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JIA96 - SiO Maser Sources in the Outer Disk of the Galaxy

Interferometry data

Short title: Jiang et al. (1996)
Authors: Jiang, B. W. Deguchi, S. Yamamura, I. Nakada, Y. Cho, S. H. Yamagata, T.
Journal: Astrophysical Journal Supplement v.106, p.463
Bibcode:

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Detection table: Show detection table (128 detection) Non-detection table: Show non-detection table (243 non-detection)

Abstract
The observations in the ²⁸SiO j = 1-0 V = 1, J = 1-0 V = 2 lines and the ²⁹SiO j = 1-0, V = 0 lines were simultaneously made toward 181 color-selected IRAS sources in the outer disk of the Galaxy (at longitudes between 90� and 250�). The ²⁸SiO lines were detected in 63 sources (56 new) and the ²⁹SiO line in 11 sources (9 new). Most of the detections are optically variable stars, mainly Mira-type variables and a few semiregular variables. The detection rate (35%) is much lower than that of the bulge survey performed by the same observational system the 45 m telescope at Nobeyama Radio Observatory. The lower detection rate of SiO maser emission is partly attributed to the increase of contaminations by stars with C-rich circumstellar envelopes and young stellar objects in the outer disk sample. The kinematical implications of the observational results are also discussed. The luminosity distances to the SiO maser sources are estimated from their IRAS fluxes at 12 mum and colors. By combining the SiO radial velocity and the luminosity distance, the rotation curve of the outer Galactic disk is found to be slightly falling within the Galactocentric distance between 8.5 and 12 kpc. The sources located within 20� from the Galactic anticenter direction are used to check for a peculiar motion of the local standard of rest.

Abstract

The observations in the ²⁸SiO j = 1-0 V = 1, J = 1-0 V = 2 lines and the ²⁹SiO j = 1-0, V = 0 lines were simultaneously made toward 181 color-selected IRAS sources in the outer disk of the Galaxy (at longitudes between 90� and 250�). The ²⁸SiO lines were detected in 63 sources (56 new) and the ²⁹SiO line in 11 sources (9 new). Most of the detections are optically variable stars, mainly Mira-type variables and a few semiregular variables. The detection rate (35%) is much lower than that of the bulge survey performed by the same observational system the 45 m telescope at Nobeyama Radio Observatory. The lower detection rate of SiO maser emission is partly attributed to the increase of contaminations by stars with C-rich circumstellar envelopes and young stellar objects in the outer disk sample. The kinematical implications of the observational results are also discussed. The luminosity distances to the SiO maser sources are estimated from their IRAS fluxes at 12 mum and colors. By combining the SiO radial velocity and the luminosity distance, the rotation curve of the outer Galactic disk is found to be slightly falling within the Galactocentric distance between 8.5 and 12 kpc. The sources located within 20� from the Galactic anticenter direction are used to check for a peculiar motion of the local standard of rest.

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Detection table from Jiang et al. (1996)

