2018ApJ...855...62N


Query : 2018ApJ...855...62N

2018ApJ...855...62N - Astrophys. J., 855, 62-62 (2018/March-1)

Candidate water vapor lines to locate the H2O snowline through high-dispersion spectroscopic observations. III. Submillimeter H2 16O and H2 18O lines.

NOTSU S., NOMURA H., WALSH C., HONDA M., HIROTA T., AKIYAMA E. and MILLAR T.J.

Abstract (from CDS):

In this paper, we extend the results presented in our former papers on using ortho-H216O line profiles to constrain the location of the H2O snowline in T Tauri and Herbig Ae disks, to include submillimeter para-H216O and ortho- and para-H218O lines. Since the number densities of the ortho- and para-H218O molecules are about 560 times smaller than their 16O analogs, they trace deeper into the disk than the ortho-H216O lines (down to z = 0, i.e., the midplane). Thus these H218O lines are potentially better probes of the position of the H2O snowline at the disk midplane, depending on the dust optical depth. The values of the Einstein A coefficients of submillimeter candidate water lines tend to be lower (typically <10–4 s–1) than infrared candidate water lines. Thus in the submillimeter candidate water line cases, the local intensity from the outer optically thin region in the disk is around 104 times smaller than that in the infrared candidate water line cases. Therefore, in the submillimeter lines, especially H218O and para-H216O lines with relatively lower upper state energies (∼a few 100 K) can also locate the position of the H2O snowline. We also investigate the possibility of future observations with ALMA to identify the position of the water snowline. There are several candidate water lines that trace the hot water gas inside the H2O snowline in ALMA Bands 5-10.

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

Journal keyword(s): astrochemistry - ISM: molecules - protoplanetary disks - stars: formation - submillimeter: planetary systems

Simbad objects: 14

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Number of rows : 14
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 [JCC87] IRAS 2A Y*O 03 28 55.55 +31 14 36.7           ~ 513 3
2 [JCC87] IRAS 4A Y*O 03 29 10.49 +31 13 30.8           ~ 770 1
3 [JCC87] IRAS 4B Y*O 03 29 12.058 +31 13 02.05           ~ 625 0
4 V* DG Tau TT* 04 27 04.6921275888 +26 06 16.060169268 13.57 13.97 10.50 12.28   K6Ve 1092 1
5 V* HL Tau Or* 04 31 38.5107609312 +18 13 57.859747968   15.89 14.49 14.39   K5 1546 0
6 V* DM Tau Or* 04 33 48.7336763736 +18 10 09.973460280 14.30 14.82 14.00     M2Ve 731 0
7 V* AA Tau Or* 04 34 55.4201902392 +24 28 53.033624580 13.14 13.34 12.20 12.03   K5Ve 801 0
8 NAME Orion-KL SFR 05 35 14.16 -05 22 21.5           ~ 2421 1
9 V* V883 Ori Or* 05 38 18.1018261392 -07 02 26.017707120           F:I: 274 0
10 NAME Orion Molecular Cloud MoC 05 56 -01.8           ~ 1227 1
11 V* TW Hya TT* 11 01 51.9053285064 -34 42 17.033218380   11.94 10.50 10.626 9.18 K6Ve 2144 1
12 HD 100546 Be* 11 33 25.4408872296 -70 11 41.241297948   6.71 6.30   6.64 A0VaekB8_lB 894 1
13 HD 163296 Ae* 17 56 21.2881851168 -21 57 21.871819008 7.00 6.93 6.85 6.86 6.67 A3VaekA1mA1 1301 0
14 DR 21 (OH) cor 20 39 01.01 +42 22 50.2           ~ 427 0

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