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Conflicting definitions of statistical weight in calculation of level-resoled dielectronic recombination #9
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Hi Will,
I see the multiplicity (mult) is defined as 2J+1 in ch_load_ion_rates, so the multiplicity is actually the weight. Thus the code is OK, but the variable mult is misnamed! It’s best not to relabel it at this stage, but I’ll insert a comment into ch_load_ion_rates pointing this out.
Thanks, Peter
From: Will Barnes ***@***.***>
Date: Tuesday, February 4, 2025 at 3:27 PM
To: chianti-atomic/chianti-idl ***@***.***>
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Subject: [EXTERNAL] [BULK] [chianti-atomic/chianti-idl] Conflicting definitions of statistical weight in calculation of level-resoled dielectronic recombination (Issue #9)
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In ch_load_2ion_rates, the level resolved dielectronic capture as well as the dielectronic recombination between the ground states of the recombining and recombined ion is calculated. The latter includes a correction factor to account for the double counting of the level-resolved rates. My understanding is that these contributions are calculated using Eqs. 4 and 5 in the Appendix of Dere et al. (2019) (the v9 paper).
Both equations include the ratio $g_s/g_k$ which I understand to be the ratio of the statistical weights of the autoionizing states ($s$) of the recombined ion and the lower-energy bound states ($k$) of the recombining ion.
In ch_load_2ion_rates, when computing the the dielectronic capture rate, the statistical weights are computed as $2J+1$ (where $J$ is the total angular momentum): https://github.com/chianti-atomic/chianti-idl/blob/0387392a6cba39ce700be0d164f53ab56b2fcd12/level_population/ch_load_2ion_rates.pro#L408-L412
However, when computing the total of the level-resolved dielectronic recombination rates, the statistical weights are computed using the multiplicity, $2S+1$ (where $S$ is the spin): https://github.com/chianti-atomic/chianti-idl/blob/0387392a6cba39ce700be0d164f53ab56b2fcd12/level_population/ch_load_2ion_rates.pro#L471-L484
Is this difference intentional? If so, why are the statistical weights defined differently in these two expressions?
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Thanks Peter! I hadn't even thought to check that function and naively assumed it was the same multiplicity in the elvlc files. |
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In
ch_load_2ion_rates
, the level resolved dielectronic capture as well as the dielectronic recombination between the ground states of the recombining and recombined ion is calculated. The latter includes a correction factor to account for the double counting of the level-resolved rates. My understanding is that these contributions are calculated using Eqs. 4 and 5 in the Appendix of Dere et al. (2019) (the v9 paper).Both equations include the ratio$g_s/g_k$ which I understand to be the ratio of the statistical weights of the autoionizing states ($s$ ) of the recombined ion and the lower-energy bound states ($k$ ) of the recombining ion.
In$2J+1$ (where $J$ is the total angular momentum):
ch_load_2ion_rates
, when computing the the dielectronic capture rate, the statistical weights are computed aschianti-idl/level_population/ch_load_2ion_rates.pro
Lines 408 to 412 in 0387392
However, when computing the total of the level-resolved dielectronic recombination rates, the statistical weights are computed using the multiplicity,$2S+1$ (where $S$ is the spin):
chianti-idl/level_population/ch_load_2ion_rates.pro
Lines 471 to 484 in 0387392
Is this difference intentional? If so, why are the statistical weights defined differently in these two expressions?
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