Data (bold boxes) and background estimates (colour fill) for m_beta vs. m_betagamma for the gluino R-hadron search (1000 GeV). The blue thin-line boxes illustrate the expected signal (on top of background) for the given R-hadron mass hypothesis. The black dashed vertical/horizontal lines at 500 GeV show the mass selection (signal region in the top-right). Two events pass this selection.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of bottom-squark R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Expected (dashed black line) and observed (solid red line) 95% CL upper limits on the cross section as a function of mass for the production of top-squark R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. The observed 8 TeV Run-1 limit and theory prediction [arXiv:1411.6795] are shown in dash-dotted and dotted lines, respectively.

Distribution of the truth-level beta for gluino R-hadrons in exemplary signal MC samples and muons in a Zmumu MC sample. All distributions have been normalised to one. The last bin contains the overflow of the histograms. The distributions illustrate the good discriminating power of the variables.

Distribution of the truth-level betagamma for gluino R-hadrons in exemplary signal MC samples and muons in a Zmumu MC sample. All distributions have been normalised to one. The last bin contains the overflow of the histograms. The distributions illustrate the good discriminating power of the variables.

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 50 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 30 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

Expected (dashed black line) and observed (solid red line) 95% confidence level upper limits on the cross section as a function of mass for the production of long-lived gluino R-hadrons. The theory prediction along with its +-1sigma uncertainty is show as a black line and a blue band, respectively. For meta-stable gluinos with a lifetime of 10 ns. (mass exclusion: about 1660 GeV expected, 1520 GeV observed).

The leptonic asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.

The leptonic asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.

The leptonic asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.

The top-antitop inclusive asymmetry in the fiducial volume.

The top-antitop asymmetry dependence on the invariant mass of top-antitop system ($m_{t\bar{t}}$) in the fiducial volume.

The top-antitop asymmetry dependence on the longitudinal boost of the top-antitop system ($\beta_z^{t\bar{t}}$) in the fiducial volume.

The top-antitop asymmetry dependence on the transverse momentum of the top-antitop system ($p_T^{t\bar{t}}$) in the fiducial volume.

The measured fiducial cross sections are corrected to the dressed level. The ratio of $C_{WZ}^{\textrm{dressed}}/C_{WZ}^{\textrm{Born}}$ factors presented in this table can be used to correct fiducial integrated cross sections from dressed to Born level.

Cross section extrapolated to total phase space and all W and Z boson decays. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the theory uncertainty and the third is the luminosity uncertainty.

The total cross section is measured at dressed level and can also be corrected to Born level use this acceptance correction factor.

Ratio of fiducial cross sections measured for $W^{+} Z$ and $W^{-} Z$ production. The first systematic uncertainty is the combined systematic uncertainty excluding the luminosity uncertainty, the second is the luminosity uncertainty.

Observed and expected upper limits at $95\%$ CL in fb on the fiducial cross section $\sigma^{\mathrm{fid.}}_{W^{\pm} Zjj \textrm{-EW} \rightarrow \ell^{'} \nu \ell \ell}$, multiplied by the $W$ and $Z$ branching ratios in a single leptonic channel with muons or electrons in the VBS fiducial phase space. Values obtained with or without subtraction of the $tZj$ contribution are presented. The $1$ $\sigma$ and $2$ $\sigma$ uncertainty intervals around the expected limits are also indicated.

Observed and expected upper limits at $95\%$ CL in fb on the fiducial cross section $\sigma^{\mathrm{fid.}}_{W^{\pm} Zjj \textrm{-EW} \rightarrow \ell^{'} \nu \ell \ell}$, multiplied by the $W$ and $Z$ branching ratios in a single leptonic channel with muons or electrons in the aQGC fiducial phase space. Values obtained with or without subtraction of the $tZj$ contribution are presented. The $1$ $\sigma$ and $2$ $\sigma$ uncertainty intervals around the expected limits are also indicated.

Expected and observed one-dimensional 95% Confidence Level intervals on the anomalous couplings parameters. Anomalous couplings are introduced as form factors using a cut-off scale $\Lambda_{\mathrm{co}}$.

