Large Hadron Collider Workshop: Aachen, 4-9 October 1990, Volume 3G. Jarlskog, D. Rein |
From inside the book
Results 1-3 of 39
Page
... tracker . F.Udo NIKHEF - H Amsterdam . Sept. 1990 . The paper discusses a LHC tracker constructed with microstrip gas counters ( ref1 ) in a solenoidal field of 4 Tesla . Figure 1 shows a cross section of a microstrip gas counter ( MSGC ) ...
... tracker . F.Udo NIKHEF - H Amsterdam . Sept. 1990 . The paper discusses a LHC tracker constructed with microstrip gas counters ( ref1 ) in a solenoidal field of 4 Tesla . Figure 1 shows a cross section of a microstrip gas counter ( MSGC ) ...
Page
... tracker has to fulfil specific requirements as high granularity to reduce the occupancy and to guarantee the required spatial resolution . Furthermore the detector has to be sufficiently radiation hard and finally the readout has to ...
... tracker has to fulfil specific requirements as high granularity to reduce the occupancy and to guarantee the required spatial resolution . Furthermore the detector has to be sufficiently radiation hard and finally the readout has to ...
Page
... tracker must provide time resolutions ≤ 10 ns and 2 - track resolutions ≤ 100 μm associated with excellent spatial precision . In addition , low occupancy of the detector elements will be vital and visual pattern recognition via CCD ...
... tracker must provide time resolutions ≤ 10 ns and 2 - track resolutions ≤ 100 μm associated with excellent spatial precision . In addition , low occupancy of the detector elements will be vital and visual pattern recognition via CCD ...
Contents
Plenary Sessions | |
Further progress in the development of the microstrip gas chamber | |
Simulation of sampling calorimeters M Nessi et | |
Copyright | |
8 other sections not shown
Common terms and phrases
absorber additional allow angle applications assumed beam calculated calorimeter cell central CERN chamber channel charge coil colliders compared components containing contribution cross crystal damage decay depends described detector devices distribution dose effect efficiency electron energy example expected experiment experimental factor fibres field Figure function geometry GeV/c given gives hadron important increase integrated interaction iron irradiation Italy jets layer lead length light limit liquid loss luminosity magnetic material measured module momentum muon needed neutron obtained operation parameters particle performance physics position possible present processing production proposed radiation range readout reduced References region resolution response sampling scintillating shower shown shows signal silicon simulation single standard strips structure Table thickness tracking trigger values voltage