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ID	Obs. RA	Obs. Dec	l	b	Source name	Line	V_peak	T_a	∫T_a dv	Date	Telescope	RMS	List	Ref.
	(J2000)	(J2000)	(deg.)	(deg.)		SiO	(km/s)	(K)	(K*km/s)			(Jy)
1	00 15 24.2	+54 54 15.1	117.720759	-7.602531	IRAS00127+5437	SiO J=1-0 v=2	-91.788	0.149	0.32	1995-05-28	NRO	0.029	NRO	JIA96
2	00 36 36.4	+68 01 13.2	121.539224	5.188705	IRAS00336+6744	SiO J=1-0 v=1	-90.973	0.143	1.13	1995-05-26	NRO	0.034	NRO	JIA96
3	00 36 36.4	+68 01 13.2	121.539224	5.188705	IRAS00336+6744	SiO J=1-0 v=2	-90.267	0.139	0.33	1995-05-26	NRO	0.036	NRO	JIA96
4	00 49 7.2	+68 05 45.5	122.714782	5.225189	IRAS00459+6749	SiO J=1-0 v=1	-90.252	0.597	2.68	1995-05-22	NRO	0.060	NRO	JIA96
5	00 49 7.2	+68 05 45.5	122.714782	5.225189	IRAS00459+6749	SiO J=1-0 v=2	-90.177	0.308	1.22	1995-05-22	NRO	0.064	NRO	JIA96
6	00 56 29.1	+60 47 14.3	123.548072	-2.078408	IRAS00534+6031	SiO J=1-0 v=1	-100.604	0.157	0.19	1995-05-26	NRO	0.032	NRO	JIA96
7	00 56 29.1	+60 47 14.3	123.548072	-2.078408	IRAS00534+6031	SiO J=1-0 v=2	-100.614	0.148	0.38	1995-05-26	NRO	0.029	NRO	JIA96
8	01 25 1.9	+61 04 38.4	126.983855	-1.529864	IRAS01217+6049	29SiO J=1-0 v=0	-12.34	0.51	0.35		NRO	0.065	NRO	JIA96
9	01 25 1.9	+61 04 38.4	126.983855	-1.529864	IRAS01217+6049	SiO J=1-0 v=1	-12.411	4.563	15.41	1995-05-01	NRO	0.066	NRO	JIA96
10	01 25 1.9	+61 04 38.4	126.983855	-1.529864	IRAS01217+6049	SiO J=1-0 v=2	-12.669	3.808	10.15	1995-05-01	NRO	0.075	NRO	JIA96
11	02 35 44.9	+65 08 57.9	133.610505	4.463113	IRAS02316+6455	29SiO J=1-0 v=0	11.03	0.64	1.57		NRO	0.119	NRO	JIA96
12	02 35 44.9	+65 08 57.9	133.610505	4.463113	IRAS02316+6455	SiO J=1-0 v=1	12.628	8.006	41.84	1995-05-01	NRO	0.115	NRO	JIA96
13	02 35 44.9	+65 08 57.9	133.610505	4.463113	IRAS02316+6455	SiO J=1-0 v=2	12.967	14.001	45.9	1995-05-01	NRO	0.122	NRO	JIA96
14	02 47 24.7	+63 58 14.2	135.241945	3.906232	IRAS02433+6345	SiO J=1-0 v=1	-55.277	0.965	3.02	1995-05-21	NRO	0.065	NRO	JIA96
15	02 47 24.7	+63 58 14.2	135.241945	3.906232	IRAS02433+6345	SiO J=1-0 v=2	-55.392	1.171	3.43	1995-05-21	NRO	0.070	NRO	JIA96
16	02 50 37.6	+56 58 57.3	138.654301	-2.205782	IRAS02469+5646	SiO J=1-0 v=1	-40.585	0.345	1.3	1995-05-21	NRO	0.062	NRO	JIA96
17	02 50 45.3	+55 48 57.9	139.187539	-3.243747	IRAS02470+5536	SiO J=1-0 v=1	-35.105	0.436	1.95	1995-05-21	NRO	0.071	NRO	JIA96
18	02 50 45.3	+55 48 57.9	139.187539	-3.243747	IRAS02470+5536	SiO J=1-0 v=2	-38.968	0.539	2.03	1995-05-21	NRO	0.073	NRO	JIA96
19	03 25 8.6	+65 32 5.2	137.970439	7.255417	IRAS03206+6521	SiO J=1-0 v=2	-37.802	0.283	0.63	1995-05-22	NRO	0.048	NRO	JIA96
20	03 51 4.9	+58 42 24.9	144.488787	3.569746	IRAS03469+5833	SiO J=1-0 v=1	-74.13	0.473	0.6	1995-05-27	NRO	0.039	NRO	JIA96
21	03 51 4.9	+58 42 24.9	144.488787	3.569746	IRAS03469+5833	SiO J=1-0 v=2	-74.456	0.342	0.49	1995-05-27	NRO	0.039	NRO	JIA96
22	03 54 56.3	+48 35 59.8	151.34336	-3.883669	IRAS03513+4827	SiO J=1-0 v=1	-56.294	1.199	5.11	1995-05-27	NRO	0.038	NRO	JIA96
23	03 54 56.3	+48 35 59.8	151.34336	-3.883669	IRAS03513+4827	SiO J=1-0 v=2	-63.849	0.818	4.99	1995-05-27	NRO	0.040	NRO	JIA96
24	04 01 13	+55 17 44.8	147.741729	1.84407	IRAS03572+5509	SiO J=1-0 v=1	-37.546	0.126	0.1	1995-05-26	NRO	0.030	NRO	JIA96
