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Table B.2:

Parameters of the 6 GHz CH3OH maser (Class II) detected in high sources with the Effelsberg 100-m telescope.

Source 		$V_{\rm LSR}$a $\int F_\nu {\rm d}V$ V $\Delta V$ $F_{\rm peak}$
  (km s-1) (Jy km s-1) (km s-1) (km s-1) (Jy)
00338+6312* -17.5f $6.4\pm0.1$ $-23.030\pm0.001$ $0.287\pm0.003$ 21.0
    $2.8\pm0.2$ $-22.64\pm0.02$ $0.74\pm0.04$ 3.62
05274+3345 -3.8 $2.40\pm0.04$ $0.324\pm0.002$ $0.331\pm0.006$ 6.81
    $10.07\pm0.04$ $1.244\pm0.003$ $0.584\pm0.004$ 16.2
    $16.59\pm0.04$ $1.609\pm0.0005$ $0.349\pm0.003$ 44.6
    $1.15\pm0.03$ $2.140\pm0.003$ $0.202\pm0.005$ 5.35
05358+3543* -17.6d $18\pm1$ $-13.8\pm0.1$ $0.5\pm0.1$ 34.4
    $15\pm1$ $-13.2\pm0.1$ $0.3\pm0.1$ 45.7
    $19\pm1$ $-12.8\pm0.1$ $0.3\pm0.1$ 51.8
    $1.5\pm1$ $-11.5\pm0.1$ $3.0\pm0.1$ 0.47
05480+2545 -9.3b $0.98\pm0.03$ $-15.250\pm0.004$ $0.238\pm0.009$ 3.88
    $3.09\pm0.04$ $-14.730\pm0.003$ $0.426\pm0.007$ 6.81
    $0.27\pm0.03$ $-13.99\pm0.02$ $0.30\pm0.05$ 0.84
    $6.15\pm0.04$ $-4.8940\pm0.0001$ $0.340\pm0.003$ 17.0
06055+2039* 8.8c $0.2\pm0.02$ $3.9\pm0.02$ $0.38\pm0.06$ 0.5
    $0.78\pm0.02$ $5.496\pm0.006$ $0.47\pm0.02$ 1.57
06056+2131 2.6 $3.7\pm0.2$ $8.8\pm0.1$ $0.3\pm0.1$ 12.7
    $2.2\pm0.2$ $9.6\pm0.1$ $0.3\pm0.1$ 7.26
    $0.7\pm0.2$ $10.6\pm0.1$ $1.1\pm0.1$ 0.605
06058+2138* 3.1c $4.1\pm0.2$ $8.470\pm0.009$ $0.43\pm0.03$ 9.10
    $5.0\pm0.1$ $9.446\pm0.001$ $0.386\pm0.008$ 12.2
    $373.0\pm0.2$ $10.590\pm0.001$ $0.784\pm0.001$ 447
    $17.7\pm0.1$ $11.45\pm0.01$ $0.212\pm0.002$ 78.7
06061+2151 -0.6 $0.51\pm0.02$ $-5.564\pm0.003$ $0.232\pm0.008$ 2.08
    $0.17\pm0.03$ $-5.05\pm0.06$ $0.7\pm0.2$ 0.227
    $0.30\pm0.02$ $10.63\pm0.03$ $0.74\pm0.07$ 0.380
06117+1350* 17.9c $2.2\pm0.8$ $14.6\pm0.1$ $0.2\pm0.1$ 9.5
    $25.0\pm0.8$ $15.1\pm0.1$ $0.5\pm0.1$ 47.8
    $4.6\pm0.8$ $15.7\pm0.1$ $0.5\pm0.1$ 8.2
17571-2328 - $0.85\pm0.01$ $143.80\pm0.03$ $1.16\pm0.05$ 0.686
    $0.29\pm0.03$ $147.30\pm0.02$ $0.37\pm0.05$ 0.731
17589-2312 21.1c $1.5\pm0.5$ $13.1\pm0.1$ $1.0\pm0.1$ 1.44
