Prepared for submission to JINST Ionization Electron Signal Processing in Single Phase LArTPCs I. Algorithm Description and Quantitative Evaluation with MicroBooNE Simulation

We describe the concept and procedure of drifted-charge extraction developed in the MicroBooNE experiment, a single-phase liquid argon time projection chamber (LArTPC). This technique converts the raw digitized TPC waveform to the number of ionization electrons passing through a wire plane at a given time. A robust recovery of the number of ionization electrons from both induction and collection anode wire planes will augment the 3D reconstruction, and is particularly important for tomographic reconstruction algorithms. A number of building blocks of the overall procedure are described. The performance of the signal processing is quantitatively evaluated by comparing extracted charge with the true charge through a detailed TPC detector simulation taking into account position-dependent induced current inside a single wire region and across multiple wires. Some areas for further improvement of the performance of the charge extraction procedure are also discussed.

[1]  M. Wojcik,et al.  Electron recombination in ionized liquid argon: a computational approach based on realistic models of electron transport and reactions. , 2011, The journal of physical chemistry. A.

[2]  B. Jones,et al.  The photomultiplier tube calibration system of the MicroBooNE experiment , 2015, 1502.04159.

[3]  A. Dell'Acqua,et al.  Geant4 - A simulation toolkit , 2003 .

[4]  D. R. Nygren,et al.  The Time Projection Chamber: A New 4 pi Detector for Charged Particles , 1976 .

[5]  B. C. Barish,et al.  A Neutrino detector sensitive to rare processes. I. A Study of neutrino electron reactions , 1976 .

[6]  Carlos Alberto Brebbia The birth of the boundary element method from conception to application , 2017 .

[7]  Bo Yu,et al.  Cold electronics for "Giant" Liquid Argon Time Projection Chambers , 2011 .

[8]  R. Hatcher,et al.  The NuMI Neutrino Beam , 2015, 1507.06690.

[9]  Simon R. Arridge,et al.  Solving Boundary Integral Problems with BEM++ , 2015, ACM Trans. Math. Softw..

[10]  H. Nyquist Thermal Agitation of Electric Charge in Conductors , 1928 .

[11]  J. Harvey,et al.  DESIGN OF GRID IONIZATION CHAMBERS , 1949 .

[12]  J. Warman,et al.  Hot-electron thermalization in solid and liquid argon, krypton, and xenon , 1982 .

[13]  C. D. Moore,et al.  The Pandora multi-algorithm approach to automated pattern recognition of cosmic-ray muon and neutrino events in the MicroBooNE detector , 2017, The European Physical Journal C.

[14]  C. Bromberg,et al.  A study of electron recombination using highly ionizing particles in the ArgoNeuT Liquid Argon TPC , 2013, 1306.1712.

[15]  S. Ramo Currents Induced by Electron Motion , 1939, Proceedings of the IRE.

[16]  Veljko Radeka,et al.  Front-End ASIC for a Liquid Argon TPC , 2011, IEEE Transactions on Nuclear Science.

[17]  V. Svelto,et al.  Extension of Ramo's theorem as applied to induced charge in semiconductor detectors☆ , 1971 .

[18]  L. Hamel,et al.  Generalized demonstration of Ramo's theorem with space charge and polarization effects , 2008 .

[19]  D. A. Wickremasinghe,et al.  Noise Characterization and Filtering in the MicroBooNE Liquid Argon TPC , 2017, 1705.07341.

[20]  C. D. Moore,et al.  Neutrino flux prediction at MiniBooNE , 2008, 0806.1449.

[21]  A. Pullia,et al.  Time-domain Simulation of electronic noises , 2004, IEEE Transactions on Nuclear Science.

[22]  D. A. Wickremasinghe,et al.  Measurement of cosmic-ray reconstruction efficiencies in the MicroBooNE LArTPC using a small external cosmic-ray counter , 2017, 1707.09903.

[23]  Sue Birchmore,et al.  Garfield , 2007, Journal of General Internal Medicine.

[24]  S. Gollapinni,et al.  Construction and assembly of the wire planes for the MicroBooNE Time Projection Chamber , 2016, 1609.06169.

[25]  C. Rubbia The Liquid Argon Time Projection Chamber: A New Concept for Neutrino Detectors , 1977 .

[26]  B. Baller Liquid Argon TPC Signal Formation, Signal Processing and Hit Reconstruction , 2017 .

[27]  Philip D. Plowright Extrapolation , 2019, Making Architecture Through Being Human.

[28]  C. D. Moore,et al.  Determination of muon momentum in the MicroBooNE LArTPC using an improved model of multiple Coulomb scattering , 2017, 1703.06187.

[29]  W. Tang,et al.  Data Unfolding with Wiener-SVD Method , 2017, 1705.03568.

[30]  Rayleigh The Problem of the Random Walk , 1905, Nature.

[31]  Veljko Radeka,et al.  Liquid-argon ionization chambers as total-absorption detectors , 1974 .

[32]  S. Kubota,et al.  Estimation of Fano factors in liquid argon, krypton, xenon and xenon-doped liquid argon , 1976 .