25	04 12 25.5	+53 55 5.8	149.87016	1.910092	IRAS04085+5347	SiO J=1-0 v=2	-15.338	0.361	0.98	1995-05-22	NRO	0.037	NRO	JIA96
26	04 24 40.2	+48 07 24.2	155.298128	-0.885753	IRAS04209+4800	SiO J=1-0 v=1	-16.766	1.208	3.64	1995-05-22	NRO	0.103	NRO	JIA96
27	04 24 40.2	+48 07 24.2	155.298128	-0.885753	IRAS04209+4800	SiO J=1-0 v=2	-16.749	1.075	2.54	1995-05-22	NRO	0.057	NRO	JIA96
28	05 06 29.7	+35 23 16.9	170.023353	-3.249369	IRAS05031+3519	SiO J=1-0 v=2	-35.462	0.231	0.62	1994-05-15	NRO	0.087	NRO	JIA96
29	05 11 19.5	+52 52 33.7	156.437702	7.835047	IRAS05073+5248	29SiO J=1-0 v=0	0.73	0.97	1.68		NRO	0.115	NRO	JIA96
30	05 11 19.5	+52 52 33.7	156.437702	7.835047	IRAS05073+5248	SiO J=1-0 v=1	1.041	9.604	20.54	1995-05-01	NRO	0.108	NRO	JIA96
31	05 11 19.5	+52 52 33.7	156.437702	7.835047	IRAS05073+5248	SiO J=1-0 v=2	1.32	12.634	27.14	1995-05-01	NRO	0.124	NRO	JIA96
32	05 12 52	+46 43 2.5	161.616883	4.446544	IRAS05091+4639	SiO J=1-0 v=1	12.676	0.116	0.15	1995-05-27	NRO	0.027	NRO	JIA96
33	05 16 22.4	+30 42 40.5	175.032964	-4.32936	IRAS05131+3039	SiO J=1-0 v=1	11.34	0.43	1.3	1994-05-15	NRO	0.043	NRO	JIA96
34	05 16 22.4	+30 42 40.5	175.032964	-4.32936	IRAS05131+3039	SiO J=1-0 v=2	12.145	0.132	0.82	1994-05-15	NRO	0.044	NRO	JIA96
35	05 17 43.4	+25 24 59.4	179.566811	-7.117846	IRAS05146+2521	SiO J=1-0 v=1	-1.292	0.424	1.21	1994-05-15	NRO	0.166	NRO	JIA96
36	05 17 43.4	+25 24 59.4	179.566811	-7.117846	IRAS05146+2521	SiO J=1-0 v=2	-1.419	0.559	1.23	1994-05-15	NRO	0.173	NRO	JIA96
37	05 31 24.7	+19 47 19.1	186.055912	-7.592823	IRAS05284+1945	SiO J=1-0 v=1	14.24	0.247	0.52	1994-05-19	NRO	0.054	NRO	JIA96
38	05 31 24.7	+19 47 19.1	186.055912	-7.592823	IRAS05284+1945	SiO J=1-0 v=2	14.647	0.375	1.56	1994-05-19	NRO	0.044	NRO	JIA96
39	05 35 33.3	+23 53 19.3	183.094871	-4.581665	IRAS05325+2351	SiO J=1-0 v=1	8.861	0.273	1.22	1994-05-16	NRO	0.085	NRO	JIA96
40	05 35 33.3	+23 53 19.3	183.094871	-4.581665	IRAS05325+2351	SiO J=1-0 v=2	8.522	0.109	0.28	1994-05-16	NRO	0.086	NRO	JIA96
41	05 38 32.9	+25 00 6.4	182.515941	-3.411416	IRAS05354+2458	SiO J=1-0 v=1	4.117	1.51	4.53	1994-05-15	NRO	0.225	NRO	JIA96
42	05 40 7.6	+37 38 10.2	171.988985	3.593034	IRAS05367+3736	SiO J=1-0 v=1	-36.633	4.201	5.62	1994-05-15	NRO	0.166	NRO	JIA96
43	05 40 7.6	+37 38 10.2	171.988985	3.593034	IRAS05367+3736	SiO J=1-0 v=2	-36.46	4.013	8.04	1994-05-15	NRO	0.169	NRO	JIA96
44	05 40 0.7	+28 42 49.2	179.542894	-1.161821	IRAS05368+2841	SiO J=1-0 v=1	-12.545	5.863	27.06	1994-05-18	NRO	0.074	NRO	JIA96
45	05 40 0.7	+28 42 49.2	179.542894	-1.161821	IRAS05368+2841	SiO J=1-0 v=2	-11.83	6.88	27.43	1994-05-18	NRO	0.063	NRO	JIA96
46	05 41 55.4	+38 56 0.5	171.068728	4.575212	IRAS05384+3854	SiO J=1-0 v=1	8.698	2.197	8.51	1994-05-18	NRO	0.063	NRO	JIA96
47	05 41 55.4	+38 56 0.5	171.068728	4.575212	IRAS05384+3854	SiO J=1-0 v=2	8.392	1.195	3.49	1994-05-18	NRO	0.061	NRO	JIA96
48	05 42 8.9	+32 02 22.1	176.964995	0.989574	IRAS05388+3200	29SiO J=1-0 v=0	4.22	1.98	2.51		NRO	0.090	NRO	JIA96
49	05 42 8.9	+32 02 22.1	176.964995	0.989574	IRAS05388+3200	SiO J=1-0 v=1	4.689	49.254	111.76	1994-05-01	NRO	0.083	NRO	JIA96
50	05 42 8.9	+32 02 22.1	176.964995	0.989574	IRAS05388+3200	SiO J=1-0 v=2	4.639	28.448	65.68	1994-05-01	NRO	0.093	NRO	JIA96
