2018ApJ...867..155L


Query : 2018ApJ...867..155L

2018ApJ...867..155L - Astrophys. J., 867, 155-155 (2018/November-2)

Red supergiants in the JWST era. I. Near-IR photometric diagnostics.

LEVESQUE E.M.

Abstract (from CDS):

The Near Infrared Camera (NIRCam) on the James Webb Space Telescope (JWST) will be an incredibly powerful instrument for studying red supergiants (RSGs). The high luminosities and red peak wavelengths of these stars make them ideal targets for JWST/NIRCam. With effective photometric diagnostics in place, imaging RSG populations in multiple filters will make it possible to determine these stars' physical properties and, in cases where JWST pre-explosion imaging is available, to identify RSG supernova progenitors. This paper uses observed and model spectra of Galactic RSGs to simulate JWST/NIRCam near-IR photometry and colors, quantify and test potential diagnostics of effective temperature and bolometric magnitude, and present photometric techniques for separating background RSG and foreground dwarf populations. While results are presented for the full suite of near-IR filters, this work shows that (F070W-F200W) is the JWST/NIRCam color index most sensitive to effective temperature, F090W is the best band for determining bolometric magnitude, and the (F070W-F090W) versus (F090W-F200W) color-color diagram can be used to separate foreground dwarf and background RSG samples. The combination of these three filters is recommended as the best suite of photometric observations to use when studying RSGs with JWST.

Abstract Copyright: © 2018. The American Astronomical Society. All rights reserved.

Journal keyword(s): stars: atmospheres - stars: massive - supergiants - techniques: photometric

Simbad objects: 19

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Number of rows : 19
N Identifier Otype ICRS (J2000)
RA
ICRS (J2000)
DEC
Mag U Mag B Mag V Mag R Mag I Sp type #ref
1850 - 2024
#notes
1 NAME SMC G 00 52 38.0 -72 48 01   2.79 2.2     ~ 11146 1
2 V* V466 Cas s*r 01 19 53.6180547504 +58 18 30.745534716 13.04 10.74 8.62 6.86 5.44 M0.5Ib 79 0
3 V* SU Per s*r 02 22 06.8948309496 +56 36 14.893650072 13.86 11.57 9.40     M3-M4Iab 145 0
4 V* RS Per s*r 02 22 24.2955658080 +57 06 34.102933812 12.37 10.09 8.7680     M3.5IabFe-1 143 0
5 V* BE Cam LP* 03 49 31.2775482648 +65 31 33.525822504 8.49 6.36 4.48 2.77 1.35 M2II 113 0
6 WOH G 64 Mi* 04 55 10.5236094912 -68 20 30.019011036     18.46 15.69 12.795 M7.5(I)e 97 0
7 NAME LMC G 05 23 34.6 -69 45 22     0.4     ~ 17432 0
8 V* V362 Aur s*r 05 27 10.2176658912 +29 55 15.795216264   9.58 7.32     M1.5Ib 93 0
9 * alf Ori s*r 05 55 10.30536 +07 24 25.4304 4.38 2.27 0.42 -1.17 -2.45 M1-M2Ia-Iab 1671 0
10 V* RY Mon C* 07 06 56.4753359184 -07 33 26.505848700   11.94 7.50     C-N5 97 0
11 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1103 0
12 V* V384 Pup s*r 07 41 02.6293485216 -31 40 59.096449344   10.81 8.77     M3Iab-Ib 59 0
13 V* QY Pup s*r 07 47 38.5262364936 -15 59 26.481207696   8.095 6.309     K1Ia-Iab 95 0
14 HD 181475 V* 19 20 48.3121994424 -04 30 09.009698112   9.09 6.96     K7IIa 50 0
15 V* NR Vul s*r 19 50 11.9276355408 +24 55 24.180686508   12.41 9.36 6.60 4.49 M1Ia: 81 0
16 V* RW Cyg s*r 20 28 50.5903286280 +39 58 54.425527932 13.00 10.60 8.00 5.32 3.25 M3-M4Ia-Iab 127 0
17 * mu. Cep s*r 21 43 30.4595558543 +58 46 48.165937434 8.85 6.43 4.08 1.98 0.22 M2-Ia 669 1
18 V* V424 Lac s*r 22 56 25.9983901008 +49 44 00.758688324 8.66 6.71 4.94 3.59 2.54 K5Ib 154 0
19 NAME Local Group GrG ~ ~           ~ 8389 0

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