Emulating the impact of additional proton–proton interactions in the ATLAS simulation by presampling sets of inelastic Monte Carlo events

Computing and Software for Big Science Springer Nature 6:1 (2022) 3

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, AC Abusleme Hoffman, BS Acharya, B Achkar, L Adam, C Adam Bourdarios, L Adamczyk, L Adamek, J Adelman, A Adiguzel, S Adorni, T Adye, AA Affolder, Y Afik

Abstract:

The accurate simulation of additional interactions at the ATLAS experiment for the analysis of proton–proton collisions delivered by the Large Hadron Collider presents a significant challenge to the computing resources. During the LHC Run 2 (2015–2018), there were up to 70 inelastic interactions per bunch crossing, which need to be accounted for in Monte Carlo (MC) production. In this document, a new method to account for these additional interactions in the simulation chain is described. Instead of sampling the inelastic interactions and adding their energy deposits to a hard-scatter interaction one-by-one, the inelastic interactions are presampled, independent of the hard scatter, and stored as combined events. Consequently, for each hard-scatter interaction, only one such presampled event needs to be added as part of the simulation chain. For the Run 2 simulation chain, with an average of 35 interactions per bunch crossing, this new method provides a substantial reduction in MC production CPU needs of around 20%, while reproducing the properties of the reconstructed quantities relevant for physics analyses with good accuracy

Model-independent constraints on $\Omega_m$ and $H(z)$ from the link between geometry and growth

(2022)

Authors:

Jaime Ruiz-Zapatero, Carlos García-García, David Alonso, Pedro G Ferreira, Richard DP Grumitt

Quantifying the poor purity and completeness of morphological samples selected by galaxy colour

Monthly Notices of the Royal Astronomical Society Oxford University Press (OUP) 510:3 (2022) 4126-4133

Authors:

Rebecca J Smethurst, Karen L Masters, Brooke D Simmons, Izzy L Garland, Tobias Géron, Boris Häußler, Sandor Kruk, Chris J Lintott, David O’Ryan, Mike Walmsley

Search for exotic decays of the Higgs boson into b$$ \overline{b} $$ and missing transverse momentum in pp collisions at $$ \sqrt{s} $$ = 13 TeV with the ATLAS detector

Journal of High Energy Physics Springer 2022:1 (2022) 63

Authors:

G Aad, B Abbott, DC Abbott, A Abed Abud, K Abeling, DK Abhayasinghe, SH Abidi, H Abramowicz, H Abreu, Y Abulaiti, AC Abusleme Hoffman, BS Acharya, B Achkar, L Adam, C Adam Bourdarios, L Adamczyk, L Adamek, SV Addepalli, J Adelman, A Adiguzel, S Adorni, T Adye, AA Affolder, Y Afik, C Agapopoulou

Abstract:

A summary of results in heavy flavour physics from Run 1 of the LHC is presented. Topics discussed include spectroscopy, mixing, CP violation and rare decays of charmed and beauty hadrons.Comment: 25 pages, 9 figures (total 17 subfigures). Invited review for Comptes Rendus de Physique de l'Academie des Science

Operation and performance of the ATLAS semiconductor tracker in LHC Run 2

Journal of Instrumentation IOP Publishing 17:01 (2022) P01013

Authors:

Georges Aad, Brad Abbott, Dale Charles Abbott, L Ambroz, G Artoni, WK Balunas, AJ Barr, D Bortoletto, F Celli, EI Conroy, Amanda Cooper-Sarkar, JA Frost, MG Foti, GE Gallardo, EJ Gallas, JC Grundy, C Gwenlan, YT Harris, CP Hays, TB Huffman, K Karava, Z Li, C Merlassino, M Mironova, Koichi Nagai, RB Nickerson, AP O’Neill, SR Paredes Saenz, CS Pollard, E Schopf, IPJ Shipsey, Y Wei, HA Smith, M Stankaityte, I Veliscek, GHA Viehhauser, AR Weidberg, PJ Windischhofer, R Wölker, KW Woźniak, S Yan, K Potamianos

Abstract:

The semiconductor tracker (SCT) is one of the tracking systems for charged particles in the ATLAS detector. It consists of 4088 silicon strip sensor modules. During Run 2 (2015–2018) the Large Hadron Collider delivered an integrated luminosity of 156 fb-1 to the ATLAS experiment at a centre-of-mass proton-proton collision energy of 13 TeV. The instantaneous luminosity and pile-up conditions were far in excess of those assumed in the original design of the SCT detector. Due to improvements to the data acquisition system, the SCT operated stably throughout Run 2. It was available for 99.9% of the integrated luminosity and achieved a data-quality efficiency of 99.85%. Detailed studies have been made of the leakage current in SCT modules and the evolution of the full depletion voltage, which are used to study the impact of radiation damage to the modules.