51	05 45 29.7	+29 07 4.3	179.830782	0.071512	IRAS05423+2905	SiO J=1-0 v=1	25.764	1.315	6.76	1994-05-16	NRO	0.065	NRO	JIA96
52	05 45 29.7	+29 07 4.3	179.830782	0.071512	IRAS05423+2905	SiO J=1-0 v=2	23.586	1.762	7.65	1994-05-16	NRO	0.065	NRO	JIA96
53	05 47 30.5	+27 08 11.4	181.754383	-0.578498	IRAS05443+2707	SiO J=1-0 v=1	-9.701	0.958	5.26	1994-05-18	NRO	0.069	NRO	JIA96
54	05 47 30.5	+27 08 11.4	181.754383	-0.578498	IRAS05443+2707	SiO J=1-0 v=2	-12.542	1.495	4.73	1994-05-18	NRO	0.060	NRO	JIA96
55	05 58 8.5	+17 20 58.5	191.440925	-3.42824	IRAS05552+1720	SiO J=1-0 v=1	42.246	0.215	1.17	1995-05-27	NRO	0.039	NRO	JIA96
56	05 58 8.5	+17 20 58.5	191.440925	-3.42824	IRAS05552+1720	SiO J=1-0 v=2	45.123	0.392	1.98	1995-05-27	NRO	0.043	NRO	JIA96
57	05 59 24.7	+38 25 38.1	173.239153	7.266695	IRAS05559+3825	SiO J=1-0 v=2	-32.476	1.754	3.28	1994-05-15	NRO	0.167	NRO	JIA96
58	06 04 16.7	+28 29 1.2	182.455992	3.303685	IRAS06011+2829	SiO J=1-0 v=1	13.038	2.493	13.46	1994-05-18	NRO	0.073	NRO	JIA96
59	06 04 16.7	+28 29 1.2	182.455992	3.303685	IRAS06011+2829	SiO J=1-0 v=2	18.3	0.645	5.17	1994-05-18	NRO	0.068	NRO	JIA96
60	06 20 21.2	+35 22 20.4	177.943035	9.545911	IRAS06170+3523	SiO J=1-0 v=1	22.329	0.2	0.78	1994-05-16	NRO	0.098	NRO	JIA96
61	06 20 21.2	+35 22 20.4	177.943035	9.545911	IRAS06170+3523	SiO J=1-0 v=2	21.812	0.365	1.74	1994-05-16	NRO	0.091	NRO	JIA96
62	06 21 51.7	-03 50 42	212.997355	-8.328928	IRAS06193-0349	SiO J=1-0 v=1	-5.94	2.836	9.08	1995-05-28	NRO	0.083	NRO	JIA96
63	06 21 51.7	-03 50 42	212.997355	-8.328928	IRAS06193-0349	SiO J=1-0 v=2	-5.505	3.826	10.67	1995-05-28	NRO	0.071	NRO	JIA96
64	06 26 52.6	+10 23 49.8	200.891515	-0.649705	IRAS06241+1025	29SiO J=1-0 v=0	-14.36	0.25	0.37		NRO	0.031	NRO	JIA96
65	06 26 52.6	+10 23 49.8	200.891515	-0.649705	IRAS06241+1025	SiO J=1-0 v=1	-13.655	0.717	3.16	1995-05-01	NRO	0.031	NRO	JIA96
66	06 26 52.6	+10 23 49.8	200.891515	-0.649705	IRAS06241+1025	SiO J=1-0 v=2	-13.679	0.539	1.91	1995-05-01	NRO	0.027	NRO	JIA96
67	06 35 31.9	-01 09 25.2	212.148207	-4.066389	IRAS06329-0106	SiO J=1-0 v=1	98.734	0.492	1.94	1995-05-28	NRO	0.057	NRO	JIA96
68	06 35 31.9	-01 09 25.2	212.148207	-4.066389	IRAS06329-0106	SiO J=1-0 v=2	98.531	0.439	2.3	1995-05-28	NRO	0.059	NRO	JIA96
69	06 37 29.6	+14 42 13.9	198.263264	3.634576	IRAS06346+1444	SiO J=1-0 v=1	5.076	0.948	6.2	1995-05-27	NRO	0.041	NRO	JIA96
70	06 37 29.6	+14 42 13.9	198.263264	3.634576	IRAS06346+1444	SiO J=1-0 v=2	1.916	0.282	1.55	1995-05-27	NRO	0.055	NRO	JIA96
71	06 42 15.6	-09 39 44.6	220.529066	-6.411065	IRAS06398-0936	SiO J=1-0 v=1	27.28	1.336	7.31	1995-05-28	NRO	0.044	NRO	JIA96
72	06 42 15.6	-09 39 44.6	220.529066	-6.411065	IRAS06398-0936	SiO J=1-0 v=2	25.424	0.786	2.76	1995-05-28	NRO	0.045	NRO	JIA96
73	06 52 46.9	+08 25 20	205.575552	4.125973	IRAS06500+0829	29SiO J=1-0 v=0	-10.96	1.23	2.12		NRO	0.042	NRO	JIA96
74	06 52 46.9	+08 25 20	205.575552	4.125973	IRAS06500+0829	SiO J=1-0 v=1	-10.554	13.63	68.57	1995-05-01	NRO	0.043	NRO	JIA96
75	06 52 46.9	+08 25 20	205.575552	4.125973	IRAS06500+0829	SiO J=1-0 v=2	-10.796	13.871	52.19	1995-05-01	NRO	0.046	NRO	JIA96
76	06 57 11.3	-19 19 13.9	230.861799	-7.457773	IRAS06550-1915	SiO J=1-0 v=1	18.087	0.251	1.63	1995-05-28	NRO	0.054	NRO	JIA96
