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1.
Phys Rev Lett ; 111(23): 231301, 2013 Dec 06.
Article in English | MEDLINE | ID: mdl-24476250

ABSTRACT

The red-giant branch (RGB) in globular clusters is extended to larger brightness if the degenerate helium core loses too much energy in "dark channels." Based on a large set of archival observations, we provide high-precision photometry for the Galactic globular cluster M5 (NGC 5904), allowing for a detailed comparison between the observed tip of the RGB with predictions based on contemporary stellar evolution theory. In particular, we derive 95% confidence limits of g(ae)<4.3×10(-13) on the axion-electron coupling and µ(ν)<4.5×10(-12)µ(B) (Bohr magneton µ(B)=e/2m(e)) on a neutrino dipole moment, based on a detailed analysis of statistical and systematic uncertainties. The cluster distance is the single largest source of uncertainty and can be improved in the future.

2.
Phys Rev Lett ; 104(25): 251101, 2010 Jun 25.
Article in English | MEDLINE | ID: mdl-20867357

ABSTRACT

An 8.8M{⊙} electron-capture supernova was simulated in spherical symmetry consistently from collapse through explosion to essentially complete deleptonization of the forming neutron star. The evolution time (∼9 s) is short because high-density effects suppress our neutrino opacities. After a short phase of accretion-enhanced luminosities (∼200 ms), luminosity equipartition among all species becomes almost perfect and the spectra of ν{e} and ν{µ,τ} very similar, ruling out the neutrino-driven wind as r-process site. We also discuss consequences for neutrino flavor oscillations.

3.
Phys Rev Lett ; 87(5): 051301, 2001 Jul 30.
Article in English | MEDLINE | ID: mdl-11497757

ABSTRACT

If large extra dimensions exist in nature, supernova (SN) cores will emit large fluxes of Kaluza-Klein gravitons, producing a cosmic background of these particles with energies and masses up to about 100 MeV. Radiative decays then give rise to a diffuse cosmic gamma-ray background with E(gamma) approximately less than 100 MeV which is well in excess of the observations if more than 0.5%-1% of the SN energy is emitted into the new channel. For two extra dimensions we derive a conservative bound on their radius of R approximately less than 0.9 x 10(-4) mm; for three extra dimensions it is R approximately less than 1.9 x 10(-7) mm.

5.
Phys Rev D Part Fields ; 54(1): 1194-1203, 1996 Jul 01.
Article in English | MEDLINE | ID: mdl-10020587
6.
Phys Rev Lett ; 76(15): 2621-2624, 1996 Apr 08.
Article in English | MEDLINE | ID: mdl-10060747
7.
Phys Rev D Part Fields ; 52(4): 1780-1799, 1995 Aug 15.
Article in English | MEDLINE | ID: mdl-10019405
8.
Phys Rev D Part Fields ; 51(12): 6635-6646, 1995 Jun 15.
Article in English | MEDLINE | ID: mdl-10018427
9.
Phys Rev D Part Fields ; 51(4): 1495-1498, 1995 Feb 15.
Article in English | MEDLINE | ID: mdl-10018616
10.
Phys Rev D Part Fields ; 50(12): 7729-7730, 1994 Dec 15.
Article in English | MEDLINE | ID: mdl-10017756
11.
Phys Rev Lett ; 70(16): 2363-2366, 1993 Apr 19.
Article in English | MEDLINE | ID: mdl-10053543
12.
Phys Rev Lett ; 68(20): 3116, 1992 May 18.
Article in English | MEDLINE | ID: mdl-10045617
13.
Phys Rev D Part Fields ; 45(5): 1782-1788, 1992 Mar 01.
Article in English | MEDLINE | ID: mdl-10014551
15.
Phys Rev D Part Fields ; 38(12): 3811-3812, 1988 Dec 15.
Article in English | MEDLINE | ID: mdl-9959146
16.
Phys Rev Lett ; 60(18): 1793-1796, 1988 May 02.
Article in English | MEDLINE | ID: mdl-10038142
17.
Phys Rev D Part Fields ; 37(5): 1237-1249, 1988 Mar 01.
Article in English | MEDLINE | ID: mdl-9958803
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