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Ladek Zdroj, February 2008, Neutrino emission in nonsuperfluid matter The effects of superfluidity COOLING OF NEUTRON STARS D.G. Yakovlev Ioffe Physical Technical Institute, St.-Petersburg, Russia 1. Formulation of the Cooling Problem 2. Superlfuidity and Heat Capacity 3. Neutrino Emission 4. Cooling Theory versus Observations
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RICHNESS OF PHYSICAL CONDITIONS
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MAIN NEUTRINO EMISSION MECHANISMS IN NEUTRON STARS Main features: unobserved (but governs the cooling) complete transparency neutrino energies ~ kT massless but low-energy neutrinos
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NEUTRINO PROCESSES IN NEUTRON STAR CRUST
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TEMPERATURE AND DENSITY DEPENDENSE OF NEUTRINO EMISSION
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~ Direct Urca Process Lattimer, Pethick, Prakash, Haensel (1991) Threshold: In inner cores of massive stars Similar processes with muons Similar processes with hyperons, e.g. Is forbidden in outer core by momentum conservation:
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Gamow and Shoenberg: Casino da Urca in Rio de Janeiro Neutrino theory of stellar collapse, Phys. Rev. 59, 539, 1941: Unrecordable cooling agent Photo and Story by R. Ruffini Welcome to the Urca World - I
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Welcome to the Urca World - II
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ENCHANCED NEUTRINO EMISSION PROCESSES IN CORES OF MASSIVE NEUTRON STARS Prakash, Prakash, Lattimer, Pethick (1992) Maxwell et al. (1977) Brown et al. (1992) Iwamoto (1980, 1982) NUCLEON-HYPERON MATTER PION CONDENSATE KAON CONDENSATE QUARK MATTER
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SLOW NEUTRINO EMISSION PROCESSES EVERYWHERE IN NEUTRON STAR CORES MODIFIED URCA [N=n or p = nucleon-spectator] NUCLEON-NUCLEON BREMSSTRAHLUNG { LEPTON MODIFIED URCA, BREMS IN COULOMB COLLISIONS Bahcall and Wolf (1965), Friman and Maxwell (1979), Maxwell (1987), Yakovlev and Levenfish (1995) Friman and Maxwell (1979) Any neutrino flavor
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Enhanced emission in inner cores of massive neutron stars Everywhere in neutron star cores Neutrino Emission Processes in Neutron Star Cores ModelProcess N/H direct Urca Pion condensate Kaon condensate Quark matter Modified Urca Bremsstrahlung
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Nucleon Matter with Open Direct Urca Process
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FAST AND SLOW NEUTRINO COOLING SUN
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Direct Urca, N/H Neutrino Emission Processes in Neutron Star Cores Outer core Inner core Slow emission Fast emission } } } } } Pion condensate Kaon condensation Or quark matter Modified Urca NN bremsstrahlung Enhanced emission in inner cores of massive neutron stars: Everywhere in neutron star cores: STANDARD Fast erg cm -3 s -1
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MAIN PHYSICAL MODELS Problems: To discriminate between neutrino mechanisms To broaden transition from slow to fast neutrino emission
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SUPERFLUID SUPPRESSION OF NEUTRINO EMISSION A= 1 S 0 B= 3 P 2 (m=0) C= 3 P 2 (m=2)
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AN EXAMPLE OF SUPERFLUID REDUCTION OF NEUTRINO EMISSION Two models for proton superfluidity Neutrino emissivity profiles Superfluidity: Suppresses modified Urca process in the outer core Suppresses direct Urca just after its threshold (“broadens the threshold”)
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Cooper pairing neutrino emission Flowers, Ruderman and Sutherland (1976) Only the standard physics involved
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Distribution over the stellar core T=3x10 8 K 2x10 8 10 8 6x10 7 3x10 7
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Neutrino luminosity due to Cooper pairing Gusakov et al. (2004)
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Summary of neutrino emission properties Neutrino emission from neutron star cores is strongly regulated by (1)Temperature (2)Composition of the matter (3)Superfluidity These regulators may affect the emissivity in a non-trivial way (enhance or suppress) What is their effect? Next lecture
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REFERENCES U. Lombardo, H.-J. Schulze. Superfluidity in neutron star matter. In: Physics of Neutron Star Interiors, edited by D. Blaschke, N. Glendenning, A. Sedrakian, Berlin: Springer, 2001, p. 30. D.G. Yakovlev, K.P. Levenfish, Yu.A. Shibanov. Cooling of neutron stars and superfluidity in their cores. Physics – Uspekhi 42, 737, 1999. D.G. Yakovlev, A.D. Kaminker, O.Y. Gnedin, P. Haensel. Neutrino emission from neutron stars. Phys. Rep. 354, Nums. 1,2, 2001.
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