squark/gluino->ee Search

Results from search for squarks in the channel 2 electrons plus MET plus 2 jets.

• Limit plot tan beta = 2 limit plot from 20 may 1997 in m(squark) m(gluino) plane
• Limit plot tan beta = 2 limit plot from 20 may 1997 in m0 mhalf plane
• Limit plot tan beta = 6 limit plot from 20 may 1997 in m0 mhalf plane
• cross sections shows cross sections for sparticle production versus m0 for tanb=2 (20may1997)
• cross sections shows cross sections for sparticle production versus m0 for tanb=6 (20may1997)
• mass splitting shows mass splitting between wino1 and zino1 versus m0 for mhalf=50
• mass splitting shows mass splitting between wino1 and zino1 versus m0 for mhalf=70
• mass splitting shows mass splitting between wino1 and zino1 versus m0 for mhalf=90
• Limit plot 95% C.L. Exclusion contour in the m_0-m_1/2 plane for SUGRA motivated susy search in the dielectron channel for tan beta=2 and negative mu The "dip" in the exclusion contour is where the decay zino_2-> sneutrino sneutrino becomes dominant; the rise at lower m_0 is where the decay zino_2 -> selectron selectron contributes to the signal.

• Limit plot 95% C.L. Exclusion contour in the m_0-m_1/2 plane for SUGRA motivated susy search in the dielectron channel superimposed on contours of constant gluino mass for tan beta=2 and negative mu

• Limit plot 95% C.L. Exclusion contour in the m_0-m_1/2 plane for SUGRA motivated susy search in the dielectron channel superimposed on contours of constant squark mass for tan beta=2 and negative mu. This limit is valid for all squarks except stop

• Limit plot 95% C.L. Exclusion contour in the m_0-m_1/2 plane for SUGRA motivated susy search in the dielectron channel superimposed on contours of constant lightest chargino mass for tan beta=2 and negative mu.

• Limit plot 95% C.L. Exclusion contour in the m_0-m_1/2 plane for SUGRA motivated susy search in the dielectron channel superimposed on contours of constant lightest chargino mass for tan beta=2 and negative mu.

• Cut Distributions Electron isolation cut vs. electron ET for QCD background events

• Cut Distributions Electron isolation cut vs. electron ET for signal M.C. events for m_0 = 140 GeV and m_1/2 = 60 GeV

• Cut Distributions Missing ET vs dielectron invarient mass for Z --> ee M.C. events

• Cut Distributions Missing ET vs. dielectron invarient mass for signal M.C. events for m_0 = 140 GeV and m_1/2 = 60 GeV

• Cut Distributions Missing ET distribution for Z --> tau tau --> ee M.C. events.

• Cut Distributions Missing Et distribution for signal M.C. events for m_0 = 140 GeV and m_1/2 = 60 GeV

• Cut Distributions No. of jets distribution with jet ET > 20 GeV for WW --> ee backgrounds.

• Cut Distributions No. of jets distribution with jet ET > 20 GeV for signal M.C. events