Author/Authors :
Gori?ek، نويسنده , , A. and Cindro، نويسنده , , Jurij V. and Dolenc، نويسنده , , I. and Frais-K?lbl، نويسنده , , H. and Griesmayer، نويسنده , , E. and Kagan، نويسنده , , H. and Korpar، نويسنده , , S. and Kramberger، نويسنده , , G. and Mandic، نويسنده , , I. and Meyer، نويسنده , , M. and Miku?، نويسنده , , M. and Pernegger، نويسنده , , H. and Smith، نويسنده , , S. and Trischuk، نويسنده , , W. and Weilhammer، نويسنده , , P. and Zavrtanik، نويسنده , , M.، نويسنده ,
Abstract :
The ATLAS experiment has chosen to use diamond for its Beam Condition Monitor (BCM) given its radiation hardness, low capacitance and short charge collection time. In addition, due to low leakage current diamonds do not require cooling. The ATLAS Beam Condition Monitoring system is based on single beam bunch crossing measurements rather than integrating the accumulated particle flux. Its fast electronics will allow separation of LHC collisions from background events such as beam gas interactions or beam accidents. There will be two stations placed symmetrically about the interaction point along the beam axis at z = ± 183.8 cm . Timing of signals from the two stations will provide almost ideal separation of beam–beam interactions and background events. The ATLAS BCM module consists of diamond pad detectors of 1 cm 2 area and 500 μ m thickness coupled to a two-stage RF current amplifier. The production of the final detector modules is almost done. A S / N ratio of 10:1 has been achieved with minimum ionizing particles (MIPs) in the test beam setup at KEK. Results from the test beams and bench measurements are presented.
Keywords :
Minimum ionizing particle , ATLAS spectrometer , PCVD diamond , Solid state detectors , Beam condition monitor , Large hadron collider
