2022ApJ...925..187P


Query : 2022ApJ...925..187P

2022ApJ...925..187P - Astrophys. J., 925, 187-187 (2022/February-1)

Photoionization Modeling of the Dusty Nova V1280 Scorpii.

PANDEY R., DAS R., SHAW G. and MONDAL S.

Abstract (from CDS):

We perform photoionization modeling of the dusty nova V1280 Scorpii (V1280 Sco) with the aim to study the changes in the physical and chemical parameters. We model the predust and postdust phase and optical and near-infrared spectra using the photoionization code CLOUDY, v.17.02, considering a two-component (low-density and high-density regions) model. From the best-fit model, we find that the temperature and luminosity of the central ionizing source in the predust phase is in the range 1.32-1.50 x 104 K and 2.95-3.16 x 1036 ergs–1, respectively, which increase to 1.58-1.62 x 104 K and 3.23-3.31 x 1036 ergs–1, respectively, in the postdust phase. It is found that a very high hydrogen density (∼1013-1014 cm–3) is required for the proper generation of spectra. Dust condensation conditions are achieved at high ejecta density (∼3.16 x 108 cm–3) and low temperature (∼2000 K) in the outer region of the ejecta. It is found that a mixture of small (0.005-0.25 µm) amorphous carbon dust grains and large (0.03-3.0 µm) astrophysical silicate dust grains is present in the ejecta in the postdust phase. Our model yields very high elemental abundance values as C/H = 13.5-20, N/H = 250, O/H = 27-35, by number, relative to solar values, during the predust phase, which decrease in the postdust phase.

Abstract Copyright: © 2022. The Author(s). Published by the American Astronomical Society.

Journal keyword(s): Novae - Photoionization - Astrophysical dust processes - White dwarf stars

Simbad objects: 25

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Number of rows : 25
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 LMCN 1991-04a No* 05 03 44.96 -70 18 13.5           ~ 62 0
2 V* T Pyx CV* 09 04 41.5061511720 -32 22 47.502932700           ~ 476 0
3 V* V382 Vel No* 10 44 48.3975221712 -52 25 31.168268472   15.945 15.737 16.173   ~ 201 0
4 V* V1065 Cen No* 11 43 10.121 -58 04 04.08       18.4   ~ 50 0
5 V* V842 Cen No* 14 35 52.5683885352 -57 37 35.391092232           ~ 160 0
6 V* V1280 Sco No* 16 57 41.2185889117 -32 20 35.700757833           ~ 110 0
7 V* V2676 Oph No* 17 26 07.08 -25 51 45.4           ~ 43 0
8 V* V2615 Oph No* 17 42 43.9985841119 -23 40 35.084130692           ~ 58 1
9 V* DQ Her CV* 18 07 30.2510391864 +45 51 32.564791872   14.605 14.443 14.800   M3+Ve 1048 1
10 V* V4160 Sgr No* 18 14 13.83 -32 12 28.5           ~ 69 0
11 V* V6567 Sgr No* 18 22 45.20 -19 36 02.6           ~ 17 0
12 V* FH Ser No* 18 30 47.0401403328 +02 36 52.029761940           ~ 215 0
13 V* V476 Sct No* 18 32 04.75 -06 43 34.3           ~ 30 0
14 V* V5668 Sgr No* 18 36 56.827920 -28 55 39.97524       16.028   ~ 142 0
15 V* V496 Sct No* 18 43 45.57 -07 36 42.0           ~ 56 0
16 V* V838 Her No* 18 46 31.4714863335 +12 14 02.104189516           ~ 304 0
17 V* QV Vul No* 19 04 40.2842064624 +21 46 14.155475808           ~ 120 0
18 V* V1419 Aql No* 19 13 06.7917062592 +01 34 23.356169184           ~ 82 0
19 V* NQ Vul No* 19 29 14.7520337784 +20 27 59.568491916           ~ 171 0
20 V* V2274 Cyg No* 20 07 17.7740102078 +36 04 32.829959153           ~ 66 0
21 V* V339 Del No* 20 23 30.6873337580 +20 46 03.765339899   17.50 16.86     ~ 225 0
22 V* QU Vul No* 20 26 46.0200167016 +27 50 43.163406959           ~ 277 0
23 V* V1974 Cyg No* 20 30 31.6546001712 +52 37 50.837478240           ~ 597 0
24 V* V2362 Cyg CV* 21 11 32.3419758636 +44 48 03.668158208           ~ 108 0
25 V* V705 Cas No* 23 41 47.2354174125 +57 31 00.826200729       16.055   ~ 207 0

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