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Figure 1:
Objects in the CRL 2136 region: the upper panel shows
the positions of radio sources 3 and 4 (filled circles),
infrared source 1 (filled square), and the class II CH3OH maser
(filled pentagon). The three little stars mark the positions
from which of 1665 MHz RCP maser emission arises and the circles mark
LCP emission. For the OH emission, the symbol sizes reflect the
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Figure 2: Radio source 4 at 43.3 GHz: the contours represent 5, 7, 9, and 11 times the 2.7 mJy beam-1 rms noise in our 43.3 GHz map. The dotted ellipse in the lower left corner represents the FWHM size of the Gaussian restoring beam, while the full line ellipses represent the maximum and nominal FWHM source size from JMFIT (see discussion in text). Angular offsets are relative to the position given in Table 1. |
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Figure 3: Top panel: H2O spectrum taken at the Effelsberg 100 m telescope on 2002 December 26. Second panel from top: VLA H2O spectrum made from our 1992 May 19 data at the pixel with maximum emission. In the third panel from top the intensity axis is expanded to show the extremely weak emission at the lowest and highest velocities. The arrows show the velocity ranges over which maps of integrated emission, marked by the rectangles in Fig. 4 were produced. The lower panel shows the RCP and LCP emission of the OH 1665 MHz line published by Argon et al. (2000). For details of how the spectrum was formed see this reference. The dotted vertical lines mark the FWHM linewidths of various molecular species mapped by van der Tak et al. (2000b), who determine a centroid LSR velocity of 22.8(0.1) km s-1. The solid line marks the velocity of the single, narrow 6.7 GHz CH3OH maser feature (Caswell et al. 1995). |
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Figure 4:
Area containing the H2O maser emission, indicated
by the dashed rectangle in Fig. 1.
The error bars in the upper panel
give the positions of H2O masers determined from channel by
channel fitting of the H2O data cube. The centers of the full line
rectangles are the positions of the centroid positions of
maps integrated over the
velocity ranges given (and indicated in Fig. 3); the sizes corresponds to the |
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Figure 5: The radio-to-submillimeter-wavelength spectral energy distributions of CRL 2136 IRS 1/RS 4 ( full dots) and Orion source I ( open dots). The full line represents a fit to our 4.9 to 43.3 GHz data for RS 4, while the dashed line is a fit to the submillimeter data of Kastner et al. (1994). Error bars of flux densities are smaller than or comparable to the symbol sizes. |
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