2014MNRAS.442..713M


Query : 2014MNRAS.442..713M

2014MNRAS.442..713M - Mon. Not. R. Astron. Soc., 442, 713-731 (2014/July-3)

Shocks in nova outflows - I. Thermal emission.

METZGER B.D., HASCOET R., VURM I., BELOBORODOV A.M., CHOMIUK L., SOKOLOSKI J.L. and NELSON T.

Abstract (from CDS):

Growing evidence for shocks in nova outflows includes (1) multiple velocity components in the optical spectra; (2) hard X-ray emission starting weeks to months after the outburst; (3) an early radio flare on time-scales of months, in excess of that predicted from the freely expanding photoionized gas; and, perhaps most dramatically, (4) ∼ GeV gamma-ray emission. We present a one-dimensional model for the shock interaction between the fast nova outflow and a dense external shell (DES) and its associated thermal X-ray, optical, and radio emission. The lower velocity DES could represent an earlier stage of mass-loss from the white dwarf or ambient material not directly related to the thermonuclear runaway. The forward shock is radiative initially when the density of shocked gas is highest, at which times radio emission originates from the dense cooling layer immediately downstream of the shock. Our predicted radio light curve is characterized by sharper rises to maximum and later peak times at progressively lower frequencies, with a peak brightness temperature that is approximately independent of frequency. We apply our model to the recent gamma-ray producing classical nova V1324 Sco, obtaining an adequate fit to the early radio maximum assuming that the DES possesses a characteristic velocity ∼ 103 km/s and mass ∼ few 10–4M☉; the former is consistent with the velocities of narrow-line absorption systems observed previously in nova spectra, while the total ejecta mass of the DES and fast outflow is consistent with that inferred independently by modelling the late radio peak as uniformly expanding photoionized gas. Importantly, however, our thermal model can only explain the peak radio fluxes if line cooling of the post-shock gas at temperatures ∼ 106K is suppressed below its collisional ionization equilibrium value for solar abundances due to photoionization; if this condition is not satisfied, this strongly suggests that the early radio peak is instead non-thermal (e.g. synchrotron) in origin. Rapid evolution of the early radio light curves requires the DES to possess a steep outer density profile, which may indicate that the onset of mass-loss from the white dwarf was rapid, providing indirect evidence that the DES was expelled as the result of the thermonuclear runaway event. Re-processed X-rays from the shock absorbed by the DES at early times are found to contribute significantly to the optical/UV emission.

Abstract Copyright: © 2014 The Authors Published by Oxford University Press on behalf of the Royal Astronomical Society (2014)

Journal keyword(s): radiation mechanisms: thermal - shock waves - novae, cataclysmic variables

Simbad objects: 17

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Number of rows : 17
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2026
#notes
1 V* GK Per No* 03 31 12.0098863320 +43 54 15.469951212   14.139 13.090 12.589   K1IV 986 0
2 LMCN 2005-11a No* 05 10 32.68 -69 12 35.7           ~ 22 0
3 LMCN 2000-07a No* 05 25 01.63 -70 14 17.4           ~ 24 0
4 V* V351 Pup No* 08 11 38.3931386664 -35 07 30.288675216           ~ 128 0
5 V* T Pyx CV* 09 04 41.5061511720 -32 22 47.502932700           ~ 476 0
6 V* V382 Vel No* 10 44 48.3975221712 -52 25 31.168268472   15.945 15.737 16.173   ~ 201 0
7 V* V382 Nor No* 16 19 44.74 -51 34 53.1           ~ 35 0
8 V* V1188 Sco No* 17 44 21.59 -34 16 35.7           ~ 31 0
9 V* V1324 Sco No* 17 50 53.9093841216 -32 37 21.090962028           ~ 100 0
10 V* V5116 Sgr No* 18 17 50.7277266627 -30 26 32.079704535     19.181   18.962 ~ 68 0
11 V* V4633 Sgr No* 18 21 40.48680 -27 31 37.2972           ~ 86 0
12 V* V476 Sct No* 18 32 04.75 -06 43 34.3           ~ 30 0
13 V* V477 Sct No* 18 38 42.93 -12 16 15.6           ~ 28 0
14 V* V838 Her No* 18 46 31.4714863335 +12 14 02.104189516           ~ 304 0
15 V* V1663 Aql No* 19 05 12.50 +05 14 12.0           Kep 39 0
16 V* V1974 Cyg No* 20 30 31.6546001712 +52 37 50.837478240           ~ 597 0
17 EM* AS 453 Sy* 21 02 09.8189024184 +45 46 32.733603228   16.04 14.68 11.38   Mep 337 0

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