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Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV
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 TeV, collected by the CMS experiment at the LHC in 2016--2018 and corresponding to an integrated luminosity of 137 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 $M_\mathrm{T2}$ 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.
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Definitions of super signal regions, along with predictions, observed data, and the observed 95% CL upper limits on the number...
Figure 11 (T1qqqq)
Figure 11 (upper)
10.17182/hepdata.90834.v1/t2
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks ($\tilde{g}\to q\bar{q}\tilde{\chi}_1^0$). Signal...
Figure 11 (T5qqqqVV)
Figure 11 (lower left)
10.17182/hepdata.90834.v1/t3
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either a...
Figure 11 (T5qqqqWW)
Figure 11 (lower right)
10.17182/hepdata.90834.v1/t4
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and a $\tilde{\chi}_1^\pm$...
Figure 12 (T1bbbb)
Figure 12 (left)
10.17182/hepdata.90834.v1/t5
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to bottom quarks ($\tilde{g}\to b\bar{b}\tilde{\chi}_1^0$). Signal...
Figure 12 (T1tttt)
Figure 12 (right)
10.17182/hepdata.90834.v1/t6
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to top quarks ($\tilde{g}\to t\bar{t}\tilde{\chi}_1^0$). Signal...
Figure 13 (T2qq)
Figure 13 (upper left)
10.17182/hepdata.90834.v1/t7
Exclusion limits at 95% CL for light-flavor squark pair production, where the squarks decay to $q\tilde{\chi}_1^0$. Signal cross sections are...
Figure 13 (T2bb)
Figure 13 (upper right)
10.17182/hepdata.90834.v1/t8
Exclusion limits at 95% CL for bottom squark pair production, where the squarks decay to $b\tilde{\chi}_1^0$. Signal cross sections are...
Figure 13 (T2tt)
Figure 13 (lower)
10.17182/hepdata.90834.v1/t9
Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $t\tilde{\chi}_1^0$. Signal cross sections are...
Figure 14 (T2bW)
Figure 14 (upper left)
10.17182/hepdata.90834.v1/t10
Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $b\tilde{\chi}_1^\pm$ and the $\tilde{\chi}_1^0$ decay...
Figure 14 (T2bt)
Figure 14 (upper right)
10.17182/hepdata.90834.v1/t11
Exclusion limits at 95% CL for top squark pair production, where the squarks decay either to $b\tilde{\chi}_1^\pm\to bW^\pm\tilde{\chi}_1^0$ or to...
Figure 14 (T2cc)
Figure 14 (lower)
10.17182/hepdata.90834.v1/t12
Exclusion limits at 95% CL for top squark pair production, where the squarks decay to $c\tilde{\chi}_1^0$. Signal cross sections are...
Figure 15 (mono-$\phi$)
Figure 15
10.17182/hepdata.90834.v1/t13
Exclusion limits at 95% CL for the mono-$\phi$ model, in which a resonantly-produced colored scalar decays to a massive Dirac...
Figure 16 ($\mathrm{LQ}\to\mathrm{q}\nu$)
Figure 16 (upper left)
10.17182/hepdata.90834.v1/t14
Cross section limits for $\mathrm{LQ}\to\mathrm{q}\nu$, where $q=u,\,d,\,s,\,\mathrm{or}\,c$. Limits are at the 95% confidence level. Theory cross sections are LO for...
Figure 16 ($\mathrm{LQ}\to\mathrm{b}\nu$)
Figure 16 (upper right)
10.17182/hepdata.90834.v1/t15
Cross section limits for $\mathrm{LQ}\to\mathrm{b}\nu$. Limits are at the 95% confidence level. Theory cross sections are LO for vector LQ,...
Figure 16 ($\mathrm{LQ}\to\mathrm{t}\nu$)
Figure 16 (lower)
10.17182/hepdata.90834.v1/t16
Cross section limits for $\mathrm{LQ}\to\mathrm{t}\nu$. Limits are at the 95% confidence level. Theory cross sections are LO for vector LQ,...
