Simulation and tracking algorithm of an Active Target Time Projection Chamber (AT-TPC)

ORAL

Abstract

The AT-TPC is a new detector being made for studying low-energy reactions induced by secondary beams with high resolution and efficiency. In order to define the construction details, a robust tracking algorithm is needed. First, reaction tracks must be simulated realisticly, obtaining all kinematic observables. Our choice of micromegas as gas-amplifier implies a nonlinear response of the pad-signal with respect to position. A simulation was developed to perform the track reconstruction based on modeling the ionization track and the corresponding drift electrons through the AT-TPC. It takes into account the energy loss of ions in the gas target, the drift of the electrons, the detector's magnetic field, the electron amplification, and the response of the electronics. All the associated fluctuations are taken into account. To extract the physical variables Monte-Carlo simulation tracks are produced and then compared to track signals using a $\chi^2$ minimization to obtain the best parameters for the track. The program was used to test different pad patterns for the micromegas electron amplification detector in order to find the optimum pad layout for the construction of the detector. The code was also used to analyse tracks produced by alpha particles from a source in a test-device

Authors

  • Saul Beceiro

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Wolfgang Mittig

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Tan Ahn

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Daniel Bazin

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University), NSCL

  • Remi Becquet

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Zbigniew Chajecki

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Adam Fritsch

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • W.G. Lynch

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University), Michigan State University

  • Aimee Shore

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)

  • Malek Tahar

    NSCL, Michigan State University, National Superconducting Cyclotron Laboratory (Michigan State University)