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TIME MONITORING OBSERVATIONS OF SiO J = 2 - 1 AND J = 3 - 2 LINES TOWARD ORION KL
We have carried out time monitoring observations of the {sup 28}SiO v = 0, 1, 2, J = 2 - 1, {sup 28}SiO v = 0, 1, 2, J = 3 - 2, and {sup 29}SiO v = 0, J = 3 - 2 transitions in Orion KL with the 14 m radio telescope at Taeduk Radio Astronomy Observatory. The pair of J = 2 - 1 and J = 3 - 2 transition...
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Published in: | The Astronomical journal 2010-01, Vol.139 (1) |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Online Access: | Get full text |
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Summary: | We have carried out time monitoring observations of the {sup 28}SiO v = 0, 1, 2, J = 2 - 1, {sup 28}SiO v = 0, 1, 2, J = 3 - 2, and {sup 29}SiO v = 0, J = 3 - 2 transitions in Orion KL with the 14 m radio telescope at Taeduk Radio Astronomy Observatory. The pair of J = 2 - 1 and J = 3 - 2 transitions was simultaneously observed from 1999 January to 2001 March. Each transition shows different characteristics. Both the v = 1, J = 2 - 1, and J = 3 - 2 masers show a relatively stable double-peaked profile and little variation in intensity. The {sup 28}SiO v = 2, J = 3 - 2 maser presents the most active intensity variations including a disappearance on 2000 February 17 and 2001 February 16. The v = 2, J = 3 - 2 maser may trace the closest region to the central young stellar object and results in the strongest variations of intensity and line profile. The v = 2, J = 2 - 1 maser was not detected in the monitoring. The {sup 28}SiO v = 0, J = 3 - 2 lines showed a large variation of peak intensity compared with {sup 28}SiO v = 0, J = 2 - 1 that might be due to partial masing. The different observational results of {sup 28}SiO v = 0, 1, J = 2 - 1, {sup 28}SiO v = 0, 1, 2, J = 3 - 2, and {sup 29}SiO v = 0, J = 3 - 2 transitions might reflect that individual transitions trace different portions of gas. |
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ISSN: | 1538-3881 1538-3881 |
DOI: | 10.1088/0004-6256/139/1/302;COUNTRYOFINPUT:INTERNATIONALATOMICENERGYAGENCY(IAEA) |