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arXiv:hep-ph/0206083·v1·High Energy Physics — Phenomenology

Dirac Neutrino Anapole Moment

L. G. Cabral-Rosetti🇲🇽 · M. Moreno🇲🇽 · A. Rosado🇲🇽

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Abstract

We calculate the Dirac neutrino anapole moment (a_{\nu_l}) in the context of the Standard Model (SM) making use of the Dirac form factor F_D(q^2) introduced recently by J. Bernabeu, L. G. Cabral-Rosetti, J. Papavassiliou y J. Vidal by using the Pinch Technique (PT) formalism, working in two different gauge-fixing schemes (R_\xi guage and the electroweak BFM), at the one loop level. We show that the neutrino anapole form factor F_A(q^2) and Dirac form factor F_D(q^2) are related as follows: F_A(q^2) = \frac{1}{q^2} F_D(q^2). Hence, the Dirac neutrino charge radius < r^2_{\nu_l} > and the anapole moment satisfy the simple relation a_{\nu_l} = {1/6} < r^2_{\nu_l} >. Therefore, we show that the anapole moment (as the charge radius) of the neutrino is a physical quantity, which only gets contribution from the proper neutrino electromagnetic vertex (in electroweak BFM), and that a_{\nu_l} is of the order 10^{-34} cm^2.

Comments: LaTex AIP style, 5 pages including 1 figure. Final version to appear in Proceedings of the VIII Mexican Workshop on Particles and Fields of the Division de Particulas y Campos de la Sociedad Mexicana de Fisica (DPyC-SMF), Cd. de Zacatecas, Zacatecas, Mexico November 14-20, 2001

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