Abstract

One of the substantial sources of systematic errors in neutrino oscillation experiments that utilize neutrinos from accelerator sources stems from a lack of precision in modeling single-pion production (SPP). Oscillation analyses rely on Monte Carlo event generators (MC), providing theoretical predictions of neutrino interactions on nuclear targets. Pions produced in these processes provide a significant fraction of oscillation signal and background on both elementary scattering and detector simulation levels. Thus, it is of critical importance to develop techniques that will allow us to accommodate state-of-the-art theoretical models describing SPP into MCs. In this work, we investigate various algorithms to implement single-pion production models in Monte Carlo event generators. Based on comparison studies, we propose a novel implementation strategy that combines satisfactory efficiency with high precision in reproducing details of theoretical models predictions, including pion angular distributions. The proposed implementation is model-independent, thereby providing a framework that can include any model for SPP. We have tested the new algorithm with the Ghent Low Energy Model for single-pion production implemented in the NuWro Monte Carlo event generator.

Highlights

  • Single-pion production (SPP) is one of the main reaction channels relevant for accelerator-based neutrino experiments, where neutrino energies range from a couple of hundred MeVs up to several GeVs [1]

  • We have tested the new algorithm with the Ghent low energy model for single-pion production implemented in the NuWro Monte Carlo event generator

  • To reliably test the performance of the abovementioned sampling algorithms, we performed simulations using the Ghent low energy model (LEM) of single-pion production implemented in the NuWro Monte Carlo event generator

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Summary

INTRODUCTION

Single-pion production (SPP) is one of the main reaction channels relevant for accelerator-based neutrino experiments, where neutrino energies range from a couple of hundred MeVs up to several GeVs [1]. SPP contributes to the commonly used CC0π experimental topology [7], provided that the pions get reabsorbed in the nuclear medium or remain otherwise undetected This interaction channel is itself a part of the signal for oscillation experiments especially with higher-energy neutrino beams such as NOvA [8] and DUNE [9], and for T2K [10]. It is seemingly an intractable problem to provide a detailed microscopic description of FSI over the sizable phase space of these experiments For this reason, the FSI are usually treated in an approximate way using intranuclear cascade models [22,23,24] implemented in various Monte Carlo neutrino event generators (MC).

KINEMATICS AND CROSS SECTION
MONTE CARLO EVENT GENERATION FOR SINGLE-PION PRODUCTION
Numerical tools
Ghent low energy model of SPP
NuWro Monte Carlo event generator
Performance
Inclusive cross section
Angular distributions of the pion
CONCLUSIONS
Full Text
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