Abstract
The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.
Original language | English |
---|---|
Article number | 179 |
Pages (from-to) | 1-48 |
Number of pages | 49 |
Journal | Journal of High Energy Physics |
Volume | 2020 |
Issue number | 3 |
DOIs | |
Publication status | Published - Mar 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
- Hadron-Hadron scattering (experiments)
- Hard scattering
- Jets
- Photon production
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In: Journal of High Energy Physics, Vol. 2020, No. 3, 179, 03.2020, p. 1-48.
Research output: Contribution to journal › Article › peer-review
TY - JOUR
T1 - Measurement of isolated-photon plus two-jet production in pp collisions at √s = 13 TeV 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 - Adachi, S.
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 - Ahmadov, F.
AU - Ahmed, W. S.
AU - Ai, X.
AU - Aielli, G.
AU - Akatsuka, S.
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 - Alexandre, D.
AU - Alexopoulos, T.
AU - Alfonsi, A.
AU - Alfonsi, F.
AU - Alhroob, M.
AU - Ali, B.
AU - Alimonti, G.
AU - Alison, J.
AU - Alkire, S. P.
AU - Allaire, C.
AU - Allbrooke, B. M.M.
AU - Allen, B. W.
AU - Allport, P. P.
AU - Aloisio, A.
AU - Alonso, A.
AU - Alonso, F.
AU - Alpigiani, C.
AU - Alshehri, A. A.
AU - Alvarez Estevez, M.
AU - Álvarez Piqueras, D.
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, C. F.
AU - Anders, J. K.
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 - Aperio Bella, L.
AU - Arabidze, G.
AU - Araque, J. P.
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 - Artamonov, A.
AU - Artoni, G.
AU - Artz, S.
AU - Asai, S.
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 - Avolio, G.
AU - Avramidou, R.
AU - Ayoub, M. K.
AU - Azoulay, A. M.
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 - Bajic, M.
AU - Bakalis, C.
AU - Baker, O. K.
AU - Bakker, P. J.
AU - Bakshi Gupta, D.
AU - Balaji, S.
AU - Baldin, E. M.
AU - Balek, P.
AU - Balli, F.
AU - Balunas, W. K.
AU - Balz, J.
AU - Banas, E.
AU - Bandyopadhyay, A.
AU - Banerjee, Sw
AU - Bannoura, A. A.E.
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 - Barnes, S. L.
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 - Barsov, S.
AU - Bartoldus, R.
AU - Bartolini, G.
AU - Barton, A. E.
AU - Bartos, P.
AU - Basalaev, 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, K. T.
AU - Bawa, H. S.
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 - Becker, M.
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 - 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 - Bertella, C.
AU - Bertram, I. A.
AU - Bessidskaia Bylund, O.
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 - 2020/3
Y1 - 2020/3
N2 - The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.
AB - The dynamics of isolated-photon plus two-jet production in pp collisions at a centre-of-mass energy of 13 TeV are studied with the ATLAS detector at the LHC using a dataset corresponding to an integrated luminosity of 36.1 fb−1. Cross sections are measured as functions of a variety of observables, including angular correlations and invariant masses of the objects in the final state, γ + jet + jet. Measurements are also performed in phase-space regions enriched in each of the two underlying physical mechanisms, namely direct and fragmentation processes. The measurements cover the range of photon (jet) transverse momenta from 150 GeV (100 GeV) to 2 TeV. The tree-level plus parton-shower predictions from Sherpa and Pythia as well as the next-to-leading-order QCD predictions from Sherpa are compared with the measurements. The next-to-leading-order QCD predictions describe the data adequately in shape and normalisation except for regions of phase space such as those with high values of the invariant mass or rapidity separation of the two jets, where the predictions overestimate the data.
KW - Hadron-Hadron scattering (experiments)
KW - Hard scattering
KW - Jets
KW - Photon production
UR - http://www.scopus.com/inward/record.url?scp=85083096465&partnerID=8YFLogxK
U2 - 10.1007/JHEP03(2020)179
DO - 10.1007/JHEP03(2020)179
M3 - Article
AN - SCOPUS:85083096465
SN - 1029-8479
VL - 2020
SP - 1
EP - 48
JO - Journal of High Energy Physics
JF - Journal of High Energy Physics
IS - 3
M1 - 179
ER -