Supersymmetric Particle Searches INSPIRE search
The exclusion of particle masses within a mass range (${\mathit m}_{\mathrm {1}}$, ${\mathit m}_{\mathrm {2}}$) will be denoted with the notation none ${\mathit m}_{\mathrm {1}}−{\mathit m}_{\mathrm {2}}$'' in the VALUE column of the following Listings. The latest unpublished results are described in the Supersymmetry: Experiment'' review.
 See related reviews: Supersymmetry, Part I (Theory) Supersymmetry, Part II (Experiment) Supersymmetric Model Assumptions
${{\widetilde{\boldsymbol \chi}}_{{1}}^{0}}$ (Lightest Neutralino) mass limit
 Accelerator limits for stable ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ $>46$ GeV  CL=95.0%
 Bounds on ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ from dark matter searches
${{\widetilde{\boldsymbol \chi}}_{{1}}^{0}}-{{\boldsymbol p}}$ elastic cross section
 Spin-dependent interactions
 Spin-independent interactions
 Other bounds on ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ from astrophysics and cosmology
 Unstable ${{\widetilde{\mathit \chi}}_{{1}}^{0}}$ (Lightest Neutralino) mass limit $> 380$ GeV  CL=95.0%
 ${{\widetilde{\mathit \chi}}_{{2}}^{0}}$, ${{\widetilde{\mathit \chi}}_{{3}}^{0}}$, ${{\widetilde{\mathit \chi}}_{{4}}^{0}}$ (Neutralinos) mass limits $> 620$ GeV  CL=95.0%
 ${{\widetilde{\mathit \chi}}_{{1}}^{\pm}}$, ${{\widetilde{\mathit \chi}}_{{2}}^{\pm}}$ (Charginos) mass limits $>94$ GeV  CL=95.0%
 Long-lived ${{\widetilde{\mathit \chi}}^{\pm}}$ (Chargino) mass limit $>620$ GeV  CL=95.0%
 ${{\widetilde{\mathit \nu}}}$ (Sneutrino) mass limit $>94$ GeV  CL=95.0%
Charged sleptons
 R-parity conserving ${{\widetilde{\mathit e}}}$ (Selectron) mass limit $>107$ GeV  CL=95.0%
 R-partiy violating ${{\widetilde{\mathit e}}}$ (Selectron) mass limit $> 410$ GeV  CL=95.0%
 R-parity conserving ${{\widetilde{\mathit \mu}}}$ (Smuon) mass limit $>94$ GeV  CL=95.0%
 R-parity violating ${{\widetilde{\mathit \mu}}}$ (Smuon) mass limit $> 410$ GeV  CL=95.0%
 R-parity conserving ${{\widetilde{\mathit \tau}}}$ (Stau) mass limit $>81.9$ GeV  CL=95.0%
 R-parity violating ${{\widetilde{\mathit \tau}}}$ (Stau) mass limit
 Long-lived ${{\widetilde{\mathit \ell}}}$ (Slepton) mass limit $>286$ GeV  CL=95.0%
${{\widetilde{\boldsymbol q}}}$ (Squark) mass limit
 R-parity conserving ${{\widetilde{\mathit q}}}$ (Squark) mass limit $> 1550$ GeV  CL=95.0%  ...
 R-parity violating ${{\widetilde{\mathit q}}}$ (Squark) mass limit
 Long-lived ${{\widetilde{\mathit q}}}$ (Squark) mass limit $>1.000 \times 10^{3}$ GeV  CL=95.0%
${{\widetilde{\boldsymbol b}}}$ (Sbottom) mass limit
 R-parity conserving ${{\widetilde{\mathit b}}}$ (Sbottom) mass limit
 R-parity violating ${{\widetilde{\mathit b}}}$ (Sbottom) mass limit $> 307$ GeV  CL=95.0%
${{\widetilde{\boldsymbol t}}}$ (Stop) mass limit
 R-parity conserving ${{\widetilde{\mathit t}}}$ (Stop) mass limit $>1.120 \times 10^{3}$ GeV  CL=95.0%
 R-parity violating ${{\widetilde{\mathit t}}}$ (Stop) mass limit
 Heavy ${{\widetilde{\mathit g}}}$ (Gluino) mass limit $>1.860 \times 10^{3}$ GeV  CL=95.0%
 Long-lived ${{\widetilde{\mathit g}}}$ (Gluino) mass limit
 Light ${{\widetilde{\mathit G}}}$ (Gravitino) mass limits from collider experiments
 Supersymmetry miscellaneous results