Expected and observed one-dimensional intervals at 95% Confidence Level on the Effective Field Theory (EFT) parameters.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Measured normalised fiducial cross section in all $\ell'^\pm \nu \ell^+ \ell^-$ channels combined, where $\ell, \ell' = e, \mu$. The first systematic uncertainty is the combined systematic uncertainty excluding theory and luminosity uncertainties, the second is the luminosity uncertainty. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$. The last bin is a cross section for all events above the lower end of the bin.

Ratio of $W^{+}Z$ over $W^{-}Z$ differential fiducial cross sections measured in all $\ell'^\pm \nu \ell^+ \ell'^-$ channels combined, where $\ell, \ell' = e, \mu$.

TOTAL NUMBER EVENTS=1093. DATA FROM T 1.

TOTAL NUMBER EVENTS=581. DATA FROM T 1.

TOTAL NUMBER EVENTS=3678. DATA FROM T 1. ALREADY PUBLISHED IN 'ADERHOLTZ ET AL' NP B8,45(1968).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = .784 GEV; WIDTH = .045], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .549 GEV; WIDT H = .046], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ETA PRODUCED THROUGH THE X0 MESON IS EXCLUDED.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = .965 GEV; WIDTH = .004], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND). [MASS CUT FROM .500 TO .600 GEV].. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.329 GEV; WIDTH = .052], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = .756 GEV; WIDT H = .115], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 8. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND). [MASS = .750 GEV; WIDTH = .825]. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 9. THE UPPER LIMITS OF CROSS-SECTIONS ARE CALCULATED WITH CONFIDENCE LEVEL OF 68 PERCENT.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.211 GEV; WIDTH = .100], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.

TOTAL NUMBER EVENTS=199. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=58. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED FOR MASS AND/OR WIDTH. [MASS = 1.221 GEV; WIDTH = .098], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=423. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=58. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=33. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. TOTAL NUMBER EVENTS=225. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. FITTED DISTRIBUTION WITH FIXED MASS AND WIDTH. [MASS = 1.230 GEV; WIDT H = .120], AND THEN TOOK ONLY EVENTS ABOVE (FITTED) BACKGROUND.. DATA FROM T 10. ERRORS CORRESPOND TO 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. DATA FROM T 11. THE UPPER LIMITS OF CROSS-SECTION FOR PRODUCTION OF N*(1518) AND N*(1688 ) ARE ESTIMATED WITH 68 PERCENT CONFIDENCE LEVEL.

TOTAL NUMBER EVENTS= 5. DATA FROM P2729.

TOTAL NUMBER EVENTS= 8. DATA FROM P2731. ALREADY PUBLISHED IN PL 29B,529(69).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=53. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=14. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=83. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=98. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS= 9. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

TOTAL NUMBER EVENTS=247. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=136. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. MADE SIMPLE MASS CUT (NEGLIGIBLE BACKGROUND).. TOTAL NUMBER EVENTS=67. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3).

TOTAL NUMBER EVENTS=150. DATA FROM T 12. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2)AND (P PI+3). AT LEAST TWO RESONANCES IN AN EVENT.

TOTAL NUMBER EVENTS=75. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=48. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=229. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=41. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=128. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=183. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=42. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=319. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=304. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=123. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

INCLUDES EVENTS WHERE SOME OF THE PARTICLES OR RESONANCES LISTED MAY BE R ESONATING WITH EACH OTHER. TOTAL NUMBER EVENTS=203. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

TOTAL NUMBER EVENTS=480. DATA FROM T 13. THE ANALYSIS HAS BEEN PERFORMED IN THE 3-DIMENSIONAL SPACE OF THE EFF ECTIVE MASSES OF THE SYSTEMS(PI+1PI-1),(PI+2PI-2PI0)AND (P PI+.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

DATA FROM T 14. THESE CROSS-SECTIONS WERE CALCULATED ASSUMING THAT NO RHO IS PRODUCED.TH EY HAVE BEEN CORRECTED FOR UNSEEN DECAY MODES.

The expected limit contour in the GLUINO-NEUTRALINO plane.

The observed limit contour in the SQUARK-NEUTRALINO plane.

The expected limit contour in the SQUARK-NEUTRALINO plane.