Abstract
A high resolution multijet analysis of hadronic events produced in e{sup +}e{sup -}annihilation at a C.M.S. energy of 91.2 GeV is described. Hadronic events produced in e{sup +}e{sup -} annihilations are generated using the Monte Carlo program JETSET7.3 with its two options: Matrix Element (M.E.) and Parton Showers (P.S.). The shower option is used with its default parameter values while the M.E. option is used with an invariant mass cut Y{sub CUT}=0.01 instead of 0.02. This choice ensures a better continuity in the evolution of the event shape variables. (K.A.) 3 refs.; 26 figs.; 1 tab.
Citation Formats
Hariri, S.
A high resolution jet analysis for LEP.
France: N. p.,
1992.
Web.
Hariri, S.
A high resolution jet analysis for LEP.
France.
Hariri, S.
1992.
"A high resolution jet analysis for LEP."
France.
@misc{etde_10109892,
title = {A high resolution jet analysis for LEP}
author = {Hariri, S}
abstractNote = {A high resolution multijet analysis of hadronic events produced in e{sup +}e{sup -}annihilation at a C.M.S. energy of 91.2 GeV is described. Hadronic events produced in e{sup +}e{sup -} annihilations are generated using the Monte Carlo program JETSET7.3 with its two options: Matrix Element (M.E.) and Parton Showers (P.S.). The shower option is used with its default parameter values while the M.E. option is used with an invariant mass cut Y{sub CUT}=0.01 instead of 0.02. This choice ensures a better continuity in the evolution of the event shape variables. (K.A.) 3 refs.; 26 figs.; 1 tab.}
place = {France}
year = {1992}
month = {Nov}
}
title = {A high resolution jet analysis for LEP}
author = {Hariri, S}
abstractNote = {A high resolution multijet analysis of hadronic events produced in e{sup +}e{sup -}annihilation at a C.M.S. energy of 91.2 GeV is described. Hadronic events produced in e{sup +}e{sup -} annihilations are generated using the Monte Carlo program JETSET7.3 with its two options: Matrix Element (M.E.) and Parton Showers (P.S.). The shower option is used with its default parameter values while the M.E. option is used with an invariant mass cut Y{sub CUT}=0.01 instead of 0.02. This choice ensures a better continuity in the evolution of the event shape variables. (K.A.) 3 refs.; 26 figs.; 1 tab.}
place = {France}
year = {1992}
month = {Nov}
}