, B. W.
AU - Allport, P. P.
AU - Aloisio, A.
AU - Alonso, F.
AU - Alpigiani, C.
AU - Alunno Camelia, E.
AU - Alvarez Estevez, M.
AU - Alviggi, M. G.
AU - Amaral Coutinho, Y.
AU - Ambler, A.
AU - Ambroz, L.
AU - Amelung, C.
AU - Amidei, D.
AU - Amor Dos Santos, S. P.
AU - Amoroso, S.
AU - Amrouche, C. S.
AU - An, F.
AU - Anastopoulos, C.
AU - Andari, N.
AU - Andeen, T.
AU - Anders, J. K.
AU - Andrean, S. Y.
AU - Andreazza, A.
AU - Andrei, V.
AU - Anelli, C. R.
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 - Aparisi Pozo, J. A.
AU - Aparo, M. A.
AU - Aperio Bella, L.
AU - Aranzabal Barrio, N.
AU - Araujo Ferraz, V.
AU - Araujo Pereira, R.
AU - Arcangeletti, C.
AU - Arce, A. T.H.
AU - Arduh, F. A.
AU - Arguin, J. F.
AU - Argyropoulos, S.
AU - Arling, J. H.
AU - Armbruster, A. J.
AU - Armstrong, A.
AU - Arnaez, O.
AU - Arnold, H.
AU - Arrubarrena Tame, Z. P.
AU - Artoni, G.
AU - Asada, H.
AU - Asai, K.
AU - Asai, S.
AU - Asawatavonvanich, T.
AU - Asbah, N.
AU - Asimakopoulou, E. M.
AU - Asquith, L.
AU - Assahsah, J.
AU - Assamagan, K.
AU - Astalos, R.
AU - Atkin, R. J.
AU - Atkinson, M.
AU - Atlay, N. B.
AU - Atmani, H.
AU - Augsten, K.
AU - Austrup, V. A.
AU - Avolio, G.
AU - Ayoub, M. K.
AU - Azuelos, G.
AU - Bachacou, H.
AU - Bachas, K.
AU - Backes, M.
AU - Backman, F.
AU - Bagnaia, P.
AU - Bahmani, M.
AU - Bahrasemani, H.
AU - Bailey, A. J.
AU - Bailey, V. R.
AU - Baines, J. T.
AU - Bakalis, C.
AU - Baker, O. K.
AU - Bakker, P. J.
AU - Bakos, E.
AU - Bakshi Gupta, D.
AU - Balaji, S.
AU - Balasubramanian, R.
AU - Baldin, E. M.
AU - Balek, P.
AU - Balli, F.
AU - Balunas, W. K.
AU - Balz, J.
AU - Banas, E.
AU - Bandieramonte, M.
AU - Bandyopadhyay, A.
AU - Banerjee, Sw
AU - Barak, L.
AU - Barbe, W. M.
AU - Barberio, E. L.
AU - Barberis, D.
AU - Barbero, M.
AU - Barbour, G.
AU - Barillari, T.
AU - Barisits, M. S.
AU - Barkeloo, J.
AU - Barklow, T.
AU - Barnea, R.
AU - Barnett, B. M.
AU - Barnett, R. M.
AU - Barnovska-Blenessy, Z.
AU - Baroncelli, A.
AU - Barone, G.
AU - Barr, A. J.
AU - Barranco Navarro, L.
AU - Barreiro, F.
AU - Barreiro Guimarães da Costa, J.
AU - Barron, U.
AU - Barsov, S.
AU - Bartels, F.
AU - Bartoldus, R.
AU - Bartolini, G.
AU - Barton, A. E.
AU - Bartos, P.
AU - Basalaev, A.
AU - Basan, A.
AU - Bassalat, A.
AU - Basso, M. J.
AU - Bates, R. L.
AU - Batlamous, S.
AU - Batley, J. R.
AU - Batool, B.
