Abstract

We investigate the radiative decay of the cosmic neutrino background and its impact on the spectrum of the cosmic microwave background (CMB) that is known to be a nearly perfect black body. We derive exact formulas for the decay of a heavier neutrino into a lighter neutrino and a photon, ${\ensuremath{\nu}}_{j}\ensuremath{\rightarrow}{\ensuremath{\nu}}_{i}+\ensuremath{\gamma}$, and of absorption as its inverse, ${\ensuremath{\nu}}_{i}+\ensuremath{\gamma}\ensuremath{\rightarrow}{\ensuremath{\nu}}_{j}$, by accounting for the precise form of the neutrino momentum distribution. Our calculations show that if the neutrinos are heavier than $\mathcal{O}(0.1)\text{ }\text{ }\mathrm{eV}$ the exact formulas give results that differ by $\ensuremath{\sim}50%$, compared with approximate ones where neutrinos are assumed to be at rest. We also find that spectral distortion due to absorption is more important for heavy neutrino masses (by a factor of $\ensuremath{\sim}10$ going from a neutrino mass of 0.01--0.1 eV). By analyzing the CMB spectral data measured with COBE-FIRAS, we obtain lower limits on the neutrino lifetime of ${\ensuremath{\tau}}_{12}\ensuremath{\gtrsim}4\ifmmode\times\else\texttimes\fi{}{10}^{21}\text{ }\text{ }\mathrm{s}$ (95% C.L.) for the smaller mass splitting and ${\ensuremath{\tau}}_{13}\ensuremath{\sim}{\ensuremath{\tau}}_{23}\ensuremath{\gtrsim}{10}^{19}\text{ }\text{ }\mathrm{s}$ for the larger mass splitting. These represent up to 1 order of magnitude improvement over previous CMB constraints. With future CMB experiments such as PIXIE, these limits will improve by roughly 4 orders of magnitude. This translates to a projected upper limit on the neutrino magnetic moment (for certain neutrino masses and decay modes) of ${\ensuremath{\mu}}_{\ensuremath{\nu}}<3\ifmmode\times\else\texttimes\fi{}{10}^{\ensuremath{-}11}\text{ }\text{ }{\ensuremath{\mu}}_{B}$, where ${\ensuremath{\mu}}_{B}$ is the Bohr magneton. Such constraints would make future precision CMB measurements competitive with lab-based constraints on neutrino magnetic moments.

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