Table 12
Table 12 in Appendix B.1, or Figure 5 (upper, left side)
10.17182/hepdata.90834.v1/t17
Predictions and observations for monojet signal regions
Table 13
Table 13 in Appendix B.1, or Figure 23 (upper)
10.17182/hepdata.90834.v1/t18
Predictions and observations for signal regions with $250 \leq H_\mathrm{T} < 450$ GeV
Table 14
Table 14 in Appendix B.1, or Figure 23 (lower)
10.17182/hepdata.90834.v1/t19
Predictions and observations for signal regions with $450 \leq H_\mathrm{T} < 575$ GeV and $N_\mathrm{j}<7$
Table 15
Table 15 in Appendix B.1, or Figure 23 (lower)
10.17182/hepdata.90834.v1/t20
Predictions and observations for signal regions with $450 \leq H_\mathrm{T} < 575$ GeV and $N_\mathrm{j}\geq7$
Table 16
Table 16 in Appendix B.1, or Figure 5 (lower)
10.17182/hepdata.90834.v1/t21
Predictions and observations for signal regions with $575 \leq H_\mathrm{T} < 1200$ GeV and $N_\mathrm{j}^\mathrm{hi}<4$
Table 17
Table 17 in Appendix B.1, or Figure 5 (lower)
10.17182/hepdata.90834.v1/t22
Predictions and observations for signal regions with $575 \leq H_\mathrm{T} < 1200$ GeV and $4\leq N_\mathrm{j}^\mathrm{hi}<7$
Table 18
Table 18 in Appendix B.1, or Figure 5 (lower)
10.17182/hepdata.90834.v1/t23
Predictions and observations for signal regions with $575 \leq H_\mathrm{T} < 1200$ GeV and $N_\mathrm{j}\geq7$
Table 19
Table 19 in Appendix B.1, or Figure 24 (upper) in Appendix C.1
10.17182/hepdata.90834.v1/t24
Predictions and observations for signal regions with $1200 \leq H_\mathrm{T} < 1500$ GeV and $N_\mathrm{j}^\mathrm{hi}<4$
Table 20
Table 20 in Appendix B.1, or Figure 24 (upper) in Appendix C.1
10.17182/hepdata.90834.v1/t25
Predictions and observations for signal regions with $1200 \leq H_\mathrm{T} < 1500$ GeV and $4\leq N_\mathrm{j}^\mathrm{hi}<7$
Table 21
Table 21 in Appendix B.1, or Figure 24 (upper) in Appendix C.1
10.17182/hepdata.90834.v1/t26
Predictions and observations for signal regions with $1200 \leq H_\mathrm{T} < 1500$ GeV and $N_\mathrm{j}\geq7$
Table 22
Table 22 in Appendix B.1, or Figure 24 (lower) in Appendix C.1
10.17182/hepdata.90834.v1/t27
Predictions and observations for signal regions with $H_\mathrm{T} \geq 1500$ GeV and $N_\mathrm{j}<7$
Table 23
Table 23 in Appendix B.1, or Figure 24 (lower) in Appendix C.1
10.17182/hepdata.90834.v1/t28
Predictions and observations for signal regions with $H_\mathrm{T} \geq 1500$ GeV and $N_\mathrm{j}\geq7$
$M_\mathrm{T2}$ covariance matrix
Additional Figure 2
10.17182/hepdata.90834.v1/t29
Covariance matrix for the 282 signal regions of the inclusive $M_\mathrm{T2}$ search
$M_\mathrm{T2}$ correlation matrix
Additional Figure 1
10.17182/hepdata.90834.v1/t30
Correlation matrix for the 282 signal regions of the inclusive $M_\mathrm{T2}$ search
$M_\mathrm{T2}$ covariance matrix bin mappings
Bin definitions for Additional Figures 1 and 2
10.17182/hepdata.90834.v1/t31
Bin number definitions for the $M_\mathrm{T2}$ covariance and correlation matrices
Figure 17 (T1qqqq 10 cm)
Figure 17 (upper left)
10.17182/hepdata.90834.v1/t32
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either the...
Figure 17 (T1qqqq 50 cm)
Figure 17 (upper right)
10.17182/hepdata.90834.v1/t33
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either the...
Figure 17 (T1qqqq 200 cm)
Figure 17 (lower)
10.17182/hepdata.90834.v1/t34
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either the...
