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Table A.1

Gaussian fit results for the lines of small hydrocarbons detected toward the Horsehead PDR at RA = 5h40m53.936s, Dec = −2°28′00′′ (J2000).

Species Transition Frequency Area Velocity Width
MHz    mK   km   s-1    km   s-1    km   s-1

C2H N = 1−0,J = 3/2−1/2   F = 1−1 87 284.105 238  ±  3 10.675  ±  0.005 0.735  ±  0.013
N = 1−0,J = 3/2−1/2   F = 2−1 87 316.898 1943  ±  6 10.682  ±  0.001 0.815  ±  0.003
N = 1−0,J = 3/2−1/2   F = 1−0 87 328.585 1035  ±  4 10.675  ±  0.002 0.769  ±  0.004
N = 1−0,J = 1/2−1/2   F = 1−1 87 401.989 1103  ±  5 10.694  ±  0.002 0.785  ±  0.004
N = 1−0,J = 1/2−1/2   F = 0−1 87 407.165 489  ±  4 10.697  ±  0.003 0.749  ±  0.008
N = 1−0,J = 1/2−1/2   F = 1−0 87 446.470 262  ±  3 10.700  ±  0.004 0.745  ±  0.011

c-C3H N = 212−111,J = 5/2−3/2   F = 3−2 91 494.231 106  ±  3 10.395  ±  0.010 0.691  ±  0.024
N = 212−111,J = 5/2−3/2   F = 2−1 91 497.525 59  ±  3 10.561  ±  0.012 0.594  ±  0.034
N = 212−111,J = 3/2−1/2   F = 1−0 91 692.752 32  ±  3 10.712  ±  0.036 0.887  ±  0.084
N = 212−111,J = 3/2−1/2   F = 2−1 91 699.471 74  ±  4 10.760  ±  0.020 0.858  ±  0.050

l-C3H J = 9/2−7/2   F = 5−4(f) 97 995.166 44  ±  7 10.605  ±  0.051 0.647  ±  0.108
J = 9/2−7/2   F = 4−3(f) 97 995.913 45  ±  10 10.583  ±  0.092 0.848  ±  0.235
J = 9/2−7/2   F = 5−4(e) 98 011.611 41  ±  7 10.629  ±  0.046 0.599  ±  0.116
J = 9/2−7/2   F = 4−3(e) 98 012.524 35  ±  8 10.550  ±  0.075 0.651  ±  0.183

c-C3H2 202−111 82 093.542 242  ±  6 10.704  ±  0.009 0.741  ±  0.023
312−303 82 966.200 68  ±  3 10.660  ±  0.012 0.618  ±  0.029
322−313 84 727.696 14  ±  2 10.633  ±  0.028 0.344  ±  0.051
212−101 85 338.893 748  ±  4 10.687  ±  0.002 0.767  ±  0.005
303−212 117 151.191 507  ±  72 10.680  ±  0.051 0.715  ±  0.117

l-C3H2 414−313 82 395.090 107  ±  7 10.681  ±  0.020 0.720  ±  0.057
404−303 83 165.256 43  ±  4 10.362  ±  0.029 0.647  ±  0.068
413−312 83 933.700 93  ±  3 10.690  ±  0.010 0.689  ±  0.025
515−414 102 992.379 81  ±  3 10.658  ±  0.012 0.657  ±  0.030
533−432 103 914.354 27  ±  2 10.592  ±  0.023 0.538  ±  0.052
505−404 103 952.926 34  ±  3 10.803  ±  0.030 0.652  ±  0.068
514−413 104 915.583 58  ±  4 10.696  ±  0.025 0.703  ±  0.058

C4H N = 9−8,J = 19/2−17/2 85 634.004 198  ±  4 10.737  ±  0.007 0.689  ±  0.018
N = 9−8,J = 17/2−15/2 85 672.579 168  ±  4 10.725  ±  0.007 0.663  ±  0.018
N = 10−9,J = 21/2−19/2 95 150.388 204  ±  3 10.734  ±  0.004 0.682  ±  0.011
N = 10−9,J = 19/2−17/2 95 188.946 177  ±  3 10.700  ±  0.005 0.665  ±  0.013
N = 11−10,J = 23/2−21/2 104 666.565 202  ±  4 10.732  ±  0.007 0.714  ±  0.019
N = 11−10,J = 21/2−19/2 104 705.106 177  ±  5 10.705  ±  0.011 0.728  ±  0.026
N = 12−11,J = 25/2−23/2 114 182.512 162  ±  12 10.665  ±  0.021 0.582  ±  0.051
N = 12−11,J = 23/2−21/2 114 221.040 186  ±  12 10.663  ±  0.022 0.719  ±  0.056

Notes. Only lines in the 3   mm band with an energy of the upper level lower than 100   K and a higher signal-to-noise ratio than 8 are shown.

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