77	06 57 11.3	-19 19 13.9	230.861799	-7.457773	IRAS06550-1915	SiO J=1-0 v=2	20.205	0.481	2.23	1995-05-28	NRO	0.050	NRO	JIA96
78	07 00 29.8	-15 17 8.7	227.58441	-4.949987	IRAS06582-1512	SiO J=1-0 v=1	65.697	0.284	0.87	1995-05-28	NRO	0.039	NRO	JIA96
79	07 00 29.8	-15 17 8.7	227.58441	-4.949987	IRAS06582-1512	SiO J=1-0 v=2	69.501	0.267	0.98	1995-05-28	NRO	0.039	NRO	JIA96
80	07 04 12.6	-16 35 34.4	229.159427	-4.744108	IRAS07019-1631	SiO J=1-0 v=1	52.153	0.793	1.44	1995-05-28	NRO	0.070	NRO	JIA96
81	07 04 12.6	-16 35 34.4	229.159427	-4.744108	IRAS07019-1631	SiO J=1-0 v=2	54.995	0.495	1.86	1995-05-28	NRO	0.072	NRO	JIA96
82	07 04 31.3	-08 57 13.4	222.385533	-1.192354	IRAS07021-0852	SiO J=1-0 v=1	76.962	0.319	0.49	1995-05-28	NRO	0.041	NRO	JIA96
83	07 04 31.3	-08 57 13.4	222.385533	-1.192354	IRAS07021-0852	SiO J=1-0 v=2	76.943	0.302	0.52	1995-05-28	NRO	0.040	NRO	JIA96
84	07 17 27.8	-24 17 12	237.454553	-5.48726	IRAS07153-2411	SiO J=1-0 v=1	59.996	0.291	0.62	1995-05-29	NRO	0.073	NRO	JIA96
85	07 17 27.8	-24 17 12	237.454553	-5.48726	IRAS07153-2411	SiO J=1-0 v=2	62.036	0.481	0.65	1995-05-29	NRO	0.074	NRO	JIA96
86	07 22 1.9	-14 56 56.4	229.683072	-0.182473	IRAS07197-1451	SiO J=1-0 v=1	41.994	0.924	4.66	1995-05-29	NRO	0.081	NRO	JIA96
87	07 22 1.9	-14 56 56.4	229.683072	-0.182473	IRAS07197-1451	SiO J=1-0 v=2	39.519	0.338	0.24	1995-05-29	NRO	0.079	NRO	JIA96
88	07 22 16	-18 52 14.6	233.170075	-1.979431	IRAS07200-1846	SiO J=1-0 v=1	31.512	0.757	2.18	1995-05-29	NRO	0.074	NRO	JIA96
89	07 22 16	-18 52 14.6	233.170075	-1.979431	IRAS07200-1846	SiO J=1-0 v=2	28.808	1.313	4.03	1995-05-29	NRO	0.135	NRO	JIA96
90	07 39 39.7	-10 43 7.5	228.023016	5.614682	IRAS07372-1036	SiO J=1-0 v=1	32.65	0.825	3.73	1995-05-29	NRO	0.118	NRO	JIA96
91	07 39 39.7	-10 43 7.5	228.023016	5.614682	IRAS07372-1036	SiO J=1-0 v=2	32.553	0.621	1.6	1995-05-29	NRO	0.125	NRO	JIA96
92	08 10 43.1	-15 19 46.9	235.89304	9.81556	IRAS08084-1510	SiO J=1-0 v=1	27.007	0.767	2.32	1995-05-29	NRO	0.075	NRO	JIA96
93	08 10 43.1	-15 19 46.9	235.89304	9.81556	IRAS08084-1510	SiO J=1-0 v=2	27.699	0.45	1.33	1995-05-29	NRO	0.090	NRO	JIA96
94	08 12 10.4	-23 43 47.6	243.236215	5.601886	IRAS08100-2334	SiO J=1-0 v=1	61.427	1.547	5.32	1995-05-29	NRO	0.102	NRO	JIA96
95	08 12 10.4	-23 43 47.6	243.236215	5.601886	IRAS08100-2334	SiO J=1-0 v=2	67.932	0.754	5.34	1995-05-29	NRO	0.110	NRO	JIA96
96	20 49 20.7	+53 48 1.6	91.784055	6.275884	IRAS20479+5336	SiO J=1-0 v=1	-56.913	0.199	0.07	1995-05-26	NRO	0.043	NRO	JIA96
97	20 49 20.7	+53 48 1.6	91.784055	6.275884	IRAS20479+5336	SiO J=1-0 v=2	-57.674	0.177	0.18	1995-05-26	NRO	0.052	NRO	JIA96
98	20 53 48.5	+53 13 58.8	91.764096	5.403196	IRAS20523+5302	SiO J=1-0 v=1	-65.142	0.299	0.92	1995-05-21	NRO	0.044	NRO	JIA96
99	20 53 48.5	+53 13 58.8	91.764096	5.403196	IRAS20523+5302	SiO J=1-0 v=2	-64.974	0.379	1.25	1995-05-21	NRO	0.045	NRO	JIA96
100	21 10 13.5	+52 51 1.1	93.108057	3.296651	IRAS21086+5238	29SiO J=1-0 v=0	-12.28	0.46	0.56		NRO	0.060	NRO	JIA96
101	21 10 13.5	+52 51 1.1	93.108057	3.296651	IRAS21086+5238	SiO J=1-0 v=1	-10.217	6.831	52.36	1995-05-01	NRO	0.059	NRO	JIA96
102	21 10 13.5	+52 51 1.1	93.108057	3.296651	IRAS21086+5238	SiO J=1-0 v=2	-9.678	7.303	53.34	1995-05-01	NRO	0.064	NRO	JIA96
