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Dejan Urošević Department of Astronomy, Faculty of Mathematics, University of Belgrade Supernova remnants: evolution, statistics, spectra
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Hydrodynamic Evolution of SNRs First phase – free expansion phase (M s < M e ), till 3/4E k → U (M s 3M e ), (for 1/2E k → U, M s M e ). Second phase – adiabatic phase (M s >> M e ) till 1/2E k → radiation Third phase – isothermal phase – formation of thick shell Forth phase – dissipation into ISM
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Radio Brightness Evolution in the Adiabatic Phase synchrotron emissivity K H 1+ - , where K from N(E)=KE 1+2 and spectral index from S - surface brightness = S / = V shell / D 2 2, where D is SNR diameter
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magnetic field H = f 1 (D) and K = f 2 (D); both functions are power low functions surface brightness becomes: D fk( ) D fH( ) V shell / D 2 = AD - finally we obtain so-called - D relation: = AD - , where =-(fk( ) +fH( )+1) and A=const.
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Trivial Theoretical - D Relation if the luminosity is constant (or independent on D) during SNR expansion we have: D -2 this is trivial form of the theoretical - D relation
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Short History of the Theoretical - D relation Shklovsky (1960) - spherical model with: H D -2 =0.5 D -6 Lequeux (1962) - shell model with: H D -2 =0.5 D -5.8
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Poveda & Woltjer (1968) - using van der Laan (1962) model with: H = const., =0.5 D -3 Kesteven (1968) - shell of constant thickness: H D -1, =0.5 D -4.5
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Duric & Seaquist (1986) - for H D -2 =0.5 D -3.5 (D>>1pc), D -5 (D >1pc) Berezhko & Volk (2004) D -4.25 (time-dependent nonlinear kinetic theory)
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STATISTICS OF SNRs
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Empirical -D Relation Necessary for determination of distances to Galactic SNRs identified only in radio continuum Necessary for confirmation of the theory in order to define valid evolutionary tracks
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Empirical -D Relations (Related Problems) Critical analyses: Green (1984, 1991, 2004) Galactic sample - distances determination problem - Malmquist Bias - volume selection effect - other selection effects (sensitivity, resolution, confusion)
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Extragalactic samples - sensitivity (surface brightness ( ) limits) - resolution (angular-size ( ) limits) - confusion
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Updated Empirical - D Relations Galactic relation (Milky Way (MW) 36 SNRs) D -2.4 (Case & Bhattacharya 1998)
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Extragalactic sample (11 galaxies) LMC, SMC, M31, M33, IC1613, NGC300, NGC6946, NGC7793, M82, NGC1569, NGC2146 (148 SNRs) - Monte Carlo simulations suggest that the effect of survey sensitivity tending to flatten the slopes toward the trivial relation (opposite to effect of Malmquist bias) (Urošević et al. 2005)
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-the only one valid empirical -D relation is constructed for M82 (21 SNRs): D -3.4, the validity was checked by Monte Carlo simulations and by L-D (luminosity- diameter) dependences (Urošević et al. 2005, Arbutina et al. 2004) - also, this relation is appropriate for determination of distances to SNRs (Arbutina et al. 2004)
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Synchrotron spectra
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Thermal Emission from SNRs Thermal Bremsstrahlung N 2 T -1/2, where N is particle concentration and T is temperature
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There are two rare types of SNRs with strong thermal emission (Urošević and Pannuti 2005)
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the first type – the relatively young SNRs in the adiabatic phase of evolution that evolve in the dense molecular cloud (MC) – D 20 pc, 1GHz ~ 10 -20 (SI) – for N 300 cm -3 and T ~ 10 6 K 1GHz, therm. 1GHz, synch.
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the second type – the extremely evolved SNRs in the late adiabatic phase expanded in denser warm medium – D 200 pc, 1GHz ~ 10 -22 (SI) – for N 1 - 10 cm -3 and T ~ 10 4 K 1GHz, therm. (0.1 - 10) 1GHz, synch.
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HB3 Urošević et al. 2007
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HB3 – observational data S 1GHz = 50 Jy D= 70 pc (for distance of 2 kpc) Shell thickness = 0.05 D ↓ ↓ ↓ Emissivity 1GHz =1.67 x 10 -37 (ergs sec -1 cm -3 Hz -1 )
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HB3 - density of environment We recall (cgs)= 7x10 -38 N 2 T -1/2 if we suppose 10 4 < T < 10 6 K ↓ ↓ ↓ 10 < n e < 35 cm -3
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SUMMARY Some updated results related to: - evolution - statistic - spectra of SNRs are given.
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THANK YOU VERY MUCH ON YOUR PATIENT!!!
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