Difference: PhysicsResultsSUS (1 vs. 22)

Revision 222019-09-09 - PieterEveraerts

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

Line: 13 to 13
 

Summer Conferences 2019 (77 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage conference
Added:
>
>
1L MJ 137 SUS-19-007 link LP
ISR + tau 77 SUS-19-002 link LP
 
Stop 1L 137 SUS-19-009 link EPS
0L + multijets with MHT 137 SUS-19-006 link EPS
Razor/MT2 with H->gg 77 SUS-18-007 link LHCP

Revision 212019-09-03 - PieterEveraerts

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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META TOPICMOVED by="moortgat" date="1458313125" from="CMS.PhysicsResultsSUS" to="CMSPublic.PhysicsResultsSUS"
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Revision 202019-07-19 - SeemaSharma

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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0L + multijets with MHT 137 SUS-19-006 link EPS
Razor/MT2 with H->gg 77 SUS-18-007 link LHCP
stop to taus 77 SUS-19-003 link LHCP
Added:
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Compressed in VBF 0L & 1L 36 SUS-17-007 link --
 

Moriond 2019 (36 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage

Revision 192019-07-15 - SeemaSharma

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

Line: 13 to 13
 

Summer Conferences 2019 (77 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage conference
Added:
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>
Stop 1L 137 SUS-19-009 link EPS
0L + multijets with MHT 137 SUS-19-006 link EPS
 
Razor/MT2 with H->gg 77 SUS-18-007 link LHCP
stop to taus 77 SUS-19-003 link LHCP

Revision 182019-07-11 - PieterEveraerts

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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Revision 172019-07-10 - PieterEveraerts

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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META TOPICMOVED by="moortgat" date="1458313125" from="CMS.PhysicsResultsSUS" to="CMSPublic.PhysicsResultsSUS"
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Revision 162019-05-24 - SeemaSharma

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

Line: 14 to 14
 

Summer Conferences 2019 (77 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage conference
Razor/MT2 with H->gg 77 SUS-18-007 link LHCP
Added:
>
>
stop to taus 77 SUS-19-003 link LHCP
 

Moriond 2019 (36 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage

Revision 152019-05-21 - SeemaSharma

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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Run 2 Summaries -- 13 TeV

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Summer Conferences 2019 (77 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage conference
Razor/MT2 with H->gg 77 SUS-18-007 link LHCP
 

Moriond 2019 (36 fb-1 -- 137 fb-1)

channel luminosity (fb-1) PAS/arXiv webpage
stau combination 77 SUS-18-006 link

Revision 142019-03-31 - LesyaShchutska

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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

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Questions? Contact the CMS SUSY Conveners
 
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Run 2 Summary plots -- 13 TeV, 2015 and 2016 datasets

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Overview of mass limits
Synopsis of the mass reach (limits at 95% CL) obtained in the context of simplified models and for different final states. The arXiv and physics analysis summary numbers in each line indicate the analyses with relevant results. Details on the models, assumptions and selections can be found in the documentation of each analysis.
barplot_Gluino.png
png pdf
Mass reach for simplified models of gluino pair production. Limits on gluino production with GMSB are shown in a separate figure.
barplot_Squark.png
png pdf
Mass reach for simplified models of squark pair production. Limits on squark production with GMSB are shown in a separate figure.
barplot_EWK.png
png pdf
Mass reach for simplified models of electroweak production of pairs of gauginos or sleptons.
barplot_GMSB.png
png pdf
Mass reach for simplified models in the context of gauge-mediated supersymmetry breaking.
 
Gluino pair production
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
T1tttt_limits_summary_cms.png
png pdf
Mass limits for a simplified model of gluino pair production with gluino decays to pairs of top quarks and the LSP.
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T2qq_limits_summary_cms.png
png pdf
Mass limits for a simplified model of first or second generation squark pair production with squark decays to a quark and the LSP. The solid (dashed) lines correspond to the observed (median expected) limits. Limits are shown for two scenarios: production of eight degenerate squarks, or of a single squark.
Chargino-neutralino or slepton pair production
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
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WH_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decays to W and H bosons, respectively, and the LSP. The two gauginos are assumed to have the same mass.
EWKino_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP, and two alternative scenarios for the neutralino via a H or a Z boson. The two gauginos are assumed to have the same mass.
EWKComb_limits_summary_cms.png
png pdf
Combined mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP. For the neutralino, three scenarios are shown, with a 100% branching fraction to a H boson and the LSP, a 100% branching fraction to a Z boson and the LSP, and 50% branching fractions for both decays. The two gauginos are assumed to have the same mass.
>
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WH_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decays to W and H bosons, respectively, and the LSP. The two gauginos are assumed to have the same mass.

Updated 23/7/2018
EWKino_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP, and two alternative scenarios for the neutralino via a H or a Z boson. The two gauginos are assumed to have the same mass.

Updated 23/7/2018
EWKComb_limits_summary_cms.png
png pdf
Combined mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP. For the neutralino, three scenarios are shown, with a 100% branching fraction to a H boson and the LSP, a 100% branching fraction to a Z boson and the LSP, and 50% branching fractions for both decays. The two gauginos are assumed to have the same mass.