    $7.1\pm0.5$ $14.7\pm0.1$ $0.4\pm0.1$ 19.1
    $9.6\pm0.5$ $15.2\pm0.1$ $0.2\pm0.1$ 39.3
    $54.7\pm0.5$ $16.0\pm0.1$ $0.8\pm0.1$ 62.5
    $2.21\pm0.06$ $17.430\pm0.006$ $0.48\pm0.02$ 4.30
    $2.59\pm0.04$ $18.7000\pm0.0008$ $0.239\pm0.005$ 10.2
    $3.80\pm 0.05$ $19.540\pm0.003$ $0.436\pm0.008$ 8.19
    $1.08\pm0.07$ $24.60\pm0.04$ $1.19\pm0.06$ 0.847
    $15.60\pm0.07$ $25.4500\pm0.0008$ $0.569\pm0.002$ 25.8
    $26.07 \pm0.05$ $26.4800\pm0.0009$ $0.937\pm0.002$ 26.1
    $10.0\pm 0.4$ $28.07\pm0.02$ $1.27\pm0.04$ 7.37
    $7.8 \pm0.2$ $28.630\pm0.003$ $0.422\pm0.007$ 17.2
18048-2019 49.1 $15.3\pm0.6$ $41.40\pm 0.110$ $0.6142\pm 0.110$ 23.3
    $17.7\pm0.6$ $42.1\pm0.1$ $0.6\pm0.1$ 27.3
    $5.9\pm0.6$ $43.2\pm0.1$ $0.4\pm0.1$ 15.5
    $0.7\pm0.6$ $44.2\pm0.1$ $1.0\pm0.1$ 0.629
    $4.1\pm0.4$ $45.8\pm0.1$ $1.9\pm0.1$ 2.03
    $5.6\pm0.4$ $46.8\pm0.1$ $0.8\pm0.1$ 6.67
    $5.2\pm0.4$ $47.1\pm0.1$ $0.3\pm0.1$ 14.6
    $1.4\pm0.4$ $48.1\pm0.1$ $0.7\pm0.1$ 1.82
    $1.0\pm0.4$ $50.4\pm0.1$ $1.0\pm0.1$ 1.00
18089-1732 32.9 $2.8\pm0.1$ $29.59\pm0.08$ $3.4\pm0.2$ 0.774
    $0.13\pm0.01$ $29.210\pm0.004$ $0.111\pm0.003$ 1.07
    $0.94\pm0.03$ $30.210\pm0.003$ $0.270\pm0.009$ 3.26
    $3.3\pm0.7$ $31.9\pm0.1$ $0.7\pm0.1$ 4.50
    $4.7\pm0.7$ $32.8\pm0.1$ $0.5\pm0.1$ 9.18
    $24.7\pm0.7$ $33.7\pm0.1$ $0.5\pm0.1$ 50.3
    $3.8\pm0.7$ $34.7\pm0.1$ $0.4\pm0.1$ 8.22

  $1.9\pm0.7$ $36.5\pm0.1$ $0.5\pm0.1$ 3.87
  32.9 $5.3\pm0.7$ $37.9\pm0.1$ $1.1\pm0.1$ 4.61
    $5.8\pm 0.7$ $38.7\pm0.1$ $0.3\pm0.1$ 17.2
    $27.1\pm0.7$ $39.2\pm0.1$ $0.5\pm0.1$ 55.4
    $3.6\pm0.7$ $42.4\pm0.1$ $10.4\pm0.1$ 0.321
18102-1800 21.1d $3.8\pm0.1$ $21.6\pm0.1$ $0.5\pm0.1$ 7.05
    $1.5\pm0.1$ $23.1\pm0.1$ $0.4\pm0.1$ 3.09
    $2.9\pm0.1$ $24.0\pm0.1$ $0.6\pm0.1$ 4.23
    $1.40\pm0.04$ $25.020\pm0.006$ $0.49\pm0.02$ 2.69
    $1.11\pm0.04$ $25.640\pm0.007$ $0.46\pm0.02$ 2.28
    $0.19\pm0.03$ $27.22\pm0.03$ $0.51\pm0.1$ 0.35
18134-1942 10.5 $2.28\pm0.08$ $4.877\pm0.004$ $0.28\pm0.01$ 7.56
    $42\pm3$ $6.4\pm0.1$ $1.1\pm0.1$ 35.0
    $37\pm3$ $6.6\pm0.1$ $0.3\pm0.1$ 107.
