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2 Observation and data analysis

Far-infrared data:

we searched for faint, small, cold sources with no IRAS associations in the region $95\hbox{$^\circ$ }<l<115\hbox{$^\circ$ }$, $10\hbox{$^\circ$ }<b<20\hbox{$^\circ$ }$, where the ISOSS survey has over 50% coverage. ISOSS 170 $\mu $m data were smoothed to the IRAS ISSA (Wheelock et al. 1994) resolution, and processed according to Tóth et al. (2000) and Hotzel (2001). Sources were selected using the following criteria: a size $FWHM \le 6\hbox{$^\prime$ }$, a 170 $\mu $m source surface brightness $8\pm 5$ MJy sr-1, and a background corrected colour parameter $CP=6.4\pm 0.5$, no associations in the IRAS Point Source Catalogue, or in the IRAS Faint Source Catalogue within 5 $\hbox{$^\prime$ }$, and no excess in the IRAS ISSA maps above 0.6 MJy sr-1. We located 50 objects fullfilling our criteria. ISOSS J20246+6540 was also detected as an $I_{170}(\rm peak)= 4$ MJy sr-1 (>$4\sigma $) pointlike source at RA(2000 $)=20^{\rm h}$24$^{\rm m}$36$^{\rm s}$ Dec(2000 $)=+65\hbox{$^\circ$ }$40 $\hbox{$^\prime$ }$ ( $l=99.8\hbox{$^\circ$ }$, $b=15.7\hbox{$^\circ$ }$). with an unsmoothed ${\it FWHM} \le 150\hbox{$^{\prime\prime}$ }$. We note that the unsmoothed ISOSS point-spread function is nearly Gaussian with $FWHM\approx 130\hbox{$^{\prime\prime}$ }$.

Optical data:

the Digital Sky Survey (DSS2) blue plates indicated optical counterparts for 41 of the 50 ISOSS sources, out of which 5 isolated, globule like sources were found. Three of them bear opaque cores resembling the globule of Dickman & Clemens (1983) and two are without any opaque core: ISOSS J20215+6820 and ISOSS J20246+6540. Table 1 lists (1) ISOSS names, (2, 3) galactic coordinates, (4) optical dimensions in arcminutes, (5) the distance to the nearest cloud neighbours
 

 
Table 1: Five ISOSS globules and their nearest cloud neighbours, CB88: Clemens & Barvainis (1988), YDM97: Yonekura (1997) (*) refers to an unnumbered peak, LM99: Lee & Myers (1999).
ISOSS name l b $a\times b$ nearest
  [ $\hbox{$^\circ$ }$] [ $\hbox{$^\circ$ }$] [ $\hbox{$^\prime$ }$] neighbour
ISOSS J20180+6345 97.71 15.29 $5\times 3$ 8'CB88 #219
ISOSS J20215+6820 102.00 17.34 $3\times 2$ 45'YDM97 #4
ISOSS J20246+6540 99.79 15.69 $4\times 2$ 20'YDM97(*)
ISOSS J20380+6352 99.05 13.51 $5\times 2$ 12'CB88 #224
ISOSS J20474+6014 96.72 10.46 $5\times 5$ 14'LM99 #349


Further 8 sources were associated with complexes of reflecting clouds. Detailed optical study of the 5 globule like clouds and a study of statistical issues will be given elsewhere. As an example we present results on ISOSS J20246+6540 which was studied using DSS2 blue and red images. In order to make surface brightness maps of ISOSS J20246+6540, stars were removed from the optical images by substituting the average surrounding photographical density value.

Radio spectroscopic measurements:

the J=(1-0) and (2-1) rotational lines of CO, 13CO and C18O were measured in Aug. 1998 with the IRAM-30 m telescope. A $4.5\hbox{$^\prime$ }\times 4.5\hbox{$^\prime$ }$ region centered on ISOSS 20246+6540 was mapped in on-the-fly mode in 12CO(1-0), 12CO(2-1) and 13CO(1-0) with angular resolutions of 22 $^{\prime\prime}$, 11 $^{\prime\prime}$, 22 $^{\prime\prime}$ respectively. Pointed measurements were performed in all the above mentioned transitions at the 13CO(1-0) peak position (22$^{\rm h}$24$^{\rm m}$46$^{\rm s}$, 65$^\circ$40$^\prime$01 $^{\prime\prime}$). Spectral resolutions of 0.1, 0.05 and 0.03 km s-1 were used. These spectra are shown in Fig. 1.
  \begin{figure}
\par\includegraphics[width=18cm,clip]{H3949F1.ps}
\end{figure} Figure 1: CO spectra at the 13CO(1-0) peak, (2-1) lines are overlaid as filled histograms. a) 12CO(1-0) and (2-1) spectra. b) 13CO(1-0) and (2-1) spectra. c) C18O(1-0) and (2-1) spectra.

The lines are narrow with a FWHM of $\le$0.5 km s-1. The results of the 1998 C18O pointed measurements were confirmed in Sep. 2000 when also the CS(2-1) and (3-2) as well as the HCO+(1-0) and (2-1) transitions were observed with the IRAM-30 telescope. The C18O, CS(2-1) and HCO+(1-0) lines were detected with S/N>5 and well resolved with the 0.03 km s-1 spectral channels. The data were calibrated to the scale of corrected antenna temperature, $T^*_{\rm A}$, by observing loads at ambient and cold temperature, as in the conventional "chopper-wheel'' calibration for millimetre wavelength observations. The data were converted to the main-beam scale by applying the relation $T_{\rm MB} =
T^*_{\rm A} (F_{\rm eff}/B_{\rm eff})$. The values for the main-beam efficiency, $B_{\rm eff}$, are 0.70 and 0.42 (July 1998), and 0.75 and 0.53 (September 2000), and the values for the forward efficiency, $F_{\rm eff}$, are 0.92 and 0.85 for CO(1-0) and CO(2-1), respectively. We checked the calibration by observing the standard sources DR 21 and W3OH and found it always to be better than 20%. Results are listed in Table 2.
 

 
Table 2: Radio spectroscopy results for pointed measurements towards the NE lobe, $\Delta T_{\rm rms}$ is given in parentheses after $T_{\rm MB}$, errors of the Gaussian line fit are given in parentheses for FWHM and $v_{\rm LSR}$, asterisk marks selfabsorbed lines.
line $T_{\rm MB}$ FWHM $v_{\rm LSR}$
  [K] [km s-1] [km s-1]
12CO(1-0) 6.7* (0.11) 0.43 (0.01) -2.70 (0.01)
12CO(2-1) 5.41 (0.17) 0.47 (0.01) -2.69 (0.01)
13CO(1-0) 4.3* (0.14) 0.32 (0.03) -2.68 (0.01)
13CO(2-1) 3.60 (0.08) 0.31 (0.01) -2.70 (0.01)
C18O(1-0) 0.11 (0.02) 0.25 (0.02) -2.68 (0.01)
C18O(2-1) 0.10 (0.03) 0.24 (0.03) -2.76 (0.02)
CS(2-1) 0.09 (0.02) 0.25 (0.02) -2.69 (0.01)
HCO+(1-0) 0.20 (0.03) 0.29 (0.03) -2.70 (0.01)



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