F. V. Böhmer, M. Ball, S. Dørheim, C. Höppner, B. Ketzer, I. Konorov, S. Neubert, S. Paul, J. Rauch, M. Vandenbroucke
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, in which antiproton-proton interaction rates up to 2 x 10^7 per second will be reached, serves as an example for the experimental environment. The simulations show that space charge densities up to 65 fC per cubic cm 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 full 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.
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http://arxiv.org/abs/1209.0482
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