    $40\pm3$ $7.7\pm0.1$ $0.4\pm0.1$ 83.2
    $8\pm3$ $8.3\pm0.1$ $0.5\pm0.1$ 16.7
    $14\pm3$ $8.8\pm0.1$ $0.4\pm0.1$ 31.1
    $3\pm3$ $13.3\pm0.1$ $0.5\pm0.1$ 5.64
    $1.6\pm0.3$ $14.4\pm0.1$ $0.5\pm0.1$ 3.01
    $7.3\pm0.4$ $14.7\pm0.1$ $0.4\pm0.1$ 16.4
    $2.5\pm0.4$ $15.4\pm0.1$ $0.4\pm0.1$ 5.26
    $1.3\pm0.4$ $16.1\pm0.1$ $0.4\pm0.1$ 3.20
18151-1208 32.8 $11.75\pm0.09$ $27.630\pm0.002$ $0.323\pm0.003$ 34.1
    $31.16\pm0.08$ $28.000\pm0.003$ $0.258\pm0.007$ 113.
    $0.57\pm0.05$ $28.990\pm0.007$ $0.30\pm0.03$ 1.78
18159-1648 22.1 $0.20\pm0.04$ $22.7\pm0.1$ $1.2\pm0.4$ 0.154
18236-1205 26.2 $0.9\pm0.2$ $25.1\pm0.1$ $1.1\pm0.1$ 0.746
    $1.8\pm0.2$ $25.2\pm0.1$ $0.5\pm0.1$ 3.37
    $3.6\pm0.2$ $27.2\pm0.1$ $0.5\pm0.1$ 6.19
    $3.0\pm0.2$ $28.7\pm0.1$ $0.5\pm0.1$ 5.98
    $0.3\pm0.2$ $29.9\pm0.1$ $0.9\pm0.1$ 0.341
18247-1147 55.9 $0.34\pm0.02$ $116.300\pm0.005$ $0.23\pm0.01$ 1.38
    $0.31\pm0.02$ $123.00\pm0.02$ $0.39\pm0.04$ 0.756
18265-1517 19.0b $8.83\pm0.06$ $14.900\pm0.003$ $0.256\pm0.002$ 32.4
    $1.44\pm0.09$ $15.55\pm0.02$ $0.53\pm0.04$ 2.55
    $6.02\pm0.06$ $17.250\pm0.002$ $0.324\pm0.004$ 17.4
    $2.33\pm0.06$ $18.660\pm0.005$ $0.38\pm0.01$ 5.82
18316-0602 42.2 $0.5\pm0.4$ $38.5\pm0.1$ $0.4\pm0.1$ 1.41
    $4.0\pm0.4$ $41.0\pm0.1$ $0.9\pm0.1$ 4.04
    $39.3\pm0.4$ $41.8\pm0.1$ $0.3\pm0.1$ 118.
