mirror of
https://github.com/TREX-CoE/trexio.git
synced 2024-11-03 20:54:07 +01:00
Add state group
This commit is contained in:
parent
3bc8a449db
commit
f0189cb8da
49
trex.org
49
trex.org
@ -641,7 +641,7 @@ prim_factor =
|
||||
can be expanded in the basis of Slater determinants $D_I$ as follows
|
||||
|
||||
\[
|
||||
| \Psi> = \sum_I C_I | D_I>
|
||||
| \Psi> = \sum_I C_I | D_I> |
|
||||
\]
|
||||
|
||||
For relatively small expansions, a given determinant can be represented as a list of ~mo.num~ occupation numbers.
|
||||
@ -650,7 +650,7 @@ prim_factor =
|
||||
(see ~int bitfield~ type in the table below). By default, the chemist notation is used, namely
|
||||
|
||||
\[
|
||||
| D_I > = | \alpha_1 \alpha_2 \ldots \alpha_{n\uparrow} \beta_1 \beta_2 \ldots \beta_{n\downarrow} >
|
||||
| D_I > = | \alpha_1 \alpha_2 \ldots \alpha_{n\uparrow} \beta_1 \beta_2 \ldots \beta_{n\downarrow} > |
|
||||
\]
|
||||
|
||||
where $\alpha$ and $\beta$ denote $\uparrow$-spin and $\downarrow$-spin electrons, respectively,
|
||||
@ -659,24 +659,49 @@ prim_factor =
|
||||
which is why the ~determinant.list~ attribute has a second dimension.
|
||||
|
||||
#+NAME: determinant
|
||||
| Variable | Type | Dimensions | Description |
|
||||
|---------------+-----------------+------------------------+--------------------------------------------------------|
|
||||
| ~num~ | ~dim~ | | Number of determinants |
|
||||
| ~list~ | ~int special~ | ~(determinant.num, 2)~ | List of determinants as integer bit fields |
|
||||
| ~coefficient~ | ~float special~ | ~(determinant.num)~ | Coefficients of the determinants from the CI expansion |
|
||||
| Variable | Type | Dimensions | Description |
|
||||
|---------------+-----------------+-------------------------------+--------------------------------------------------------|
|
||||
| ~num~ | ~dim~ | | Number of determinants |
|
||||
| ~list~ | ~int special~ | ~(determinant.num)~ | List of determinants as integer bit fields |
|
||||
| ~coefficient~ | ~float special~ | ~(state.num,determinant.num)~ | Coefficients of the determinants from the CI expansion |
|
||||
|
||||
#+CALL: json(data=determinant, title="determinant")
|
||||
|
||||
#+RESULTS:
|
||||
:results:
|
||||
:RESULTS:
|
||||
#+begin_src python :tangle trex.json
|
||||
"determinant": {
|
||||
"num" : [ "dim" , [] ]
|
||||
, "list" : [ "int special" , [ "2", "determinant.num" ] ]
|
||||
, "coefficient" : [ "float special", [ "determinant.num" ] ]
|
||||
"num" : [ "dim" , [] ]
|
||||
, "list" : [ "int special" , [ "determinant.num" ] ]
|
||||
, "coefficient" : [ "float special", [ "determinant.num", "state.num" ] ]
|
||||
} ,
|
||||
#+end_src
|
||||
:end:
|
||||
:END:
|
||||
|
||||
* Excited states (state group)
|
||||
|
||||
By default, the ~determinant~ group corresponds to the ground state.
|
||||
However, it should be also possible to store the coefficients that
|
||||
correspond to excited state wave functions for the same set of
|
||||
determinants. This is the goal of the present group
|
||||
|
||||
#+NAME: state
|
||||
| Variable | Type | Dimensions | Description |
|
||||
|----------+-------+---------------+------------------------------------------------|
|
||||
| ~num~ | ~dim~ | | Number of states (including the ground state) |
|
||||
| ~label~ | ~str~ | ~(state.num)~ | Label of a given state (e.g. 'S' for singlets) |
|
||||
|
||||
#+CALL: json(data=state, title="state")
|
||||
|
||||
#+RESULTS:
|
||||
:RESULTS:
|
||||
#+begin_src python :tangle trex.json
|
||||
"state": {
|
||||
"num" : [ "dim", [] ]
|
||||
, "label" : [ "str", [ "state.num" ] ]
|
||||
} ,
|
||||
#+end_src
|
||||
:END:
|
||||
|
||||
* Reduced density matrices (rdm group)
|
||||
|
||||
|
Loading…
Reference in New Issue
Block a user