AU - Battaglia, M.
AU - Bauce, M.
AU - Bauer, F.
AU - Bauer, P.
AU - Bawa, H. S.
AU - Bayirli, A.
AU - Beacham, J. B.
AU - Beau, T.
AU - Beauchemin, P. H.
AU - Becherer, F.
AU - Bechtle, P.
AU - Beck, H. C.
AU - Beck, H. P.
AU - Becker, K.
AU - Becot, C.
AU - Beddall, A. J.
AU - Beddall, A. J.
AU - Bednyakov, V. A.
AU - Bedognetti, M.
AU - Bee, C. P.
AU - Beermann, T. A.
AU - Begalli, M.
AU - Begel, M.
AU - Behera, A.
AU - Behr, J. K.
AU - Beisiegel, F.
AU - Belfkir, M.
AU - Bell, A. S.
AU - Bella, G.
AU - Bellagamba, L.
AU - Bellerive, A.
AU - Bellos, P.
AU - Beloborodov, K.
AU - Belotskiy, K.
AU - Belyaev, N. L.
AU - Benchekroun, D.
AU - Benekos, N.
AU - Benhammou, Y.
AU - Benjamin, D. P.
AU - Benoit, M.
AU - Bensinger, J. R.
AU - Bentvelsen, S.
AU - Beresford, L.
AU - Beretta, M.
AU - Berge, D.
AU - Bergeaas Kuutmann, E.
AU - Berger, N.
AU - Bergmann, B.
AU - Bergsten, L. J.
AU - Beringer, J.
AU - Berlendis, S.
AU - Bernardi, G.
AU - Bernius, C.
AU - Bernlochner, F. U.
AU - Berry, T.
AU - Berta, P.
AU - Berthold, 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 - 2020/10
Y1 - 2020/10
N2 - A search for new-physics resonances decaying into a lepton and a jet performed by the ATLAS experiment is presented. Scalar leptoquarks pair-produced in pp collisions at √s = 13 TeV at the Large Hadron Collider are considered using an integrated luminosity of 139 fb−1, corresponding to the full Run 2 dataset. They are searched for in events with two electrons or two muons and two or more jets, including jets identified as arising from the fragmentation of c- or b-quarks. The observed yield in each channel is consistent with the Standard Model background expectation. Leptoquarks with masses below 1.8 TeV and 1.7 TeV are excluded in the electron and muon channels, respectively, assuming a branching ratio into a charged lepton and a quark of 100%, with minimal dependence on the quark flavour. Upper limits on the aforementioned branching ratio are also given as a function of the leptoquark mass.
AB - A search for new-physics resonances decaying into a lepton and a jet performed by the ATLAS experiment is presented. Scalar leptoquarks pair-produced in pp collisions at √s = 13 TeV at the Large Hadron Collider are considered using an integrated luminosity of 139 fb−1, corresponding to the full Run 2 dataset. They are searched for in events with two electrons or two muons and two or more jets, including jets identified as arising from the fragmentation of c- or b-quarks. The observed yield in each channel is consistent with the Standard Model background expectation. Leptoquarks with masses below 1.8 TeV and 1.7 TeV are excluded in the electron and muon channels, respectively, assuming a branching ratio into a charged lepton and a quark of 100%, with minimal dependence on the quark flavour. Upper limits on the aforementioned branching ratio are also given as a function of the leptoquark mass.
KW - Beyond Standard Model
KW - Exotics
KW - Hadron-Hadron scattering (experiments)
KW - Particle and resonance production
UR - http://www.scopus.com/inward/record.url?scp=85093967333&partnerID=8YFLogxK
U2 - 10.1007/JHEP10(2020)112
DO - 10.1007/JHEP10(2020)112
M3 - Article
AN - SCOPUS:85093967333
SN - 1029-8479
VL - 2020
SP - 1
EP - 44
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 10
M1 - 112
ER -