SUPERNOVA NEUTRINO OPACITY FROM NUCLEON-NUCLEON BREMSSTRAHLUNG AND RELATED PROCESSES

Elastic scattering on nucleons, νN → Nν, is the dominant supernova (SN) opacity source for μ and τ neutrinos. The dominant energy- and number-changing processes were thought to be νe- → e-ν and ν↔e+e− until Suzuki showed that the bremsstrahlung process νNN↔NN was actually more important. We find that for energy exchange, the related "inelastic scattering process" νNN↔NNν is even more effective by about a factor of 10. A simple estimate implies that the νμ and ντ spectra emitted during the Kelvin-Helmholtz cooling phase are much closer to that of e than had been thought previously. To facilitate a numerical study of the spectra formation we derive a scattering kernel that governs both bremsstrahlung and inelastic scattering and give an analytic approximation formula. We consider only neutron-neutron interactions; we use a one-pion exchange potential in Born approximation, nonrelativistic neutrons, and the long-wavelength limit, simplifications that appear justified for the surface layers of an SN core. We include the pion mass in the potential, and we allow for an arbitrary degree of neutron degeneracy. Our treatment does not include the neutron-proton process and does not include nucleon-nucleon correlations. Our perturbative approach applies only to the SN surface layers, i.e., to densities below about 1014 g cm-3.

[1]  J. Mathiot,et al.  Axion emission from SN1987A. Nuclear physics constraints , 1989 .

[2]  G. Raffelt,et al.  Reduction of weak interaction rates in neutron stars by nucleon spin fluctuations: Degenerate case , 1996, astro-ph/9610193.

[3]  M. Prakash,et al.  Neutrino Scattering in a Newly Born Neutron Star , 1996, astro-ph/9610115.

[4]  B. Friman,et al.  Neutrino emissivities of neutron stars. , 1979 .

[5]  D. Tubbs Conservative scattering, electron scattering, and neutrino thermalization. , 1979 .

[6]  Keikichi G. Nakamura,et al.  Frontiers of neutrino astrophysics , 1993 .

[7]  Turner,et al.  Axions, SN 1987A, and one-pion exchange. , 1988, Physical review. D, Particles and fields.

[8]  D. Bugg Pions and nuclei , 1981, Nature.

[9]  G. Raffelt Stars as laboratories for fundamental physics , 1996 .

[10]  Saul A. Teukolsky,et al.  Black Holes , 1998 .

[11]  V. Weisskopf,et al.  Theoretical Nuclear Physics , 1953 .

[12]  Janka,et al.  Nucleon spin fluctuations and the supernova emission of neutrinos and axions. , 1996, Physical review letters.

[13]  Dieter Forster,et al.  Hydrodynamic fluctuations, broken symmetry, and correlation functions , 1975 .

[14]  Raffelt,et al.  Supernova neutrino scattering rates reduced by nucleon spin fluctuations: Perturbative limit. , 1996, Physical review. D, Particles and fields.

[15]  Saul A. Teukolsky,et al.  Black Holes, White Dwarfs, and Neutron Stars , 1983 .

[16]  A. Burrows,et al.  Postshock neutrino transport and electron capture in stellar collapse , 1982 .

[17]  H. Janka,et al.  Ledoux Convection in Protoneutron Stars—A Clue to Supernova Nucleosynthesis? , 1996, astro-ph/9610203.

[18]  Kim,et al.  Invisible-axion emissions from SN 1987A. , 1989, Physical review letters.

[19]  A. Burrows,et al.  Signatures of stellar collapse in electron-type neutrinos , 1983, Nature.