2004NewA....9..545H


Query : 2004NewA....9..545H

2004NewA....9..545H - New Astronomy, 9, 545-564 (2004/September-0)

Searching for radiative pumping lines of OH masers: II. The 53.3 µm absorption line towards 1612 MHz OH maser sources.

HE J.H. and CHEN P.S.

Abstract (from CDS):

This is the second paper in a series aiming at searching for infrared pumping lines for galactic 1612 MHz OH masers. Our paper I is devoted to the 34.6 mum absorption lines in ISO SWS spectra towards a large sample of galactic OH/IR sources. This paper analyzes the 53.3 mum line in the ISO LWS spectra towards a similar sample of OH/IR sources. A search with position radius of 1 arcmin in ISO Data Archive (IDA) results in 137 LWS spectra covering 53.3 mum associated with 47 galactic OH/IR sources and 4 ones associated with megamasers Arp 220 and NGC 253. (These two magamasers are included for comparison purpose only.) Ten of these galactic OH/IR sources are found to show and another 5 ones tentatively show the 53.3 mum absorption while another 7 sources (our group U1 and U2 sources) highly probably do not show this line. The source class is found to be correlated with the type of spectral profile: red supergiants (RSGs) and AGB stars tend to show strong blue-shifted fillinge! mission in their 53.3 mum absorption line profiles while H II regions tend to show a weak red-shifted filling emission in the line profile. GC sources and megamasers mainly show symmetrical profile in the line core while megamasers tend to show an additional absorption tail on the blue side of the line profile. It is argued that the filling emission might be the manifestation of an unresolved half emission half absorption profile of the 53.3 mum doublet which might be produced by the transitions among the two levels: 2Pi1/2(J=3/2) and 2Pi1/2(J=5/2) and their closely related levels. The 53.3 to 34.6 mum equivalent width (EW) ratio is close to unity for RSGs but much larger than unity for GC sources and megamasers while H II regions only show the 53.3 mum line. The pump rate defined as maser to IR photon flux ratio is approximately 5% for RSGs. The pump rates of GC sources are three order of magnitude smaller. Both the large 53.3 to 34.6 mum EW ratio and the small pump rate o! f the GC OH masers reflect that the two detected `pumping lines' in these sources are actually of interstellar origin. The pump rate of Arp 220 is 32% - much larger than that of RSGs, which indicates that the contribution of other pumping mechanisms to this megamaser is important. A handful of non-detections of the 34.6 or 53.3 mum line or both can be explained partly by the genuinely weakness of the OH masers and partly by some other mechanisms weakening the IR pumping lines, such as clumpy OH shell or limb filling emission.

Abstract Copyright:

Journal keyword(s): Masers - Stars: AGB and post-AGB - Circumstellar matter - Supergiants - HII regions - Radio lines: stars

