# Calibration of the charge and energy loss per unit length of the   MicroBooNE liquid argon time projection chamber using muons and protons

**Authors:** MicroBooNE collaboration: C. Adams, M. Alrashed, R. An, J. Anthony, J., Asaadi, A. Ashkenazi, S. Balasubramanian, B. Baller, C. Barnes, G. Barr, V., Basque, M. Bass, F. Bay, S. Berkman, A. Bhanderi, A. Bhat, M. Bishai, A., Blake, T. Bolton, L. Camilleri, D. Caratelli, I. Caro Terrazas, R. Carr, R., Castillo Fernandez, F. Cavanna, G. Cerati, Y. Chen, E. Church, D. Cianci,, E.O. Cohen, J.M. Conrad, M. Convery, L. Cooper-Troendle, J.I. Crespo-Anadon,, M. Del Tutto, D. Devitt, A. Diaz, L. Domine, K. Duffy, S. Dytman, B. Eberly,, A. Ereditato, L. Escudero Sanchez, J. Esquivel, J.J. Evans, R.S. Fitzpatrick,, B.T. Fleming, N. Foppiani, D. Franco, A.P. Furmanski, D. Garcia-Gamez, S., Gardiner, V. Genty, D. Goeldi, S. Gollapinni, O. Goodwin, E. Gramellini, P., Green, H. Greenlee, R. Grosso, L. Gu, W. Gu, R. Guenette, P. Guzowski, P., Hamilton, O. Hen, C. Hill, G.A. Horton-Smith, A. Hourlier, E.C. Huang, R., Itay, C. James, J. Jan de Vries, X. Ji, L. Jiang, J.H. Jo, R.A. Johnson, J., Joshi, Y.J. Jwa, G. Karagiorgi, W. Ketchum, B. Kirby, M. Kirby, T., Kobilarcik, I. Kreslo, I. Lepetic, Y. Li, A. Lister, B.R. Littlejohn, S., Lockwitz, D. Lorca, W.C. Louis, M. Luethi, B. Lundberg, X. Luo, A., Marchionni, S. Marcocci, C. Mariani, J. Marshall, J. Martin-Albo, D.A., Martinez Caicedo, K. Mason, A. Mastbaum, N. McConkey, V. Meddage, T. Mettler,, K. Miller, J. Mills, K. Mistry, T. Mohayai, A. Mogan, J. Moon, M. Mooney,, C.D. Moore, J. Mousseau, M. Murphy, R. Murrells, D. Naples, R.K. Neely, P., Nienaber, J. Nowak, O. Palamara, V. Pandey, V. Paolone, A. Papadopoulou, V., Papavassiliou, S.F. Pate, A. Paudel, Z. Pavlovic, E. Piasetzky, D. Porzio, S., Prince, G. Pulliam, X. Qian, J.L. Raaf, A. Rafique, L. Ren, L. Rochester,, H.E. Rogers, M. Ross-Lonergan, C. Rudolf von Rohr, B. Russell, G. Scanavini,, D.W. Schmitz, A. Schukraft, W. Seligman, M.H. Shaevitz, R. Sharankova, J., Sinclair, A. Smith, E.L. Snider, M. Soderberg, S. Soldner-Rembold, S.R., Soleti, P. Spentzouris, J. Spitz, M. Stancari, J. St. John, T. Strauss, K., Sutton, S. Sword-Fehlberg, A.M. Szelc, N. Tagg, W. Tang, K. Terao, R.T., Thornton, M. Toups, Y.-T. Tsai, S. Tufanli, T. Usher, W. Van De Pontseele,, R.G. Van de Water, B. Viren, M. Weber, H. Wei, D.A. Wickremasinghe, Z., Williams, S. Wolbers, T. Wongjirad, K. Woodruff, M. Wospakrik, W. Wu, T., Yang, G. Yarbrough, L.E. Yates, G.P. Zeller, J. Zennamo, C. Zhang

arXiv: 1907.11736 · 2020-04-07

## TL;DR

This paper presents a data-driven calibration method for the MicroBooNE liquid argon TPC, improving energy measurement accuracy and particle identification by correcting for various detector effects using cosmic-ray muons and stopping protons.

## Contribution

The paper introduces a novel calibration technique that accounts for multiple detector effects, enhancing energy scale precision and particle identification in liquid argon TPCs.

## Key findings

- Achieved 2% absolute energy scale uncertainty in data.
- Improved proton selection efficiency by 2%.
- Enhanced energy loss measurement accuracy for ionizing particles.

## Abstract

We describe a method used to calibrate the position- and time-dependent response of the MicroBooNE liquid argon time projection chamber anode wires to ionization particle energy loss. The method makes use of crossing cosmic-ray muons to partially correct anode wire signals for multiple effects as a function of time and position, including cross-connected TPC wires, space charge effects, electron attachment to impurities, diffusion, and recombination. The overall energy scale is then determined using fully-contained beam-induced muons originating and stopping in the active region of the detector. Using this method, we obtain an absolute energy scale uncertainty of 2\% in data. We use stopping protons to further refine the relation between the measured charge and the energy loss for highly-ionizing particles. This data-driven detector calibration improves both the measurement of total deposited energy and particle identification based on energy loss per unit length as a function of residual range. As an example, the proton selection efficiency is increased by 2\% after detector calibration.

## Full text

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## Figures

64 figures with captions in the complete paper: https://tomesphere.com/paper/1907.11736/full.md

## References

28 references — full list in the complete paper: https://tomesphere.com/paper/1907.11736/full.md

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Source: https://tomesphere.com/paper/1907.11736