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Observations and Data Reduction

A SEARCH FOR NHtex2html_wrap_inline952 IN THE LARGE MAGELLANIC CLOUD

JÓÌrgen Osterberg, Lister Staveley-Smith, Joel M. Weisberg, John M. Dickey, Ulrich Mebold, PASA, 14 (3), 246
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Next Section: The Target Positions
Title/Abstract Page: A SEARCH FOR NH
Previous Section: Introduction
Contents Page: Volume 14, Number 3

Observations and Data Reduction

tex2html_wrap_inline972

The observations were taken during the period 1994 February 12-21 using the Parkes telescope. The feed at the frequency of the observed tex2html_wrap_inline972 (J,K)Òš= (1,1) transition (23.694495 GHz) only illuminates the inner 44 m of the telescope, resulting in a FWHP beamwidth of 1'.4 (20 pc at the LMC distance of 50 kpc). The efficiency of the Parkes telescope at this frequency is tex2html_wrap_inline1012. The receiver was a single-channel maser. Owing to relatively high humidity at the time of the observations, typical system temperatures were 130 to 160 K.

Òš

=1mm

no.Positionrms Source Type Associated Objects Reference
tex2html_wrap_inline1014(J2000)tex2html_wrap_inline1016(J2000)mK
1 05Òš36Òš03.75 -69Òš30Òš24.02 11.9 HI condensation (4)
2 05Òš37Òš23.98 -69Òš33Òš22.63 17.6 HI condensation (4)
3 05Òš37Òš47.6 -69Òš10Òš21.0 23.8 HI condensation (4)
4 05Òš39Òš17.0 -69Òš03Òš20.0 19.0 HI condensation (4)
5 05Òš39Òš34.57 -69Òš45Òš33.6 9.21 CO condensation LI-LMCÒš1501 (3)
6 05Òš39Òš52.1 -69Òš45Òš10 21.8 Continuum Source (1)
7 05Òš39Òš58.8 -70Òš10Òš57.6 24.6 CO condensation Molecular Cloud Complex 35 (2)
8 05Òš40Òš03.9 -69Òš37Òš50.37 8.33 HI condensation (4)
9 05Òš40Òš06.5 -69Òš44Òš44 11.8 IRAS Point Source LI-LMCÒš1518 (1)
10 05Òš40Òš09.0 -69Òš44Òš34.0 15.9 CO condensation (1)
11 05Òš40Òš37.05 -70Òš10Òš40.37 10.5 CO condensation LI-LMCÒš1541 (3)
12 05Òš42Òš58.9 -69Òš45Òš12.5 12.5 CO condensation LI-LMCÒš1609 (3)
Table 1: Observed Positions in the 30 Dor Region and around N159

(1) Hunt & Whiteoak (1994); (2) Cohen et al. (1988); (3) Israel et al. (1993); (4) This paper

The AT autocorrelator was configured to process two bands, each with 2048 channels. The first band was at the (J,K)Òš= (1,1) transition, and the second band was used to observe the (2,2) transition at 23.722633 GHz, which is not discussed any further. The channel spacing was 7.8 kHz (0.1 kmstex2html_wrap_inline1018) with a total bandwidth of 16 MHz (202.4 kmstex2html_wrap_inline1018). At the start or end of every observing day, strong Galactic sources were observed for calibration purposes. These sources were near the outflow region associated with the Herbig Ae star RCrA (Anglada et al 1989) and the HII region OMC-2 in Orion (Batchelor et al. 1977). The data for each position were averaged with a weight proportional to the inverse square of the system temperature for each integration. Baselines were fitted and subtracted and a Gaussian smooth was applied resulting in a velocity resolution of 0.4 kmstex2html_wrap_inline1018. The first two positions (Nos. 3 & 10 in Table 1) were observed in beam-switching mode, using a 1 Hz synchronous waveguide switch to alternate between two beams separated by 4'.5 on the sky. However, the remaining positions were observed in position-switching mode where each object was observed in a sequence consisting of 5 min on source and 5 min on a nearby `blank-sky' region. The total integration times were typically 3 hours for each pointing.

HI

We briefly describe the tex2html_wrap_inline102621 cm HI data used to help choose our tex2html_wrap_inline972 target pointings. The data consists of five sets of 12-hr observations obtained in 1993 January, March, May and July with the Australia Telescope Compact Array. The uv-plane was well sampled to distances of 7 ktex2html_wrap_inline1026 (1.5 km), resulting in a synthesised FWHP beamwidth of 45'' (11 pc). We used a correlator configuration with a bandwidth of 4 MHz, divided in 1024 channels, resulting in a channel spacing of 0.8 kmstex2html_wrap_inline1018. The center frequency was 1419 MHz, corresponding to a center heliocentric velocity of 297 kmstex2html_wrap_inline1018. Three adjacent fields, listed in Table 2 were observed. Each field has an extent limited by the primary antenna beamwidth of 34' (490 pc) FWHP, resulting in a combined field of approximately tex2html_wrap_inline1040 (tex2html_wrap_inline1042 pc) centred approximately 12' (170 pc) SSW of 30 Dor. The HI spectra used in this paper were extracted from the resulting data cube.

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=1mm

Field-No.Positioncentred on
tex2html_wrap_inline1014(J2000) tex2html_wrap_inline1016(J2000)
1 05Òš35Òš27.9 -69Òš16Òš31.6 SN1987A
2 05Òš38Òš47.0 -69Òš05Òš50.1 30 Doradus
3 05Òš38Òš47.0 -69Òš27Òš49.8 Giant Molecular Cloud
Table 2: Phase centres of fields, observed in HI with the Compact Array


Next Section: The Target Positions
Title/Abstract Page: A SEARCH FOR NH
Previous Section: Introduction
Contents Page: Volume 14, Number 3

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