103	21 23 9.4	+55 49 14.3	96.559518	4.00778	IRAS21216+5536	SiO J=1-0 v=1	-8.408	0.254	1.02	1995-05-21	NRO	0.044	NRO	JIA96
104	21 23 9.4	+55 49 14.3	96.559518	4.00778	IRAS21216+5536	SiO J=1-0 v=2	-10.187	0.254	0.89	1995-05-21	NRO	0.051	NRO	JIA96
105	21 35 52.7	+51 14 42.1	94.788546	-0.614392	IRAS21341+5101	SiO J=1-0 v=1	1.446	0.515	3.33	1995-05-22	NRO	0.078	NRO	JIA96
106	21 35 52.7	+51 14 42.1	94.788546	-0.614392	IRAS21341+5101	SiO J=1-0 v=2	-6.554	1.051	2.91	1995-05-22	NRO	0.068	NRO	JIA96
107	21 46 52.8	+60 13 48.9	101.865557	5.141579	IRAS21453+5959	SiO J=1-0 v=1	-45.267	0.434	2.05	1995-05-22	NRO	0.068	NRO	JIA96
108	21 46 52.8	+60 13 48.9	101.865557	5.141579	IRAS21453+5959	SiO J=1-0 v=2	-44.802	0.586	1.37	1995-05-22	NRO	0.076	NRO	JIA96
109	21 46 52.7	+64 36 6.1	104.711434	8.477273	IRAS21456+6422	29SiO J=1-0 v=0	-45.28	0.69	0.44		NRO	0.076	NRO	JIA96
110	21 46 52.7	+64 36 6.1	104.711434	8.477273	IRAS21456+6422	SiO J=1-0 v=1	-45.755	4.855	27.75	1995-05-01	NRO	0.074	NRO	JIA96
111	21 46 52.7	+64 36 6.1	104.711434	8.477273	IRAS21456+6422	SiO J=1-0 v=2	-46.791	9.825	34.71	1995-05-01	NRO	0.081	NRO	JIA96
112	21 52 19.5	+62 48 38.9	104.022801	6.715154	IRAS21509+6234	SiO J=1-0 v=1	-69.07	0.177	1.05	1995-05-22	NRO	0.059	NRO	JIA96
113	21 52 19.5	+62 48 38.9	104.022801	6.715154	IRAS21509+6234	SiO J=1-0 v=2	-69.647	0.51	1.55	1995-05-22	NRO	0.055	NRO	JIA96
114	21 53 46.5	+60 32 16.1	102.722188	4.838538	IRAS21522+6018	SiO J=1-0 v=1	22.397	0.448	2	1995-05-22	NRO	0.074	NRO	JIA96
115	21 53 46.5	+60 32 16.1	102.722188	4.838538	IRAS21522+6018	SiO J=1-0 v=2	20.058	1.322	2.98	1995-05-22	NRO	0.069	NRO	JIA96
116	21 58 1.6	+56 44 49.6	100.811248	1.516638	IRAS21563+5630	29SiO J=1-0 v=0	-12.11	0.56	1.02		NRO	0.069	NRO	JIA96
117	21 58 1.6	+56 44 49.6	100.811248	1.516638	IRAS21563+5630	SiO J=1-0 v=1	-11.285	6.611	38.26	1995-05-01	NRO	0.065	NRO	JIA96
118	21 58 1.6	+56 44 49.6	100.811248	1.516638	IRAS21563+5630	SiO J=1-0 v=2	-5.519	7.717	37.26	1995-05-01	NRO	0.079	NRO	JIA96
119	22 12 15.5	+51 35 3.4	99.440535	-3.877409	IRAS22103+5120	29SiO J=1-0 v=0	-51.15	0.34	0.28		NRO	0.052	NRO	JIA96
120	22 12 15.5	+51 35 3.4	99.440535	-3.877409	IRAS22103+5120	SiO J=1-0 v=1	-50.37	2.155	15.17	1995-05-01	NRO	0.060	NRO	JIA96
121	22 12 15.5	+51 35 3.4	99.440535	-3.877409	IRAS22103+5120	SiO J=1-0 v=2	-50.289	1.732	11.94	1995-05-01	NRO	0.048	NRO	JIA96
122	22 41 27.1	+56 39 8.3	105.745357	-1.818489	IRAS22394+5623	SiO J=1-0 v=1	-26.424	0.906	2.18	1995-05-21	NRO	0.062	NRO	JIA96
123	22 41 27.1	+56 39 8.3	105.745357	-1.818489	IRAS22394+5623	SiO J=1-0 v=2	-26.319	0.875	2.32	1995-05-21	NRO	0.060	NRO	JIA96
124	22 48 14.2	+69 58 29.2	112.688613	9.592411	IRAS22466+6942	SiO J=1-0 v=1	-48.217	0.332	0.32	1995-05-21	NRO	0.062	NRO	JIA96
125	22 48 14.2	+69 58 29.2	112.688613	9.592411	IRAS22466+6942	SiO J=1-0 v=2	-47.897	0.185	0.1	1995-05-21	NRO	0.060	NRO	JIA96
126	23 58 25.1	+51 23 21.9	114.561641	-10.618604	IRAS23558+5106	29SiO J=1-0 v=0	24.71	1.89	2.44		NRO	0.117	NRO	JIA96
127	23 58 25.1	+51 23 21.9	114.561641	-10.618604	IRAS23558+5106	SiO J=1-0 v=1	25.311	34.34	183	1995-05-01	NRO	0.120	NRO	JIA96
128	23 58 25.1	+51 23 21.9	114.561641	-10.618604	IRAS23558+5106	SiO J=1-0 v=2	27.844	55.177	324.77	1995-05-01	NRO	0.136	NRO	JIA96