    $0.7\pm0.4$ $42.5\pm0.1$ $0.4\pm0.1$ 1.87
18317-0845 62.4 $0.22\pm0.03$ $59.67\pm0.05$ $0.7\pm0.1$ 0.304
    $0.27\pm0.04$ $63.15\pm0.03$ $0.48\pm0.06$ 0.537
    $0.60\pm0.07$ $63.890\pm0.005$ $0.28\pm0.02$ 1.99
    $3.5\pm0.1$ $64.39\pm0.01$ $0.96\pm0.04$ 3.39
    $0.49\pm0.05$ $65.020\pm0.005$ $0.26\pm0.02$ 1.75
    $0.18\pm0.02$ $65.77\pm0.01$ $0.22\pm0.02$ 0.771
18372-0541 22.8 $0.95\pm0.04$ $18.25\pm0.01$ $0.54\pm0.02$ 1.65
    $2.81\pm0.03$ $22.900\pm0.001$ $0.296\pm0.004$ 8.91
    $2.8\pm0.1$ $24.06\pm0.02$ $1.00\pm0.06$ 2.67
    $3.7\pm0.1$ $24.860\pm0.003$ $0.433\pm0.007$ 8.11
18408-0353 102.1b $0.20\pm0.04$ $100.00\pm0.06$ $0.7\pm0.2$ 0.293
    $0.11\pm0.03$ $105.30\pm0.03$ $0.3\pm0.1$ 0.334
    $0.57\pm0.02$ $106.400\pm0.003$ $0.238\pm0.009$ 2.24
18488+0000 83.2 $2.7\pm0.3$ $90.2\pm0.1$ $0.6\pm0.1$ 4.17
    $1.7\pm0.3$ $90.9\pm0.1$ $0.4\pm0.1$ 3.78
    $0.6\pm0.3$ $91.4\pm0.1$ $0.2\pm0.1$ 2.69
    $6.3\pm0.3$ $91.9\pm0.1$ $0.4\pm0.1$ 13.8
    $0.27\pm0.02$ $94.190\pm0.007$ $0.24\pm0.02$ 1.07
    $0.12\pm0.02$ $94.69\pm0.02$ $0.25\pm0.04$ 0.478

18507+0121

 57.1 $8.62\pm0.02$ $55.660\pm0.003$ $0.394\pm0.003$ 20.6
    $0.17\pm0.01$ $57.860\pm0.003$ $0.20\pm0.01$ 0.766
    $0.93\pm0.08$ $59.9\pm0.1$ $0.4\pm0.1$ 2.05
    $1.8\pm0.08$ $62.5\pm0.1$ $0.6\pm0.1$ 2.73
18517+0437 43.7 $1.4\pm0.1$ $39.64\pm0.03$ $1.0\pm0.1$ 1.33
    $138.1\pm0.3$ $41.180\pm0.003$ $0.524\pm0.003$ 248.
    $1.56\pm0.2$ $42.75\pm0.04$ $0.8\pm0.1$ 1.88
    $3.2\pm0.2$ $45.34\pm0.05$ $1.7\pm0.1$ 1.81
    $1.67\pm0.08$ $45.910\pm0.004$ $0.23\pm0.01$ 6.74
    $0.69\pm0.08$ $48.22\pm0.02$ $0.40\pm0.06$ 1.62
    $2.35\pm0.08$ $51.26\pm0.01$ $0.50\pm0.02$ 4.38
18532+0047 58.6 $0.23\pm0.02$ $61.89\pm0.02$ $0.48\pm0.05$ 0.449
18566+0408 85.1 $0.12\pm0.02$ $78.41\pm0.02$ $0.26\pm0.05$ 0.447
    $0.31\pm0.02$ $79.19\pm0.01$ $0.33\pm0.03$ 0.882
    $1.12\pm0.02$ $79.680\pm0.004$ $0.37\pm0.01$ 2.80
    $1.56\pm0.07$ $83.7\pm0.1$ $0.3\pm0.1$ 4.72
    $1.39\pm0.07$ $84.3\pm0.1$ $0.6\pm0.1$ 2.09
    $0.96\pm0.07$ $84.9\pm0.1$ $0.3\pm0.1$ 2.65
    $1.31\pm0.07$ $86.3\pm0.1$ $0.6\pm0.1$ 2.18
    $0.23\pm0.07$ $87.7\pm0.1$ $0.7\pm0.1$ 0.302
19230+1341 39.6 $6.69\pm0.01$ $35.800\pm0.001$ $0.658\pm0.003$ 9.56
    $16.10\pm0.05$ $36.900\pm0.001$ $0.867\pm0.003$ 17.4
    $1.00\pm0.03$ $38.390\pm0.003$ $0.32\pm0.01$ 2.97
