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Add determinant group
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trex.org
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trex.org
@ -635,7 +635,49 @@ prim_factor =
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#+end_src
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:end:
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* TODO Slater determinants
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* Slater determinants (determinant group)
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The configuration interaction (CI) wave function $\Psi$
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can be expanded in the basis of Slater determinants $D_I$ as follows
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\[
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|\Psi> = \sum_I C_I |D_I>
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\]
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For relatively small expansions, a given determinant can be represented as a list of ~mo.num~ occupation numbers.
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However, this requires a lot of extra memory and would be technically impossible for larger expansions
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(~millions of determinants). This is why the determinants are stored as bit fields in the TREXIO file
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(see ~int bitfield~ type in the table below). By default, the chemist notation is used, namely
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\[
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| D_I > = | \alpha_1 \alpha_2 \ldots \alpha_{n\uparrow} \beta_1 \beta_2 \ldots \beta_{n\downarrow} >
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\
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where $\alpha$ and $\beta$ denote $\uparrow$-spin and $\downarrow$-spin electrons, respectively,
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$n\uparrow$ and $n\downarrow$ correspond to ~electron.up_num~ and ~electron.dn_num~, respectively.
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Internally, bit fields for $\alpha$ and $\beta$ electrons are stored separately,
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which is why the ~determinant.list~ attribute has a second dimension.
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#+NAME: determinant
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| Variable | Type | Dimensions | Description |
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|---------------+----------------+------------------------+--------------------------------------------------------|
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| ~num~ | ~dim~ | | Number of determinants |
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| ~list~ | ~int bitfield~ | ~(determinant.num, 2)~ | List of determinants as integer bit fields |
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| ~coefficient~ | ~float~ | ~(determinant.num)~ | Coefficients of the determinants from the CI expansion |
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#+CALL: json(data=determinant, title="determinant")
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#+RESULTS:
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:results:
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#+begin_src python :tangle trex.json
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"determinant": {
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"num" : [ "dim" , [] ]
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, "list" : [ "int binary", [ "2", "determinant.num" ] ]
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, "coefficient" : [ "float" , [ "determinant.num" ] ]
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} ,
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#+end_src
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:end:
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* Reduced density matrices (rdm group)
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The reduced density matrices are defined in the basis of molecular
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