Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te

Abstract Two related searches for phenomena beyond the standard model (BSM) are performed using events with hadronic jets and significant transverse momentum imbalance. The results are based on a sample of proton–proton collisions at a center-of-mass energy of $$13\,\text {Te}\text {V...

Full description

Bibliographic Details
Main Authors: Sirunyan, A. M, Tumasyan, A., Adam, W., Ambrogi, F., Bergauer, T., Brandstetter, J., Dragicevic, M., Erö, J., Del Valle, A. E, Flechl, M., Frühwirth, R., Jeitler, M., Krammer, N., Krätschmer, I., Liko, D., Madlener, T., Mikulec, I., Rad, N., Schieck, J., Schöfbeck, R.
Other Authors: Massachusetts Institute of Technology. Department of Physics
Format: Article
Language:English
Published: Springer Berlin Heidelberg 2021
Online Access:https://hdl.handle.net/1721.1/131635
_version_ 1811095207850016768
author Sirunyan, A. M
Tumasyan, A.
Adam, W.
Ambrogi, F.
Bergauer, T.
Brandstetter, J.
Dragicevic, M.
Erö, J.
Del Valle, A. E
Flechl, M.
Frühwirth, R.
Jeitler, M.
Krammer, N.
Krätschmer, I.
Liko, D.
Madlener, T.
Mikulec, I.
Rad, N.
Schieck, J.
Schöfbeck, R.
author2 Massachusetts Institute of Technology. Department of Physics
author_facet Massachusetts Institute of Technology. Department of Physics
Sirunyan, A. M
Tumasyan, A.
Adam, W.
Ambrogi, F.
Bergauer, T.
Brandstetter, J.
Dragicevic, M.
Erö, J.
Del Valle, A. E
Flechl, M.
Frühwirth, R.
Jeitler, M.
Krammer, N.
Krätschmer, I.
Liko, D.
Madlener, T.
Mikulec, I.
Rad, N.
Schieck, J.
Schöfbeck, R.
author_sort Sirunyan, A. M
collection MIT
description Abstract Two related searches for phenomena beyond the standard model (BSM) are performed using events with hadronic jets and significant transverse momentum imbalance. The results are based on a sample of proton–proton collisions at a center-of-mass energy of $$13\,\text {Te}\text {V} $$13Te, collected by the CMS experiment at the LHC in 2016–2018 and corresponding to an integrated luminosity of 137$$\,\text {fb}^{-1}$$fb-1. The first search is inclusive, based on signal regions defined by the hadronic energy in the event, the jet multiplicity, the number of jets identified as originating from bottom quarks, and the value of the kinematic variable $$M_{\mathrm {T2}}$$MT2 for events with at least two jets. For events with exactly one jet, the transverse momentum of the jet is used instead. The second search looks in addition for disappearing tracks produced by BSM long-lived charged particles that decay within the volume of the tracking detector. No excess event yield is observed above the predicted standard model background. This is used to constrain a range of BSM models that predict the following: the pair production of gluinos and squarks in the context of supersymmetry models conserving R-parity, with or without intermediate long-lived charginos produced in the decay chain; the resonant production of a colored scalar state decaying to a massive Dirac fermion and a quark; or the pair production of scalar and vector leptoquarks each decaying to a neutrino and a top, bottom, or light-flavor quark. In most of the cases, the results obtained are the most stringent constraints to date.
first_indexed 2024-09-23T16:12:33Z
format Article
id mit-1721.1/131635
institution Massachusetts Institute of Technology
language English
last_indexed 2024-09-23T16:12:33Z
publishDate 2021
publisher Springer Berlin Heidelberg
record_format dspace
spelling mit-1721.1/1316352024-01-03T18:19:57Z Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te Sirunyan, A. M Tumasyan, A. Adam, W. Ambrogi, F. Bergauer, T. Brandstetter, J. Dragicevic, M. Erö, J. Del Valle, A. E Flechl, M. Frühwirth, R. Jeitler, M. Krammer, N. Krätschmer, I. Liko, D. Madlener, T. Mikulec, I. Rad, N. Schieck, J. Schöfbeck, R. Massachusetts Institute of Technology. Department of Physics Abstract Two related searches for phenomena beyond the standard model (BSM) are performed using events with hadronic jets and significant transverse momentum imbalance. The results are based on a sample of proton–proton collisions at a center-of-mass energy of $$13\,\text {Te}\text {V} $$13Te, collected by the CMS experiment at the LHC in 2016–2018 and corresponding to an integrated luminosity of 137$$\,\text {fb}^{-1}$$fb-1. The first search is inclusive, based on signal regions defined by the hadronic energy in the event, the jet multiplicity, the number of jets identified as originating from bottom quarks, and the value of the kinematic variable $$M_{\mathrm {T2}}$$MT2 for events with at least two jets. For events with exactly one jet, the transverse momentum of the jet is used instead. The second search looks in addition for disappearing tracks produced by BSM long-lived charged particles that decay within the volume of the tracking detector. No excess event yield is observed above the predicted standard model background. This is used to constrain a range of BSM models that predict the following: the pair production of gluinos and squarks in the context of supersymmetry models conserving R-parity, with or without intermediate long-lived charginos produced in the decay chain; the resonant production of a colored scalar state decaying to a massive Dirac fermion and a quark; or the pair production of scalar and vector leptoquarks each decaying to a neutrino and a top, bottom, or light-flavor quark. In most of the cases, the results obtained are the most stringent constraints to date. 2021-09-20T17:29:12Z 2021-09-20T17:29:12Z 2020-01-03 2020-06-26T12:46:55Z Article http://purl.org/eprint/type/JournalArticle https://hdl.handle.net/1721.1/131635 The European Physical Journal C. 2020 Jan 03;80(1):3 PUBLISHER_CC en https://doi.org/10.1140/epjc/s10052-019-7493-x Creative Commons Attribution https://creativecommons.org/licenses/by/4.0/ CERN for the benefit of the CMS collaboration application/pdf Springer Berlin Heidelberg Springer Berlin Heidelberg
spellingShingle Sirunyan, A. M
Tumasyan, A.
Adam, W.
Ambrogi, F.
Bergauer, T.
Brandstetter, J.
Dragicevic, M.
Erö, J.
Del Valle, A. E
Flechl, M.
Frühwirth, R.
Jeitler, M.
Krammer, N.
Krätschmer, I.
Liko, D.
Madlener, T.
Mikulec, I.
Rad, N.
Schieck, J.
Schöfbeck, R.
Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title_full Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title_fullStr Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title_full_unstemmed Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title_short Searches for physics beyond the standard model with the $$M_{\mathrm {T2}}$$MT2 variable in hadronic final states with and without disappearing tracks in proton–proton collisions at $$\sqrt{s}=13\,\text {Te}\text {V} $$s=13Te
title_sort searches for physics beyond the standard model with the m mathrm t2 mt2 variable in hadronic final states with and without disappearing tracks in proton proton collisions at sqrt s 13 text te text v s 13te
url https://hdl.handle.net/1721.1/131635
work_keys_str_mv AT sirunyanam searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT tumasyana searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT adamw searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT ambrogif searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT bergauert searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT brandstetterj searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT dragicevicm searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT eroj searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT delvalleae searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT flechlm searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT fruhwirthr searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT jeitlerm searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT krammern searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT kratschmeri searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT likod searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT madlenert searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT mikuleci searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT radn searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT schieckj searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te
AT schofbeckr searchesforphysicsbeyondthestandardmodelwiththemmathrmt2mt2variableinhadronicfinalstateswithandwithoutdisappearingtracksinprotonprotoncollisionsatsqrts13texttetextvs13te