Simbad objects: 56

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Number of rows : 56
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 NGC 253 SyG 00 47 33.134 -25 17 19.68   8.03   6.94 8.1 ~ 3337 2
2 IRC +10011 OH* 01 06 25.9879717848 +12 35 52.896392052   20.7   18.26 14.01 M8 420 0
3 OH 127.8-00.0 OH* 01 33 51.21048 +62 26 53.2032           O-rich 181 0
4 V* IK Tau OH* 03 53 28.8924743304 +11 24 21.895183368 16.99 14.463 16.171 14.101   M7-11 638 0
5 ZOAG G184.95-00.85 SFR 05 53 42.717 +24 14 54.01           ~ 39 0
6 IRAS 05506+2414 Y*O 05 53 43.5659728656 +24 14 44.663981208           G9-K2 44 0
7 NAME Mon R2 HII 06 07 47.58 -06 22 42.6           ~ 742 2
8 RAFGL 961 Y*O 06 34 37.74144 +04 12 44.1972           O-rich 240 1
9 PN Vo 1 PN 06 59 26.4167860656 -79 38 47.118534828           [WC10] 100 0
10 V* VY CMa s*r 07 22 58.3261352189 -25 46 03.194390594 12.01 10.068 8.691 7.938   M5Iae 1104 0
11 MR 22 PN 10 21 33.85920 -58 05 47.6628           A2Ie 101 0
12 V* R Crt AB* 11 00 33.8525664720 -18 19 29.582708520   10.33 9.80     M7/8III 211 0
13 IC 4553 SyG 15 34 57.22396 +23 30 11.6084   14.76 13.88     ~ 2961 4
14 IRAS 15452-5459 pA* 15 49 11.3344710672 -55 08 51.846940176           O-rich 31 0
15 NGC 6153 PN 16 31 30.5708444544 -40 15 12.646208700   10.7 15.55     ~ 303 0
16 IRAS 16342-3814 pA* 16 37 39.8691983808 -38 20 17.443998996           ~ 136 0
17 NGC 6302 PN 17 13 44.5 -37 06 11           O-rich 795 1
18 RAFGL 6815S pA* 17 18 19.8040606320 -32 27 21.547417932           G2I 148 0
19 RAFGL 5379 OH* 17 44 24.0074369832 -31 55 35.414175828           O-rich 88 0
20 IRAS 17424-2852 IR 17 45 38.9 -28 53 28           ~ 10 0
21 RAFGL 2003 IR 17 45 39.1 -29 00 23           ~ 22 0
22 NAME Sgr A* X 17 45 40.03599 -29 00 28.1699           ~ 4392 3
23 NAME Quintuplet Cluster OpC 17 46 13.9 -28 49 48           ~ 526 0
24 IRAS 17431-2846 IR 17 46 17.9 -28 48 01           ~ 10 0
25 OH 000.3-00.2 OH* 17 47 06.94704 -28 44 41.9136           O-rich 78 1
26 LBN 3 HII 17 47 08.0 -28 46 30           ~ 82 3
27 IRAS 17439-2845 HII 17 47 08.6 -28 46 18           ~ 86 1
28 IRAS 17441-2822 HII 17 47 20.224 -28 23 04.13           ~ 28 0
29 NAME Sgr B2 MoC 17 47 20.4 -28 23 07           ~ 2266 1
30 Hen 2-289 Sy* 17 49 48.2107694784 -37 01 27.797630520       13.828   M4/5:e 162 0
31 RAFGL 2046 HII 18 00 32.1 -24 04 03           ~ 362 0
32 V* VX Sgr s*r 18 08 04.0442790744 -22 13 26.600899044 11.72 9.41 6.52 3.90 2.11 M8.5Ia 596 0
33 RAFGL 2136 Y*O 18 22 26.52888 -13 30 14.0400           ~ 285 0
34 OH 018.2+00.4 OH* 18 22 43.08192 -12 47 41.5356           O-rich 40 0
35 V* V370 Ser Or* 18 29 49.24584 +01 16 31.5480           ~ 31 0
36 OH 026.5+00.6 OH* 18 37 32.50920 -05 23 59.1936           O-rich 301 1
37 IRAS 18437-0302 AB* 18 46 23.76480 -02 59 21.6924           O-rich 2 0
38 OH 032.8-00.3 OH* 18 52 22.25472 -00 14 11.8428           O-rich 123 0
39 RAFGL 2290 OH* 18 58 30.0951077544 +06 42 57.696212124           O-rich 126 0
40 OH 037.1-00.8 OH* 19 02 06.28560 +03 20 15.9900           O-rich 74 0
41 V* R Aql OH* 19 06 22.2510922392 +08 13 48.012661776 8.06 7.69 6.09     M6.5-9e 564 2
42 HD 179821 pA* 19 13 58.6082398776 +00 07 31.935181836 10.81 9.694 8.19     G4_0-Ia 239 0
43 PN Vy 2-2 PN 19 24 22.2390166933 +09 53 56.259102426   14.02 12.65 13.38   O-rich 261 0
44 IRC +10420 pA* 19 26 48.0979492536 +11 21 16.758531216   13.98 11.66     F8Ia+e 477 0
45 PN K 3-35 PN 19 27 43.9749997920 +21 30 02.907990216           O-rich 149 0
46 Min 1-92 pA* 19 36 18.9295687968 +29 32 49.785288144 12.13 12.35 11.75 11.54   B0.5IV[e] 254 0
47 V* Z Cyg Mi* 20 01 27.5075704056 +50 02 32.634937212   11.12 7.10 8.79   M5.5-6.5e 162 0
48 IRC -10529 OH* 20 10 27.8731455576 -06 16 13.758742596         15.49 M: 141 0
49 WSRTGP 2025+3712 HII 20 27 26.4 +37 22 48           ~ 48 0
50 NAME SH 2-106 IR Y*O 20 27 26.502 +37 22 42.03           ~ 163 1
51 NML Cyg s*r 20 46 25.5392819088 +40 06 59.464289232           M7/8 508 0
52 IRAS 22036+5306 pA* 22 05 30.28608 +53 21 32.7888           F4III 78 0
53 SH 2-140 OpC 22 19 07.8 +63 17 07           ~ 658 2
54 IRAS 22176+6303 Y*O 22 19 18.23 +63 18 47.5           ~ 595 0
55 RAFGL 2885 OH* 22 19 27.47784 +59 51 21.7080           O-rich 136 0
56 V* R Aqr Sy* 23 43 49.4634303216 -15 17 04.176349872   8.823 7.683 9.37   M6.5-8.5e 784 0

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