TY - JOUR
T1 - Simulation ofspace-chargeeffectsinanungatedgem-basedtpc
AU - Böhmer, F. V.
AU - Ball, M.
AU - Dørheim, S.
AU - Höppner, C.
AU - Ketzer, B.
AU - Konorov, I.
AU - Neubert, S.
AU - Paul, S.
AU - Rauch, J.
AU - Vandenbroucke, M.
PY - 2013
Y1 - 2013
N2 - A fundamental limit to the application of Time Projection Chambers (TPCs) in high-rate experiments is the accumulation of slowly drifting ions in the active gas volume, which compromises the homogeneity of the drift field and hence the detector resolution. Conventionally, this problem is overcome by the use of ion-gating structures. This method, however, introduces large dead times and restricts trigger rates to a few hundred per second. The ion gate can be eliminated from the setup by the use of Gas Electron Multiplier (GEM) foils for gas amplification, which intrinsically suppress the backflow of ions. This makes the continuous operation of a TPC at high rates feasible. In this work, Monte Carlo simulations of the buildup of ion space charge in a GEM-based TPC and the correction of the resulting drift distortions are discussed, based on realistic numbers for the ion backflow in a triple-GEM amplification stack. A TPC in the future panda experiment at FAIR serves as an example for the experimental environment. The simulations show that space charge densities up to 65 fC cm i are reached, leading to electron drift distortions of up to 10 mm. The application of a laser calibration system to correct these distortions is investigated. Based on lull simulations of the detector physics and response, we show that it is possible to correct for the drift distortions and to maintain the good momentum resolution of the GEM-TPC.
AB - A fundamental limit to the application of Time Projection Chambers (TPCs) in high-rate experiments is the accumulation of slowly drifting ions in the active gas volume, which compromises the homogeneity of the drift field and hence the detector resolution. Conventionally, this problem is overcome by the use of ion-gating structures. This method, however, introduces large dead times and restricts trigger rates to a few hundred per second. The ion gate can be eliminated from the setup by the use of Gas Electron Multiplier (GEM) foils for gas amplification, which intrinsically suppress the backflow of ions. This makes the continuous operation of a TPC at high rates feasible. In this work, Monte Carlo simulations of the buildup of ion space charge in a GEM-based TPC and the correction of the resulting drift distortions are discussed, based on realistic numbers for the ion backflow in a triple-GEM amplification stack. A TPC in the future panda experiment at FAIR serves as an example for the experimental environment. The simulations show that space charge densities up to 65 fC cm i are reached, leading to electron drift distortions of up to 10 mm. The application of a laser calibration system to correct these distortions is investigated. Based on lull simulations of the detector physics and response, we show that it is possible to correct for the drift distortions and to maintain the good momentum resolution of the GEM-TPC.
KW - Drift distortions
KW - Gas electron multiplier
KW - Ion backflow
KW - Laser calibration
KW - Particle tracking
KW - Space charge
KW - Time projectionchamber
UR - http://www.scopus.com/inward/record.url?scp=84885448586&partnerID=8YFLogxK
U2 - 10.1016/j.nima.2013.04.020
DO - 10.1016/j.nima.2013.04.020
M3 - Article
AN - SCOPUS:84885448586
SN - 0168-9002
VL - 719
SP - 101
EP - 108
JO - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
JF - Nuclear Instruments and Methods in Physics Research, Section A: Accelerators, Spectrometers, Detectors and Associated Equipment
ER -