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Sterile neutrino searches with reactor antineutrinos using coherent neutrino-nucleus scattering experiments

S. P. Behera, D. K. Mishra, P. K. Netrakanti, R. Sehgal, Kirtikesh Kumar, R. Dey, and V. Jha
Phys. Rev. D 108, 113002 – Published 4 December 2023

Abstract

We present an analysis on the sensitivity to the active-sterile neutrino mixing with Germanium (Ge) and Silicon (Si) detectors in the context of the proposed coherent elastic neutrino-nucleus experiment in India. The study has been carried out with 3 (active)+1(sterile) neutrino oscillation model. It is observed that the measurements that can be carried out with the Ge detector exhibit better sensitivity to the active-sterile neutrino mixing as compared to the Si detector. Both detectors are able to exclude most of the anomaly regions observed by the GALLIUM experiment. The Ge detector with mass 10 kg, can observe the active-sterile neutrino oscillation at 95% confidence level, provided that sin22θ140.09 at Δm412=1.0eV2 for an exposure of 1-yr. At higher values of Δm412, a better sensitivity is obtained at a short baseline. It is also found that the threshold as well as resolution of the detectors play a crucial role on the measurements of active-sterile neutrino mixing parameters.

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  • Received 28 August 2023
  • Accepted 9 November 2023

DOI:https://doi.org/10.1103/PhysRevD.108.113002

Published by the American Physical Society under the terms of the Creative Commons Attribution 4.0 International license. Further distribution of this work must maintain attribution to the author(s) and the published article’s title, journal citation, and DOI. Funded by SCOAP3.

Published by the American Physical Society

Physics Subject Headings (PhySH)

Nuclear PhysicsParticles & Fields

Authors & Affiliations

S. P. Behera1,*, D. K. Mishra1, P. K. Netrakanti1, R. Sehgal1, Kirtikesh Kumar1, R. Dey1,2, and V. Jha1,2

  • 1Nuclear Physics Division, Bhabha Atomic Research Centre, Mumbai - 400085, India
  • 2Homi Bhabha National Institute, Anushakti Nagar, Mumbai - 400094, India

  • *shiba@barc.gov.in

Article Text

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Issue

Vol. 108, Iss. 11 — 1 December 2023

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Images

  • Figure 1
    Figure 1

    Schematic representation of experimental setup for CEνNS measurement. BP: boronated polyethylene, thickness: 10 cm, HDPE: high density polyethylene, thickness: 10 cm.

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  • Figure 2
    Figure 2

    Maximal recoil energy of Si and Ge nuclei as a function of energy of the reactor ν¯es.

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  • Figure 3
    Figure 3

    Differential event rate variation with maximal recoil energy using Si and Ge detectors.

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  • Figure 4
    Figure 4

    The comparison of ASN mixing sensitivity at 95% C.L. for the Ge and Si detectors placed at fixed distances of 4 m, 13 m, 25 m, and 30 m from the (a) U-Apsara, (b) DHRUVA, (c) PFBR, and (d) VVER reactors, respectively.

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  • Figure 5
    Figure 5

    The comparison of ASN mixing sensitivity at 95% C.L. for different detector mass of the (a) Si and (b) Ge detectors placed at distance of 4 m from the U-Apsara reactor.

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  • Figure 6
    Figure 6

    The comparison of ASN mixing sensitivity at 95% C.L. for different detector threshold for the (a) Si and (b) Ge detectors placed at 4 m from the U-Apsara reactor facility.

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  • Figure 7
    Figure 7

    The comparison of ASN mixing sensitivity at 95% C.L. for different resolution of Ge detector placed at 4 m from the U-Apsara reactor facility.

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  • Figure 8
    Figure 8

    The comparison of ASN mixing sensitivity at 95% C.L. of Ge detector in presence of background placed at 4 m from the U-Apsara reactor facility. The signal to background ratio is one considered here.

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