Distribution of sources in all sky (l,b)

Distribution of sources in all sky using Aladin

Tip: Click on some source to get more informaiton

Distribution of sources in IRAS color-color diagram

Tip: Use "Box select" or "Lasso select" to display colour-selected sources in Aladin all-sky view

Tip: Click on some source to look at the different surveys. You must select some surveys in previous page at "View images"

Original color diagram is taken form van der Veen & Habing (1987)

Type	Description
I	Oxygen-rich non-variable stars without circumstellar shells
II	Variable stars with "young" O-rich circumstellar shells
IIIa	Variable stars with more evolved O-rich circumstellar shells
IIIb	Variable stars with thick O-rich circumstellar shells
IV	Variable stars with very thick O-rich circumstellar shells
V	Planetary nebulae and non- variable stars with very cool circumstellar shells
VIa	Variable stars with relatively cold dust at large distances; a significant part of the stars is carbon-rich
VIb	Variable stars with relatively hot dust close to the star and relatively cold dust at large distances; Some of the objects have proven to be O-rich
VII	Variable stars with more evolved C-rich circumstellar shells
VIII	Different sort of objects

Distribution of the detection velocities versus galactic longitude from JIA96

Tip: Use "Box select" or "Lasso select" to display velocity-selected sources in Aladin all-sky view

Tip: Click on some source to look at the different surveys. You must select some surveys in previous page at "View images"

Longitude-Velocity Map is taken form Dame, Hartmann & Thaddeus (2001)

