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Revision 2347, 1.6 kB
(checked in by gary, 3 months ago)
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merge data to head of trunk to make easier to test of various systems
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| 1 | 20429 // magic number - today's date |
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| 2 | # fits for colllisional rates within H2 |
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| 3 | # >>refer H2 coll Hp Gerlich, D., 1990, J. Chem. Phys., 92, 2377-2388 |
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| 4 | #rate(up -> low) = k0 * exp( -delta E/kT ), k0 = a[0] *1e-10 cm^3 s^-1, a[1] is dE in milli Ev |
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| 5 | # |
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| 6 | # NB - this data has been fit with a different equation from the other 4 |
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| 7 | # the last zero is to be parallel with the other data files but is not used |
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| 8 | # the following are the downward collision rates, which we use. He also gives upward rates, |
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| 9 | # which are at the end of this file, but they are not in detailed balance with the downward |
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| 10 | # rates. Something is seriously wrong with the paper. |
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| 11 | # |
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| 12 | #v_upper j_upper v_lower j_lower a b c |
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| 13 | 0 1 0 0 2.024 -0.331 0 |
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| 14 | 0 2 0 0 2.889 -0.171 0 |
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| 15 | 0 2 0 1 9.575 -0.183 0 |
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| 16 | 0 3 0 0 0.522 -0.268 0 |
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| 17 | 0 3 0 1 8.202 -0.25 0 |
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| 18 | 0 3 0 2 2.729 -0.249 0 |
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| 19 | 0 4 0 0 1.071 -0.199 0 |
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| 20 | 0 4 0 1 3.398 -0.176 0 |
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| 21 | 0 4 0 2 5.7 -0.159 0 |
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| 22 | 0 4 0 3 7.91 -0.147 0 |
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| 23 | 0 5 0 0 0.246 -0.281 0 |
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| 24 | 0 5 0 1 3.818 -0.255 0 |
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| 25 | 0 5 0 2 1.275 -0.241 0 |
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| 26 | 0 5 0 3 8.883 -0.223 0 |
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| 27 | 0 5 0 4 2.246 -0.217 0 |
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| 28 | 0 6 0 0 0.565 -0.203 0 |
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| 29 | 0 6 0 1 1.755 -0.169 0 |
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| 30 | 0 6 0 2 2.932 -0.156 0 |
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| 31 | 0 6 0 3 4.088 -0.142 0 |
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| 32 | 0 6 0 4 5.209 -0.124 0 |
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| 33 | 0 6 0 5 6.223 -0.124 0 |
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| 34 | 0 7 0 0 0.145 -0.254 0 |
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| 35 | 0 7 0 1 2.23 -0.216 0 |
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| 36 | 0 7 0 2 0.743 -0.207 0 |
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| 37 | 0 7 0 3 5.179 -0.199 0 |
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| 38 | 0 7 0 4 1.32 -0.189 0 |
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| 39 | 0 7 0 5 7.977 -0.177 0 |
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| 40 | 0 7 0 6 1.828 -0.193 0 |
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| 41 | 0 8 0 0 0.432 -0.349 0 |
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| 42 | 0 8 0 1 1.107 -0.052 0 |
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| 43 | 0 8 0 2 1.792 -0.12 0 |
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| 44 | 0 8 0 3 2.496 -0.118 0 |
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| 45 | 0 8 0 4 3.185 -0.115 0 |
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| 46 | 0 8 0 5 3.851 -0.109 0 |
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| 47 | 0 8 0 6 4.489 -0.101 0 |
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| 48 | 0 8 0 7 4.974 -0.135 0 |
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| 49 | 0 9 0 0 0.16 -0.159 0 |
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| 50 | 0 9 0 1 2.448 -0.177 0 |
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| 51 | 0 9 0 2 0.803 -0.144 0 |
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| 52 | 0 9 0 3 5.074 -0.188 0 |
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| 53 | 0 9 0 4 0.744 -0.06 0 |
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| 54 | 0 9 0 5 4.445 -0.1 0 |
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| 55 | 0 9 0 6 1.039 -0.098 0 |
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| 56 | 0 9 0 7 5.915 -0.094 0 |
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