Boosting background suppression in the NEXT experiment through Richardson-Lucy deconvolution
Abstract
Next-generation neutrinoless double beta decay experiments aim for half-life sensitivities of ~ yr, requiring suppressing backgrounds to <1 count/tonne/yr. For this, any extra background rejection handle, beyond excellent energy resolution and the use of extremely radiopure materials, is of utmost importance. The NEXT experiment exploits differences in the spatial ionization patterns of double beta decay and single-electron events to discriminate signal from background. While the former display two Bragg peak dense ionization regions at the opposite ends of the track, the latter typically have only one such feature. Thus, comparing the energies at the track extremes provides an additional rejection tool. The unique combination of the topology-based background discrimination and excellent energy resolution (1% FWHM at the Q-value of the decay) is the distinguishing feature of NEXT. Previous studies demonstrated a topological background rejection factor of ~5 when reconstructing electron-positron pairs in the Tl 1.6 MeV double escape peak (with Compton events as background), recorded in the NEXT-White demonstrator at the Laboratorio Subterr\'aneo de Canfranc, with 72% signal efficiency. This was recently improved through the use of a deep convolutional neural network to yield a background rejection factor of ~10 with 65% signal efficiency. Here, we present a new reconstruction method, based on the Richardson-Lucy deconvolution algorithm, which allows reversing the blurring induced by electron diffusion and electroluminescence light production in the NEXT TPC. The new method yields highly refined 3D images of reconstructed events, and, as a result, significantly improves the topological background discrimination. When applied to real-data 1.6 MeV pairs, it leads to a background rejection factor of 27 at 57% signal efficiency.
Keywords
Cite
@article{arxiv.2102.11931,
title = {Boosting background suppression in the NEXT experiment through Richardson-Lucy deconvolution},
author = {A. Simón and Y. Ifergan and A. B. Redwine and R. Weiss-Babai and L. Arazi and C. Adams and H. Almazán and V. Álvarez and B. Aparicio and A. I. Aranburu and I. J. Arnquist and C. D. R Azevedo and K. Bailey and F. Ballester and J. M. Benlloch-Rodríguez and F. I. G. M. Borges and N. Byrnes and S. Cárcel and J. V. Carrión and S. Cebrián and E. Church and C. A. N. Conde and T. Contreras and F. P. Cossío and A. A. Denisenko and G. Díaz and J. Díaz and J. Escada and R. Esteve and R. Felkai and L. M. P. Fernandes and P. Ferrario and A. L. Ferreira and F. Foss and E. D. C. Freitas and Z. Freixa and J. Generowicz and A. Goldschmidt and J. J. Gómez-Cadenas and R. González and D. González-Díaz and S. Gosh and R. Guenette and R. M. Gutiérrez and J. Haefner and K. Hafidi and J. Hauptman and C. A. O. Henriques and J. A. Hernando Morata and P. Herrero and V. Herrero and J. Ho and B. J. P. Jones and M. Kekic and L. Labarga and A. Laing and P. Lebrun and N. López-March and M. Losada and R. D. P. Mano and J. Martín-Albo and A. Martínez and M. Martínez-Vara and G. Martínez-Lema and A. D. McDonald and Z. -E. Meziani and F. Monrabal and C. M. B. Monteiro and F. J. Mora and J. Muñoz Vidal and C. Newhouse and P. Novella and D. R. Nygren and E. Oblak and M. Odriozola-Gimeno and B. Palmeiro and A. Para and J. Pérez and M. Querol and J. Renner and L. Ripoll and I. Rivilla and Y. Rodríguez García and J. Rodríguez and C. Rogero and L. Rogers and B. Romeo and C. Romo-Luque and F. P. Santos and J. M. F. dos Santos and M. Sorel and C. Stanford and J. M. R. Teixeira and P. Thapa and J. F. Toledo and J. Torrent and A. Usón and J. F. C. A. Veloso and T. T. Vuong and R. Webb and J. T. White and K. Woodruff and N. Yahlali},
journal= {arXiv preprint arXiv:2102.11931},
year = {2021}
}
Comments
Submitted to JHEP