Distribution of sources from JIA96 in (l,b) histograms

Display associated data

Group name
Different Line detections
IRAS source	IRAS coordinates (RA, Dec)	IRAS source distance (arcsec)	IRAS flux density (F12,F25,F60,F100)
2MASS source	2MASS coordinates (RA, Dec)	2MASS source distance (arcsec)	2MASS magnituted (J,H,K)
GCVS source	GCVS coordinates (RA, Dec)	GCVS source distance (arcsec)	GCVS parameters
WISE source	WISE coordinates (RA, Dec)	WISE source distance (arcsec)	WISE magnitudes (w1, w2, w3, w4)
Akari IRC source	Akari IRC coordinates (RA, Dec)	Akari IRC source distance (arcsec)	Akari IRC fluxes (S09, S18)
Akari FIS source	Akari FIS coordinates (RA, Dec)	Akari FIS source distance (arcsec)	Akari FIS fluxes (S65, S90, S140, S160)
Continuum source	Continuum coordinates (RA, Dec)	Continuum source distance (arcsec)	Continuum parameters
Bolocam GPS	BGPS coordinates (RA, Dec)	BGPS source distance (arcsec)	BGPS parameters
EGO source	EGO coordinates (RA, Dec)	EGO source distance (arcsec)	EGO parameters
Select all	Select all	Select all	Select all

View images

DSS (optical)	SDSS (optical+NIR)	2MASS (JHK)	WISE (4-22 um)	IRAC (3-8 um)	GLIMPSE 360 (3.6-4.5 um)
AKARI color (60-160 um)	PACS color (70-160 um)	SPIRE color (250-500 um)	ATLASGAL (870 um)	ATLASGAL+Planck (870 um)	Bolocam (1.1 mm)
NVSS (1.4 GHz)	Image size: arcsec (default is 120 arcsec)
	Image size: arcsec (default is 120 arcsec)

DSS colored	2MASS colored	WISE colored
SDSS color	IRAC color I1,I2,I4	GLIMPSE 360
PACS color (70-160 um)	SPIRE color (250-500 um)	NVSS (1.4GHz)
ATLASGAL 870 um	ATLASGAL 870 um + Planck	Bolocam 1.1 mm
UKIDSS K	2MASS K

select MAX(sio_data.ra_hms) as ra_hms,MAX(sio_data.dec_dms) as dec_dms,MAX(sio_data.source_name) as source_name,MAX(sio_data.ra) as ra,MAX(sio_data.dec) as dec,MAX(sio_data.l) as l,MAX(sio_data.b) as b,MAX(sio_data.vlow) as vlow,MAX(sio_data.vup) as vup,MAX(sio_data.vpeak) as vpeak,MAX(sio_data.vpeak_e) as vpeak_e,MAX(sio_data.vpeak2) as vpeak2,MAX(sio_data.vpeak2_e) as vpeak2_e,MAX(sio_data.dv) as dv,MAX(sio_data.other_name) as other_name,MAX(sio_data.peak) as peak,MAX(sio_data.peak_e) as peak_e,MAX(sio_data.peak2) as peak2,MAX(sio_data.peak2_e) as peak2_e,MAX(sio_data.int) as int,MAX(sio_data.int_e) as int_e,MAX(sio_data.rms) as rms,MAX(sio_data.date) as date,MAX(sio_data.date2) as date2,MAX(sio_data.telescope_ref) as telescope_ref,MAX(sio_data.units) as units,MAX(sio_data.beam) as beam,MAX(sio_data.ref) as ref,MAX(sio_data.list_ref) as list_ref,MAX(sio_data.ascii) as ascii,MAX(sio_data.image) as image,MAX(sio_data.id) as id,MAX(sio_data.date_txt) as date_txt,MAX(sio_data.line) as line FROM sio_data  WHERE ref ilike 'JIA96' AND detected=true AND hide=false GROUP BY ref

select sio_data.ra_hms,sio_data.dec_dms,sio_data.source_name,sio_data.ra,sio_data.dec,sio_data.l,sio_data.b,sio_data.vlow,sio_data.vup,sio_data.vpeak,sio_data.vpeak_e,sio_data.vpeak2,sio_data.vpeak2_e,sio_data.dv,sio_data.other_name,sio_data.peak,sio_data.peak_e,sio_data.peak2,sio_data.peak2_e,sio_data.int,sio_data.int_e,sio_data.rms,sio_data.date,sio_data.date2,sio_data.telescope_ref,sio_data.units,sio_data.beam,sio_data.ref,sio_data.list_ref,sio_data.ascii,sio_data.image,sio_data.id,sio_data.date_txt,sio_data.line FROM sio_data   WHERE ref ilike 'JIA96' AND detected=true AND hide=false ORDER BY detected DESC,id