1984
DOI: 10.1016/0370-2693(84)90101-1
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Cosmological and experimental constraints on the tau neutrino

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Cited by 113 publications
(54 citation statements)
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“…One of the standard distortions, known as the Compton y-distortion, is created in the regime of inefficient energy transfer between electrons and photons, relevant at redshift z 5 × 10 4 . Processes creating this type of distortion include the inverse-Compton scattering of CMB photons off hot electrons during the epoch of reionization and structure formation Hu et al 1994b;Refregier & et al 2000;Hill et al 2015), also known in connection with the thermal Sunyaev-Zeldovich (tSZ) effect (Zeldovich & Sunyaev 1969), but can also be related to non-standard physics, e.g., the presence of long-lived decaying particles (Sarkar & Cooper 1984;Ellis et al 1992;Hu & Silk 1993b;Chluba 2013a).…”
Section: Introductionmentioning
confidence: 99%
“…One of the standard distortions, known as the Compton y-distortion, is created in the regime of inefficient energy transfer between electrons and photons, relevant at redshift z 5 × 10 4 . Processes creating this type of distortion include the inverse-Compton scattering of CMB photons off hot electrons during the epoch of reionization and structure formation Hu et al 1994b;Refregier & et al 2000;Hill et al 2015), also known in connection with the thermal Sunyaev-Zeldovich (tSZ) effect (Zeldovich & Sunyaev 1969), but can also be related to non-standard physics, e.g., the presence of long-lived decaying particles (Sarkar & Cooper 1984;Ellis et al 1992;Hu & Silk 1993b;Chluba 2013a).…”
Section: Introductionmentioning
confidence: 99%
“…We can now identify the temperature T m at which the particle energy density ρ x (≃ m x n x ) would † This assumes thermalization of the released energy which is very efficient for decay lifetimes < ∼ 10 5 sec (Illarianov andSunyaev 1975, Sarkar andCooper 1984). For longer lifetimes thermalization is incomplete, but then the absence of a spectral distortion in the CMBR sets equally restrictive constraints on the decaying particle abundance (e.g.…”
Section: Bounds On Non-relativistic Relicsmentioning
confidence: 99%
“…We emphasize that this bound is more general than the similar one (5.7) which only applies to Dirac neutrinos which decay 'invisibly' after nucleosynthesis. Sarkar and Cooper (1984) had argued that a ν τ lighter than 1 MeV has no decay modes which are fast enough to satisfy the constraint (5.8) from the energy density. The radiative decay ν τ → ν e γ is generally too slow and in any case is observationally required to have a lifetime greater than the age of the universe (see Sciama 1993).…”
Section: Neutrino Decaysmentioning
confidence: 99%
“…Commonly discussed spectral distortions are primarily due to energy release (Zeldovich & Sunyaev 1969;Sunyaev & Zeldovich 1970;Burigana et al 1991;Hu & Silk 1993a), for example, because of decaying relic particles (Sarkar & Cooper 1984;Kawasaki & Sato 1986;Hu & Silk 1993b; or the damping of primordial acoustic waves at small scales (Hu et al 1994a;Chluba et al 2012b,a), which causes µ-, y-and r-distortions. In the future, these signals may be detected with an experiment similar to PIXIE (Kogut et al 2011), a satellite concept which could provide a major leap forward in sensitivity over COBE/FIRAS (Fixsen et al 1996) and may open a new unexplored window to the early Universe.…”
Section: Introductionmentioning
confidence: 99%