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Stars as Laboratories for Fundamental Physics - MPP Theory Group

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442 Chapter 11<br />

linear equations of motion <strong>for</strong> the neutrino density matrix which causes<br />

an “off-diagonal refractive index” <strong>as</strong> discussed in Sect. 9.3.2. Qian and<br />

Fuller (1995) have per<strong>for</strong>med an approximately self-consistent analysis<br />

of this problem. All told, they found that the neutrino-neutrino interactions<br />

have a relatively small impact on the parameter space where flavor<br />

conversion disturbs the r-process. Within the overall precision of these<br />

arguments and calculations, their final exclusion plot is nearly identical<br />

with the schematic picture shown in Fig. 11.21. Qian and Fuller’s<br />

findings are corroborated by a study per<strong>for</strong>med by Sigl (1995a).<br />

c) Summary<br />

In summary, there remains a large range of mixing angles where neutrino<br />

oscillations between ν e and ν µ or ν τ with a cosmologically interesting<br />

m<strong>as</strong>s could help to explode supernovae, and yet not disturb<br />

r-process nucleosynthesis. If one <strong>as</strong>sumes a m<strong>as</strong>s hierarchy with ν e<br />

dominated by the lightest, ν τ by the heaviest m<strong>as</strong>s eigenstate, the cosmologically<br />

relevant neutrino would be identified with ν τ . It is interesting<br />

that the relevant range of mixing angles, 3×10 −4 < ∼ θ < ∼ 3×10 −3 ,<br />

overlaps with the mixing angle among the first and third family quarks<br />

which is in the range 0.002−0.005 (Eq. 7.6). There<strong>for</strong>e, a scenario<br />

where a m<strong>as</strong>sive ν τ plays a cosmologically important role, helps to explode<br />

supernovae, and leaves r-process nucleosynthesis unscathed does<br />

not appear to be entirely far-fetched. This scenario leaves the possibility<br />

open that the MSW effect solves the solar neutrino problem by<br />

ν e -ν µ oscillations.<br />

11.4.6 A Caveat<br />

All existing discussions of neutrino flavor oscillations in SNe were b<strong>as</strong>ed<br />

on spherically symmetric, smooth density profiles. However, there<br />

can be significant density variations, convection, turbulence, and so<br />

<strong>for</strong>th. There<strong>for</strong>e, it is clear that many of my statements about mediuminduced<br />

oscillation effects are provisional. Further studies will be required<br />

to develop a more complete picture of SNe and their neutrino<br />

oscillations <strong>as</strong> 3-dimensional events.<br />

A first study of SN neutrino oscillations with an inhomogeneous density<br />

profile w<strong>as</strong> recently per<strong>for</strong>med by Loreti et al. (1995). They added<br />

a random density field to the standard smooth profile and studied the<br />

impact on neutrino oscillations. They found that the shock-revival scenario<br />

involving MSW oscillations can be significantly affected in the

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