Search for direct stau production in events with two hadronic tau-leptons in root s=13 TeV pp collisions with the ATLAS detector

Physical Review D American Physical Society 101:3 (2020) 32009

Authors:

G Aad, B Abbott, Dc Abbott, A Abed Abud, K Abeling, Dk Abhayasinghe, Sh Abidi, Os AbouZeid, Nl Abraham, H Abramowicz, H Abreu, Y Abulaiti, Bs Acharya, B Achkar, S Adachi, L Adam, C Adam Bourdarios, L Adamczyk, L Adamek, J Adelman, M Adersberger, A Adiguzel, S Adorni, T Adye, Aa Affolder, Y Afik, C Agapopoulou, Mn Agaras, A Aggarwal, C Agheorghiesei, Ja Aguilar-Saavedra, F Ahmadov, Ws Ahmed, X Ai, G Aielli, S Akatsuka, Tpa Akesson, E Akilli, Av Akimov, K Al Khoury, Gl Alberghi, J Albert, MJ Alconada Verzini, S Alderweireldt, M Aleksa, In Aleksandrov, C Alexa, D Alexandre, T Alexopoulos

Abstract:

A search for the direct production of the supersymmetric partners of τ-leptons (staus) in final states with two hadronically decaying τ-leptons is presented. The analysis uses a dataset of pp collisions corresponding to an integrated luminosity of 139 fb-1, recorded with the ATLAS detector at the Large Hadron Collider at a center-of-mass energy of 13 TeV. No significant deviation from the expected Standard Model background is observed. Limits are derived in scenarios of direct production of stau pairs with each stau decaying into the stable lightest neutralino and one τ-lepton in simplified models where the two stau mass eigenstates are degenerate. Stau masses from 120 GeV to 390 GeV are excluded at 95% confidence level for a massless lightest neutralino.

Measurement of azimuthal anisotropy of muons from charm and bottom hadrons in pp collisions at sqrt[s]=13  TeV with the ATLAS Detector

Physical Review Letters American Physical Society 124:8 (2020) 82301

Authors:

G Aad, B Abbott, Dc Abbott, A Abed Abud, K Abeling, Dk Abhayasinghe, Sh Abidi, Os AbouZeid, Nl Abraham, H Abramowicz, H Abreu, Y Abulaiti, Bs Acharya, B Achkar, S Adachi, L Adam, C Adam Bourdarios, L Adamczyk, L Adamek, J Adelman, M Adersberger, A Adiguzel, S Adorni, T Adye, Aa Affolder, Y Afik, C Agapopoulou, Mn Agaras, A Aggarwal, C Agheorghiesei, Ja Aguilar-Saavedra, F Ahmadov, Ws Ahmed, X Ai, G Aielli, S Akatsuka, Tpa Åkesson, E Akilli, Av Akimov, K Al Khoury, Gl Alberghi, J Albert, Mj Alconada Verzini, S Alderweireldt, M Aleksa, In Aleksandrov, C Alexa, D Alexandre, T Alexopoulos

Abstract:

The elliptic flow of muons from the decay of charm and bottom hadrons is measured in pp collisions at sqrt[s]=13  TeV using a data sample with an integrated luminosity of 150  pb^{-1} recorded by the ATLAS detector at the LHC. The muons from heavy-flavor decay are separated from light-hadron decay muons using momentum imbalance between the tracking and muon spectrometers. The heavy-flavor decay muons are further separated into those from charm decay and those from bottom decay using the distance-of-closest-approach to the collision vertex. The measurement is performed for muons in the transverse momentum range 4-7 GeV and pseudorapidity range |η|<2.4. A significant nonzero elliptic anisotropy coefficient v_{2} is observed for muons from charm decays, while the v_{2} value for muons from bottom decays is consistent with zero within uncertainties.

Measurement of neutron-proton capture in the SNO+ water phase

(2020)

Authors:

The SNO Collaboration, :, MR Anderson, S Andringa, M Askins, DJ Auty, N Barros, F Barão, R Bayes, EW Beier, A Bialek, SD Biller, E Blucher, R Bonventre, M Boulay, E Caden, EJ Callaghan, J Caravaca, D Chauhan, M Chen, O Chkvorets, B Cleveland, MA Cox, MM Depatie, J Dittmer, F Di Lodovico, AD Earle, E Falk, N Fatemighomi, V Fischer, E Fletcher, R Ford, K Frankiewicz, K Gilje, D Gooding, C Grant, J Grove, AL Hallin, D Hallman, S Hans, J Hartnell, P Harvey, WJ Heintzelman, RL Helmer, D Horne, B Hreljac, J Hu, ASM Hussain, AS Inácio, CJ Jillings, T Kaptanoglu, P Khaghani, JR Klein, R Knapik, LL Kormos, B Krar, C Kraus, CB Krauss, T Kroupova, I Lam, BJ Land, A LaTorre, I Lawson, L Lebanowski, EJ Leming, A Li, J Lidgard, B Liggins, YH Lin, Y Liu, V Lozza, M Luo, S Maguire, A Maio, S Manecki, J Maneira, RD Martin, E Marzec, A Mastbaum, N McCauley, AB McDonald, P Mekarski, M Meyer, C Mills, I Morton-Blake, S Nae, M Nirkko, LJ Nolan, HM O'Keeffe, GD Orebi Gann, MJ Parnell, J Paton, SJM Peeters, T Pershing, L Pickard, G Prior, A Reichold, S Riccetto, R Richardson, M Rigan, J Rose, R Rosero, PM Rost, J Rumleskie, I Semenec, F Shaker, MK Sharma, K Singh, P Skensved, M Smiley, MI Stringer, R Svoboda, B Tam, L Tian, J Tseng, E Turner, R Van Berg, JGC Veinot, CJ Virtue, E Vázquez-Jáuregui, SC Walton, J Wang, M Ward, JJ Weigand, JR Wilson, P Woosaree, A Wright, JP Yanez, M Yeh, T Zhang, Y Zhang, K Zuber, A Zummo

Search for electroweak production of charginos and sleptons decaying into final states with two leptons and missing transverse momentum in √s=13 TeV pp collisions using the ATLAS detector

European Physical Journal C Springer Nature 80:2 (2020) 123

Authors:

ATLAS Collaboration, G Aad, B Abbott, Alan Barr

Abstract:

A search for the electroweak production of charginos and sleptons decaying into final states with two electrons or muons is presented. The analysis is based on 139 fb−1 of proton–proton collisions recorded by the ATLAS detector at the Large Hadron Collider at s√=13 TeV. Three R-parity-conserving scenarios where the lightest neutralino is the lightest supersymmetric particle are considered: the production of chargino pairs with decays via either W bosons or sleptons, and the direct production of slepton pairs. The analysis is optimised for the first of these scenarios, but the results are also interpreted in the others. No significant deviations from the Standard Model expectations are observed and limits at 95% confidence level are set on the masses of relevant supersymmetric particles in each of the scenarios. For a massless lightest neutralino, masses up to 420 GeV are excluded for the production of the lightest-chargino pairs assuming W-boson-mediated decays and up to 1 TeV for slepton-mediated decays, whereas for slepton-pair production masses up to 700 GeV are excluded assuming three generations of mass-degenerate sleptons.

Measurement of the azimuthal anisotropy of charged-particle production in Xe plus Xe collisions at root S-NN=5.44 TeV with the ATLAS detector

Physical Review C American Physical Society 101:2 (2020) 24906

Authors:

G Aad, B Abbott, Dc Abbott, A Abed Abud, K Abeling, Dk Abhayasinghe, Sh Abidi, Os AbouZeid, Nl Abraham, H Abramowicz, H Abreu, Y Abulaiti, Bs Acharya, B Achkar, S Adachi, L Adam, C Adam Bourdarios, L Adamczyk, L Adamek, J Adelman, M Adersberger, A Adiguzel, S Adorni, T Adye, Aa Affolder, Y Afik, C Agapopoulou, Mn Agaras, A Aggarwal, C Agheorghiesei, Ja Aguilar-Saavedra, F Ahmadov, Ws Ahmed, X Ai, G Aielli, S Akatsuka, Tpa Akesson, E Akilli, Av Akimov, K Al Khoury, Gl Alberghi, J Albert, MJ Alconada Verzini, S Alderweireldt, M Aleksa, In Aleksandrov, C Alexa, T Alexopoulos, A Alfonsi

Abstract:

This paper describes the measurements of flow harmonics v2-v6 in 3μb-1 of Xe+Xe collisions at sNN=5.44 TeV performed using the ATLAS detector at the Large Hadron Collider (LHC). Measurements of the centrality, multiplicity, and pT dependence of the vn obtained using two-particle correlations and the scalar product technique are presented. The measurements are also performed using a template-fit procedure, which was developed to remove nonflow correlations in small collision systems. This nonflow removal is shown to have a significant influence on the measured vn at high pT, especially in peripheral events. Comparisons of the measured vn with measurements in Pb+Pb collisions and p+Pb collisions at sNN=5.02 TeV are also presented. The vn values in Xe+Xe collisions are observed to be larger than those in Pb+Pb collisions for n=2, 3, and 4 in the most central events. However, with decreasing centrality or increasing harmonic order n, the vn values in Xe+Xe collisions become smaller than those in Pb+Pb collisions. The vn in Xe+Xe and Pb+Pb collisions are also compared as a function of the mean number of participating nucleons, (Npart), and the measured charged-particle multiplicity in the detector. The v3 values in Xe+Xe and Pb+Pb collisions are observed to be similar at the same (Npart) or multiplicity, but the other harmonics are significantly different. The ratios of the measured vn in Xe+Xe and Pb+Pb collisions, as a function of centrality, are also compared to theoretical calculations.