tau^- \to \pi^- \eta \nu_\tau$ decay induced by QED one-loop effects
The $\tau^- \to \pi^-\eta\nu_{\tau}$ decay is forbidden in the Standard Model in the limit of exact $G$-parity, it becomes a rare decay due to isospin symmetry breaking and it is very sensitive to the effects of effective scalar interactions. Since the parameters driving isospin breaking, $(m_d-m_u)...
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Main Authors | , , |
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Format | Journal Article |
Language | English |
Published |
15.08.2023
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Subjects | |
Online Access | Get full text |
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Summary: | The $\tau^- \to \pi^-\eta\nu_{\tau}$ decay is forbidden in the Standard Model
in the limit of exact $G$-parity, it becomes a rare decay due to isospin
symmetry breaking and it is very sensitive to the effects of effective scalar
interactions. Since the parameters driving isospin breaking,
$(m_d-m_u)/(m_s-\bar{m})$ and $\alpha$, are of the same order, one may expect
their $G$-parity breaking effects in this decay can be of similar magnitudes.
In this work, we evaluate the effects of isospin-breaking amplitudes originated
from a virtual photon at one-loop in a resonance dominance model to describe
photon-hadron interactions. We find that these effects can shift the leading SM
predictions based on the $u-d$ quark mass difference by roughly $12\%$, and
should be taken into consideration in a precision comparison of theory and
experiment in order to draw meaningful conclusions on New Physics. The effects
in the rate of the analogous $\tau^- \to \pi^-\eta'\nu_{\tau}$ decay can be
larger ($\sim$ $78\%$), under the approximations assumed in this model. |
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DOI: | 10.48550/arxiv.2308.08067 |