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  • Open Access

Search for a light Z in the LμLτ scenario with the NA64-e experiment at CERN

Yu. M. Andreev et al. (NA64 collaboration)
Phys. Rev. D 106, 032015 – Published 25 August 2022

Abstract

The extension of Standard Model made by inclusion of additional U(1) gauge LμLτ symmetry can explain the difference between the measured and the predicted value of the muon magnetic moment and solve the tension in B meson decays. This model predicts the existence of a new, light Z vector boson, predominantly coupled to second and third generation leptons, whose interaction with electrons is due to a loop mechanism involving muons and taus. In this work, we present a rigorous evaluation of the upper limits in the Z parameter space, obtained from the analysis of the data collected by the NA64-e experiment at CERN SPS, that performed a search for light dark matter with 2.84×1011 electrons impinging with 100 GeV on an active thick target. The resulting limits touch the muon g2 preferred band for values of the Z mass of order of 1 MeV, while the sensitivity projections for the future high-statistics NA64-e runs demonstrate the power of the electrons/positron beam approach in this theoretical scenario.

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  • Received 10 June 2022
  • Accepted 2 August 2022
  • Corrected 19 January 2023

DOI:https://doi.org/10.1103/PhysRevD.106.032015

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)

Particles & Fields

Corrections

19 January 2023

Correction: The surname of the 48th author contained an error and has been fixed.

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Vol. 106, Iss. 3 — 1 August 2022

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Images

  • Figure 1
    Figure 1

    The loop diagram inducing a kinetic mixing between the Z and the photon.

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  • Figure 2
    Figure 2

    The real and imaginary part of the function Π(q2). For illustration purposes, the arbitrary coupling choice gZ=2π2/e was made.

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  • Figure 3
    Figure 3

    The three main Z production processes for an electron/positron beam impinging on a fixed target: (a) radiative Z production; (b) nonresonant e+e annihilation; (c) resonant Z production in e+e annihilation.

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  • Figure 4
    Figure 4

    Schematic view of the NA64-e detector in the nominal, invisible mode configuration. See text for further details.

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  • Figure 5
    Figure 5

    The electrons and positrons differential track length in the NA64-e ECAL as a function of the energy. For positrons, the two distributions for lead and plastic scintillator are almost identical.

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  • Figure 6
    Figure 6

    The “downstream” NA64-e signal detection efficiency ηdown as a function of the emitted Z energy EF, for different models and corresponding parameters.

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  • Figure 7
    Figure 7

    The NA64-e exclusion limit for the LμLτ model, for the “vanilla” (left) and “dark” (right) flavor (red curve). The red (orange) dashed curves represent the sensitivity projections for a future high-statistics NA64-e run with an electron (positron) beam, for a total accumulated charge of 1013 EOT, while the green dashed curve is the sensitivity projection of NA64-μ [42]. The gray areas are the regions excluded by phenomenological reanalysis of neutrino experiments [34, 35], while the blue region is the area excluded by BABAR [28] for the vanilla case. Finally, the black curves represent the so-called “thermal target” for the two values of αD=0.1 and αD=0.02, i.e., the preferred combination of the parameters to explain the observed dark matter relic density. These have been calculated through Eq. (5) by rescaling the results from Ref. [25].

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  • Figure 8
    Figure 8

    The real part of the Π(q2) function, comparing the numerical result obtained from Eq. (6) with the numerical parameterization FR adopted in this work. For illustration purposes, the arbitrary coupling choice gZ=2π2/e was made.

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