Updated 23/7/2018
 
Chargino-neutralino pair production with decays via sleptons
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
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Sleptons_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decay chains involving sleptons. The two gauginos are assumed to have the same mass. Three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$.
EWK-slep_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.
EWK-slep-0p5_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The mass of the slepton is set to the average of $m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}$ and $m_{\tilde{\chi}^{0}_{1}}$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.
>
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Sleptons_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decay chains involving sleptons. The two gauginos are assumed to have the same mass. Three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$.

Updated 23/7/2018
EWK-slep_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.

Updated 23/7/2018
EWK-slep-0p5_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The mass of the slepton is set to the average of $m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}$ and $m_{\tilde{\chi}^{0}_{1}}$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.

Updated 23/7/2018
 
EWK production - most stringent limits
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
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EWK-best_limits_summary_cms.png
png pdf
Summary of the most stringent limits obtained by CMS searches for the production of pairs of the lightest chargino and the second-lightest neutralino, of chargino pairs, and of slepton pairs. The models for the first category are described above. The same assumptions are made for chargino pair production. For slepton production, the four states corresponding to left- and right-handed leptons of the first two generations are assumed to be mass degenerate.
>
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EWK-best_limits_summary_cms.png
png pdf
Summary of the most stringent limits obtained by CMS searches for the production of pairs of the lightest chargino and the second-lightest neutralino, of chargino pairs, and of slepton pairs. The models for the first category are described above. The same assumptions are made for chargino pair production. For slepton production, the four states corresponding to left- and right-handed leptons of the first two generations are assumed to be mass degenerate.

Updated 23/7/2018
 
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Revision 32018-07-19 - WolfgangAdam

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CMS Supersymmetry Physics Results

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Run 2 Summary plots -- 13 TeV, 2015 and 2016 datasets

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Gluino pair production
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
T1tttt_limits_summary_cms.png
png pdf
Mass limits for a simplified model of gluino pair production with gluino decays to pairs of top quarks and the LSP.
T1bbbb_limits_summary_cms.png
png pdf
Mass limits for a simplified model of gluino pair production with gluino decays to pairs of bottom quarks and the LSP.
T1qqqq_limits_summary_cms.png
png pdf
Mass limits for a simplified model of gluino pair production with gluino decays to pairs of light quarks and the LSP.
T5qqqqVV_limits_summary_cms.png
png pdf
Mass limits for a simplified model of gluino pair production with gluino decays via an intermediate chargino ($\tilde{\chi}^{\pm}_{1}$) or neutralino ($\tilde{\chi}^{0}_{2}$) to a final state with a quark, an antiquark, and either a W± or a Z boson. The mass of the intermediate gaugino is set to the average of the top squark and LSP masses.
Squark pair production
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
T2tt_limits_summary_cms.png
png pdf
Mass limits for a simplified model of top squark pair production with squark decays to a on- or off-shell top quark and the LSP, leading to final states with two bottom quarks, two W bosons, and two LSPs.
T2tt234body_limits_summary_cms.png
png pdf
Mass limits for a simplified model of top squark pair production with top squark decays via on- or off-shell top quarks and W bosons. Three kinematic areas are shown that correspond to decays to a top quark and the LSP; a bottom quark, W boson, and the LSP; and a four-body decay to a bottom quark, a fermion-antifermion pair, and the LSP. The top squark is assumed to decay promptly.
T2tt4body-c_limits_summary_cms.png
png pdf
Mass limits for simplified models of top squark pair production with top squarks decaying either a bottom quark, a fermion-antifermion pair, and an LSP, or to a charm quark and the LSP. The limits are shown in the plane of the top squark mass and the mass difference between the squark and the LSP. The top squark is assumed to decay promptly.
T6bbWW_limits_summary_cms.png
png pdf
Mass limits for a simplified model of top squark pair production with top squark decays via an intermediate chargino ($\tilde{\chi}^{\pm}_{1}$) or neutralino ($\tilde{\chi}^{0}_{2}$). The mass of the intermediate gaugino is set to the average of the top squark and LSP masses. For models covering both scenarios, the branching fraction to each of the states is set to 1/3.
T2bb_limits_summary_cms.png
png pdf
Mass limits for a simplified model of bottom squark pair production with squark decays to a bottom quark and the LSP.
T2qq_limits_summary_cms.png
png pdf
Mass limits for a simplified model of first or second generation squark pair production with squark decays to a quark and the LSP. The solid (dashed) lines correspond to the observed (median expected) limits. Limits are shown for two scenarios: production of eight degenerate squarks, or of a single squark.
Chargino-neutralino or slepton pair production
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
WH_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decays to W and H bosons, respectively, and the LSP. The two gauginos are assumed to have the same mass.
EWKino_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP, and two alternative scenarios for the neutralino via a H or a Z boson. The two gauginos are assumed to have the same mass.
EWKComb_limits_summary_cms.png
png pdf
Combined mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with chargino decays to a W boson and the LSP. For the neutralino, three scenarios are shown, with a 100% branching fraction to a H boson and the LSP, a 100% branching fraction to a Z boson and the LSP, and 50% branching fractions for both decays. The two gauginos are assumed to have the same mass.
Chargino-neutralino pair production with decays via sleptons
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
Sleptons_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino, with decay chains involving sleptons. The two gauginos are assumed to have the same mass. Three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$.
EWK-slep_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The x-values shown in the legend indicate the ratios of the mass differences, $(m_{\tilde{l}}-m_{\tilde{\chi}^{0}_{1}})/(m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}-m_{\tilde{\chi}^{0}_{1}})$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.
EWK-slep-0p5_limits_summary_cms.png
png pdf
Mass limits for simplified models for the production of pairs of the lightest chargino and the second-lightest neutralino. The two gauginos are assumed to have the same mass. Two sets of results are shown. In the first set, decays proceed via a slepton. Here, three scenarios are considered: a "flavour-democratic" model with the same branching fractions to all lepton flavours, a "tau-enriched" model with 100% branching fraction of the chargino to $\tilde{\tau}$, while the neutralino decays to all three flavours, and a "tau-dominated" model with both chargino and neutralino decays proceeding exclusively via $\tilde{\tau}$. The mass of the slepton is set to the average of $m_{\tilde{\chi}^{\pm}_{1},\tilde{\chi}^{0}_{2}}$ and $m_{\tilde{\chi}^{0}_{1}}$. For the second set of results, the chargino decays to a W boson and the LSP, and while the neutralino decays via a H or a Z boson.
EWK production - most stringent limits
Mass limits at 95% CL obtained in the context of simplified models. In the figures, the solid (dashed) lines correspond to the observed (median expected) limits. The arXiv numbers corresponding to the different analyses are shown in the legend. Details on the models and the selections can be found in the documentation of each analysis.
EWK-best_limits_summary_cms.png
png pdf
Summary of the most stringent limits obtained by CMS searches for the production of pairs of the lightest chargino and the second-lightest neutralino, of chargino pairs, and of slepton pairs. The models for the first category are described above. The same assumptions are made for chargino pair production. For slepton production, the four states corresponding to left- and right-handed leptons of the first two generations are assumed to be mass degenerate.
 