Figure 18 (T2qq 10 cm)
Figure 18 (upper left)
10.17182/hepdata.90834.v1/t35
Exclusion limits at 95% CL for direct light squark pair production, where the squarks decay to light-flavor quarks and either...
Figure 18 (T2qq 50 cm)
Figure 18 (upper right)
10.17182/hepdata.90834.v1/t36
Exclusion limits at 95% CL for direct light squark pair production, where the squarks decay to light-flavor quarks and either...
Figure 18 (T2qq 200 cm)
Figure 18 (lower)
10.17182/hepdata.90834.v1/t37
Exclusion limits at 95% CL for direct light squark pair production, where the squarks decay to light-flavor quarks and either...
Figure 19 (T2bt 10 cm)
Figure 19 (upper left)
10.17182/hepdata.90834.v1/t38
Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...
Figure 19 (T2bt 50 cm)
Figure 19 (upper right)
10.17182/hepdata.90834.v1/t39
Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...
Figure 19 (T2bt 200 cm)
Figure 19 (lower)
10.17182/hepdata.90834.v1/t40
Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...
Figure 20 (T1qqqq Max Chargino Exclusion)
Figure 20 (upper left)
10.17182/hepdata.90834.v1/t41
The maximum chargino mass excluded at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks...
Figure 20 (T2qq, one light squark, Max Chargino Exclusion)
Figure 20 (lower left)
10.17182/hepdata.90834.v1/t42
The maximum chargino mass excluded at 95% CL for direct squark pair production, where the squarks decay to light-flavor quarks...
Figure 20 (T2qq Max Chargino Exclusion)
Figure 20 (lower right)
10.17182/hepdata.90834.v1/t43
The maximum chargino mass excluded at 95% CL for direct squark pair production, where the squarks decay to light-flavor quarks...
Figure 21 (T2bt Max Chargino Exclusion)
Figure 21
10.17182/hepdata.90834.v1/t44
Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...
Figure 22 (T1qqqq Fixed Masses)
Figure 22 (upper)
10.17182/hepdata.90834.v1/t45
Exclusion limits at 95% CL for direct gluino pair production, where the gluinos decay to light-flavor quarks and either the...
Figure 22 (T2qq Fixed Masses)
Figure 22 (lower left)
10.17182/hepdata.90834.v1/t46
Exclusion limits at 95% CL for direct squark pair production, where the squarks decay to light-flavor quarks and either the...
Figure 22 (T2bt Fixed Masses)
Figure 22 (lower right)
10.17182/hepdata.90834.v1/t47
Exclusion limits at 95% CL for direct stop pair production, where the stops decay to either a top and the...
Table 24
Table 24 in Appendix B.2
10.17182/hepdata.90834.v1/t48
Predictions and observations for 2016 disappearing track signal regions
Table 25
Table 25 in Appendix B.2
10.17182/hepdata.90834.v1/t49
Predictions and observations for 2017-2018 pixel track signal regions
Table 26
Table 26 in Appendix B.2
10.17182/hepdata.90834.v1/t50
Predictions and observations for 2017-2018 medium (M) and long (L) length track signal regions
When using this data, please cite the original publication:
CMS
Collaboration
(2020).
Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV. Eur.Phys.J.C 80 (2020) 3.
Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV. HEPData (collection).
https://doi.org/10.17182/hepdata.90834
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CMS
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Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV (Version 1). HEPData (collection).
https://doi.org/10.17182/hepdata.90834.v1
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“Table 6 (SSRs)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t1
CMS
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(2023).
“Figure 11 (T1qqqq)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t2
CMS
Collaboration
(2023).
“Figure 11 (T5qqqqVV)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t3
CMS
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(2023).
“Figure 11 (T5qqqqWW)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t4
CMS
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(2023).
“Figure 12 (T1bbbb)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t5
CMS
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(2023).
“Figure 12 (T1tttt)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t6
CMS
Collaboration
(2023).
“Figure 13 (T2qq)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t7
CMS
Collaboration
(2023).
“Figure 13 (T2bb)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t8
CMS
Collaboration
(2023).
“Figure 13 (T2tt)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t9
CMS
Collaboration
(2023).
