| 1 | 01 09 29 //the magic number for this format file |
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| 2 | # |
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| 3 | # This file defines the continuum resolution used by the code. |
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| 4 | # It is designed to be edited by a person and allows any continuum |
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| 5 | # resolution to be entered. |
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| 6 | # |
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| 7 | # the command |
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| 8 | # set continuum resolution |
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| 9 | # proves a way to change the resolution of the entire continuum |
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| 10 | # by a constant factor without editing this file. This file |
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| 11 | # provides a way to change the resolution of only parts of the |
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| 12 | # continuum, and to change the default behavior of the code. |
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| 13 | # |
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| 14 | # if the continuum resolution is changed either with the |
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| 15 | # set continuum command, or by changing this file, it will be necessary |
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| 16 | # to recompile the stellar atmosphere and grain opacity files |
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| 17 | # |
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| 18 | # Each line is an ordered pair of numbers, |
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| 19 | # The first is the upper limit of an energy interval in Rydbergs |
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| 20 | # and the second number is the resolution expressed as delta E/E. |
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| 21 | # The code's execution time is pretty much set by the number of |
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| 22 | # continuum points, so increasing the resolution will require more time. |
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| 23 | # |
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| 24 | # The numbers are interpreted as linear quantities unless negative, |
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| 25 | # when they are assumed to be logs. |
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| 26 | # |
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| 27 | # There is no limit to the number of bounds since the arrays |
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| 28 | # are dynamically allocated. |
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| 29 | # |
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| 30 | # this is the first range, and has a lower limit of the low-energy |
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| 31 | # bound of the code. So the continuum will have a resolution of 0.1 |
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| 32 | # between the low-energy limit and 2e-5 Ryd. |
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| 33 | 0.00002 0.1 |
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| 34 | # |
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| 35 | # the energy range 2e-5 to 600 ryd will have a resolution of 0.005 |
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| 36 | 600. 0.005 |
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| 37 | # |
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| 38 | # the last number must have an upper bound of zero, which is |
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| 39 | # interpreted as the upper energy bound of the code |
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| 40 | # so the energy range from 600 Ryd to the high-energy limit of the |
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| 41 | # code will by 0.03 |
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| 42 | 0 0.03 |
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