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Main Authors: Flores-Orea, Y., Toscano, J. J.
Format: Preprint
Published: 2025
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Online Access:https://arxiv.org/abs/2508.09400
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author Flores-Orea, Y.
Toscano, J. J.
author_facet Flores-Orea, Y.
Toscano, J. J.
contents CPT-odd effects on the neutrino charge radius are studied within the Standard Model Extension. We consider CPT violation from the electroweak Yang-Mills sector, characterized by Lorentz-violating coefficients $(k_1)_μ$ and $(k_2)_μ$, which have positive mass units. The $\barννγ$ vertex arises at tree level via exchange of two $Z$ bosons. Although suppressed by $\frac{1}{m_Z^4}$, this process is notable. The vertex function $Γ_μ$ includes three independent gauge structures satisfying the Ward identity $q^μΓ_μ= 0$, characteristic of neutral particles, and induces gauge-independent electromagnetic form factors. Besides charge and anapole, two novel form factors appear. The charge form factor $f_Q(q^2)$ contains an energy-dependent term causing $f_Q(0)\neq 0$, so electromagnetic properties are undefined for real photons with CPT violation. Instead, $f_Q$ and the charge radius are defined in the static limit: $q^0=0$ and $\mathbf{q}\to 0$. Here, $f_Q(0, \mathbf{0})=0$ and a correction to the SM neutrino charge radius is found: \[ \langle r^2_ν\rangle_{CPTV} = \frac{3c_{2W}}{2c_W^4} \left[\frac{k_2^2}{m_Z^2} + \frac{\mathbf{k}_2^2}{m_Z^2}\cos^2θ_γ\right] \frac{1}{m_Z^2}, \] with $θ_γ$ the angle between $\mathbf{q}$ and $\mathbf{k}_2$. Using recent bounds on $(k_i)_μ$ and reasonable assumptions, we obtain a small correction $\langle r^2_ν\rangle_{CPTV} \leq 0.83 \times 10^{-51}\ \mathrm{cm}^2$.
format Preprint
id arxiv_https___arxiv_org_abs_2508_09400
institution arXiv
publishDate 2025
record_format arxiv
spellingShingle Effects of CPT violation on the neutrino charge radius in the Standard Model Extension
Flores-Orea, Y.
Toscano, J. J.
High Energy Physics - Phenomenology
CPT-odd effects on the neutrino charge radius are studied within the Standard Model Extension. We consider CPT violation from the electroweak Yang-Mills sector, characterized by Lorentz-violating coefficients $(k_1)_μ$ and $(k_2)_μ$, which have positive mass units. The $\barννγ$ vertex arises at tree level via exchange of two $Z$ bosons. Although suppressed by $\frac{1}{m_Z^4}$, this process is notable. The vertex function $Γ_μ$ includes three independent gauge structures satisfying the Ward identity $q^μΓ_μ= 0$, characteristic of neutral particles, and induces gauge-independent electromagnetic form factors. Besides charge and anapole, two novel form factors appear. The charge form factor $f_Q(q^2)$ contains an energy-dependent term causing $f_Q(0)\neq 0$, so electromagnetic properties are undefined for real photons with CPT violation. Instead, $f_Q$ and the charge radius are defined in the static limit: $q^0=0$ and $\mathbf{q}\to 0$. Here, $f_Q(0, \mathbf{0})=0$ and a correction to the SM neutrino charge radius is found: \[ \langle r^2_ν\rangle_{CPTV} = \frac{3c_{2W}}{2c_W^4} \left[\frac{k_2^2}{m_Z^2} + \frac{\mathbf{k}_2^2}{m_Z^2}\cos^2θ_γ\right] \frac{1}{m_Z^2}, \] with $θ_γ$ the angle between $\mathbf{q}$ and $\mathbf{k}_2$. Using recent bounds on $(k_i)_μ$ and reasonable assumptions, we obtain a small correction $\langle r^2_ν\rangle_{CPTV} \leq 0.83 \times 10^{-51}\ \mathrm{cm}^2$.
title Effects of CPT violation on the neutrino charge radius in the Standard Model Extension
topic High Energy Physics - Phenomenology
url https://arxiv.org/abs/2508.09400