    $3.43\pm0.05$ $39.180\pm0.005$ $0.93\pm0.02$ 3.47
    $0.95\pm0.03$ $40.65\pm0.01$ $0.74\pm0.03$ 1.20
19282+1814 24.1 $1.55\pm0.02$ $18.860\pm0.004$ $0.513\pm0.008$ 2.83
19388+2357 34.6 $3.3\pm0.4$ $36.4\pm0.1$ $0.7\pm0.1$ 4.18
    $3.5\pm0.4$ $37.2\pm0.1$ $0.5\pm0.1$ 6.75
    $8.8\pm0.4$ $38.2\pm0.1$ $0.4\pm0.1$ 23.0
    $0.4\pm0.4$ $38.7\pm0.1$ $0.2\pm0.1$ 1.63
    $1.1\pm0.4$ $39.6\pm0.1$ $0.4\pm0.1$ 2.90
20062+3550 0.6 $0.49\pm0.05$ $-3.0\pm0.1$ $0.5\pm0.1$ 0.883
    $0.48\pm0.05$ $-2.6\pm0.1$ $0.3\pm0.1$ 1.57
    $1.47\pm0.05$ $5.9\pm0.1$ $0.4\pm0.1$ 3.75
  0.6 $0.83\pm0.05$ $6.6\pm0.1$ $0.4\pm0.1$ 1.92
20126+4104 -3.9 $1.49\pm0.03$ $-8.393\pm0.005$ $0.56\pm0.02$ 2.52
    $4.6\pm0.9$ $-7.7\pm0.1$ $0.4\pm0.1$ 11.0
    $4.9\pm0.9$ $-6.5\pm0.1$ $0.5\pm0.1$ 9.09
    $18.5\pm0.9$ $-6.6\pm0.1$ $1.3\pm0.1$ 13.4
    $12.2\pm0.9$ $-6.2\pm0.1$ $0.3\pm0.1$ 41.4
    $1.2\pm0.9$ $-4.9\pm0.1$ $0.4\pm0.1$ 2.68
20350+4126 -2.5b $0.20\pm0.03$ $-10.93\pm0.08$ $0.9\pm0.2$ 0.206
    $0.09\pm0.02$ $-4.07\pm0.04$ $0.31\pm0.07$ 0.268
21306+5540* -71.1f $0.13\pm0.02$ $-78.27\pm0.05$ $0.6\pm0.1$ 0.22
    $0.38\pm0.02$ $-73.33\pm0.01$ $0.36\pm0.02$ 1.01
    $0.49\pm0.03$ $-71.04\pm0.02$ $0.69\pm0.06$ 0.66
    $0.47\pm0.03$ $-69.90\pm0.01$ $0.46\pm0.04$ 0.95
    $0.20\pm0.03$ $-68.66\pm0.08$ $1.0\pm0.2$ 0.2
22272+6358 -9.9 $0.46\pm0.02$ $-12.880\pm0.008$ $0.30\pm0.02$ 1.43
    $0.37\pm0.02$ $-12.40\pm0.02$ $0.41\pm0.03$ 0.853
    $20.78\pm0.02$ $-11.010\pm0.003$ $0.367\pm0.003$ 53.1
    $6.03\pm0.02$ $-10.270\pm0.001$ $0.372\pm0.002$ 15.2
22506+5944 -51.5 $0.17\pm0.04$ $-55.6\pm0.1$ $0.9\pm0.3$ 0.172
    $0.81\pm0.02$ $-53.880\pm0.006$ $0.44\pm0.01$ 1.72
22543+6145* -11.1c $71\pm1$ $-4.7\pm0.1$ $0.6\pm0.1$ 147
    $129\pm1$ $-4.1\pm0.1$ $0.3\pm0.1$ 361
    $101\pm1$ $-3.8\pm0.1$ $0.2\pm0.1$ 394
    $156\pm1$ $-2.5\pm0.1$ $0.5\pm0.1$ 296
    $30\pm1$ $-1.8\pm0.1$ $0.3\pm0.1$ 92

Notes.  (*) Sources rejected by Palla et al. (1991); (a) from Molinari et al. (1996) except when differently specified; (b) from NH3 observations performed with the Nobeyama 45-m telescope simultaneously to the CH3OH maser observations; (c) from CS (2-1) observations, Bronfman et al. (1996); (d) from Sridharan et al. (2002); (e) from Richards et al. (1987); (f) from Sunada et al. (2007) and references therein.


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