Run 1 Summary plots -- 7 and 8 TeV

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Revision 12018-07-18 - LesyaShchutska

Line: 1 to 1
Added:
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META TOPICPARENT name="CMSPublic.PhysicsResults"

CMS Supersymmetry Physics Results

Questions? Contact the CMS SUSY Conveners

Links to list of all CMS SUSY results

Recent CMS SUSY physics results, preliminary and final

Other / older results

Run 2 Summaries -- 13 TeV

Summer 2018 (36 fb-1)

channel PAS/arXiv webpage conference
stau combination SUS-17-003 link ICHEP'18
photon + 1L + MET SUS-17-012 link ICHEP'18
RPV smuon SUS-17-008 link LHCP'18

Winter/Spring 2018 (36 fb-1)

channel PAS/arXiv webpage
0L + jets with alphaT SUS-16-038 link
1L compressed stop MVA SUS-17-005 link
2lOS charginos / compressed stop SUS-17-010 link
LQ with MT2 SUS-18-001 link

Fall/Winter 2017 (36 fb-1)

channel PAS/arXiv webpage conference
stau (1L/2L) SUS-17-002 link SUSY'17
sleptons SUS-17-009 link SUSY'17
gluino / boosted H SUS-17-006 link SUSY'17

Summer Conferences 2017 (36 fb-1)

channel PAS/arXiv webpage conference
0L + top tag SUS-16-050 link LHCP
1L compressed stop SUS-16-052 link EPS
Hadronic staus SUS-17-003 link EPS
Ewkino combination SUS-17-004 link EPS
1L RPV SUS-16-040 link LP

Moriond 2017 (36 fb-1)

channel PAS/arXiv webpage channel PAS/arXiv webpage
0L + jets with MHT SUS-16-033 link   Photon + MET SUS-16-046 link
0L + jets with MT2 SUS-16-036 link   Photon + HT SUS-16-047 link
1L + jets + MET with MJ SUS-16-037 link   Stop 0L SUS-16-049 link
1L + jets + MET with ΔΦ SUS-16-042 link   Stop 1L SUS-16-051 link
2SS Leptons SUS-16-035 link   Stop 2L SUS-17-001 link
multilepton EWK SUS-16-039 link   Sbottom and compressed stop SUS-16-032 link
multileptons + jets SUS-16-041 link   GMSB Higgsinos in 4b SUS-16-044 link
2L soft SUS-16-048 link   2OS leptons SUS-16-034 link
Razor + Higgs->gg SUS-16-045 link   EWK WH(bb) SUS-16-043 link

Run 2 Summary plots -- 13 TeV, 2015 and 2016 datasets

Run 1 Summary plots -- 7 and 8 TeV

Publications in CERN Document Server

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