“Figure 14 (T2bW)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t10
CMS
Collaboration
(2023).
“Figure 14 (T2bt)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t11
CMS
Collaboration
(2023).
“Figure 14 (T2cc)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t12
CMS
Collaboration
(2023).
“Figure 15 (mono-$\phi$)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t13
CMS
Collaboration
(2023).
“Figure 16 ($\mathrm{LQ}\to\mathrm{q}\nu$)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t14
CMS
Collaboration
(2023).
“Figure 16 ($\mathrm{LQ}\to\mathrm{b}\nu$)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t15
CMS
Collaboration
(2023).
“Figure 16 ($\mathrm{LQ}\to\mathrm{t}\nu$)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t16
CMS
Collaboration
(2023).
“Table 12” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t17
CMS
Collaboration
(2023).
“Table 13” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t18
CMS
Collaboration
(2023).
“Table 14” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t19
CMS
Collaboration
(2023).
“Table 15” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t20
CMS
Collaboration
(2023).
“Table 16” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t21
CMS
Collaboration
(2023).
“Table 17” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t22
CMS
Collaboration
(2023).
“Table 18” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t23
CMS
Collaboration
(2023).
“Table 19” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t24
CMS
Collaboration
(2023).
“Table 20” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t25
CMS
Collaboration
(2023).
“Table 21” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t26
CMS
Collaboration
(2023).
“Table 22” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t27
CMS
Collaboration
(2023).
“Table 23” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t28
CMS
Collaboration
(2023).
“$M_\mathrm{T2}$ covariance matrix” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t29
CMS
Collaboration
(2023).
“$M_\mathrm{T2}$ correlation matrix” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t30
CMS
Collaboration
(2023).
“$M_\mathrm{T2}$ covariance matrix bin mappings” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t31
CMS
Collaboration
(2023).
“Figure 17 (T1qqqq 10 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t32
CMS
Collaboration
(2023).
“Figure 17 (T1qqqq 50 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t33
CMS
Collaboration
(2023).
“Figure 17 (T1qqqq 200 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t34
CMS
Collaboration
(2023).
“Figure 18 (T2qq 10 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t35
CMS
Collaboration
(2023).
“Figure 18 (T2qq 50 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t36
CMS
Collaboration
(2023).
“Figure 18 (T2qq 200 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t37
CMS
Collaboration
(2023).
“Figure 19 (T2bt 10 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t38
CMS
Collaboration
(2023).
“Figure 19 (T2bt 50 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t39
CMS
Collaboration
(2023).
“Figure 19 (T2bt 200 cm)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t40
CMS
Collaboration
(2023).
“Figure 20 (T1qqqq Max Chargino Exclusion)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t41
CMS
Collaboration
(2023).
“Figure 20 (T2qq, one light squark, Max Chargino Exclusion)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t42
CMS
Collaboration
(2023).
“Figure 20 (T2qq Max Chargino Exclusion)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t43
CMS
Collaboration
(2023).
“Figure 21 (T2bt Max Chargino Exclusion)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t44
CMS
Collaboration
(2023).
“Figure 22 (T1qqqq Fixed Masses)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t45
CMS
Collaboration
(2023).
“Figure 22 (T2qq Fixed Masses)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t46
CMS
Collaboration
(2023).
“Figure 22 (T2bt Fixed Masses)” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t47
CMS
Collaboration
(2023).
“Table 24” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t48
CMS
Collaboration
(2023).
“Table 25” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t49
CMS
Collaboration
(2023).
“Table 26” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t50
CMS
Collaboration
(2023).
“$M_\mathrm{T2}$ disappearing tracks covariance matrix” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t51
CMS
Collaboration
(2023).
“$M_\mathrm{T2}$ disappearing tracks correlation matrix” of “Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV” (Version 1). HEPData (dataset).
https://doi.org/10.17182/hepdata.90834.v1/t52
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CMS
Collaboration
(2020).
Searches for physics beyond the standard model with the $M_\mathrm{T2}$ variable in hadronic final states with and without disappearing tracks in proton-proton collisions at $\sqrt{s}=$ 13 TeV. Eur.Phys.J.C 80 (2020) 3.
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