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Integrated amplitudes
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trex.org
73
trex.org
@ -943,6 +943,79 @@ power = [
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#+end_src
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#+end_src
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:end:
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:end:
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** Amplitudes (amplitude group)
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The wave function may be expressed in terms of action of the cluster
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operator $\hat{T}$:
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\[
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\hat{T} = \hat{T}_1 + \hat{T}_2 + \hat{T}_3 + \dots
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\]
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on a reference wave function $\Psi$, where $\hat{T}_1$ is the single excitation operator,
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\[
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\hat{T}_1 = \sum_{ia} t_{i}^{a}\, \hat{a}^\dagger_a \hat{a}_i
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\],
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$\hat{T}_2$ is the double excitation operator,
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\[
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\hat{T}_2 = \frac{1}{4} \sum_{ijab} t_{ij}^{ab}\, \hat{a}^\dagger_a \hat{a}^\dagger_b \hat{a}_j \hat{a}_i
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\],
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/etc/. Indices $i,j,a,b$ denote molecular orbital indices.
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Wave functions obtained with perturbation theory of configuration
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interaction are of the form
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\[ |\Phi\rangle = \hat{T}|\Psi\rangle \]
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and coupled-cluster wave functions are of the form
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\[ |\Phi\rangle = e^{\hat{T}}| \Psi \rangle \]
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The reference wave function is stored using the ~determinant~ and/or
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~csf~ groups, and the amplitudes are stored using the current group.
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The attributes with the ~exp~ suffix correspond to exponentialized operators.
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The order of the indices is chosen such that
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- ~t(i,a)~ = $t_{i}^{a}$.
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- ~t(i,j,a,b)~ = $t_{ij}^{ab}$,
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- ~t(i,j,k,a,b,c)~ = $t_{ijk}^{abc}$,
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- ~t(i,j,k,l,a,b,c,d)~ = $t_{ijkl}^{abcd}$,
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- $\dots$
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#+NAME: amplitude
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| Variable | Type | Dimensions | Description |
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|-----------------+----------------+-------------------------------------------------------------+-------------------------------------------------|
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| ~single~ | ~float sparse~ | ~(mo.num,mo.num)~ | Single excitation amplitudes |
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| ~single_exp~ | ~float sparse~ | ~(mo.num,mo.num)~ | Exponentialized single excitation amplitudes |
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| ~double~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num)~ | Double excitation amplitudes |
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| ~double_exp~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num)~ | Exponentialized double excitation amplitudes |
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| ~triple~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num,mo.num,mo.num)~ | Triple excitation amplitudes |
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| ~triple_exp~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num,mo.num,mo.num)~ | Exponentialized triple excitation amplitudes |
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| ~quadruple~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num,mo.num,mo.num,mo.num,mo.num)~ | Quadruple excitation amplitudes |
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| ~quadruple_exp~ | ~float sparse~ | ~(mo.num,mo.num,mo.num,mo.num,mo.num,mo.num,mo.num,mo.num)~ | Exponentialized quadruple excitation amplitudes |
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#+CALL: json(data=amplitude, title="amplitude")
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#+RESULTS:
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:results:
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#+begin_src python :tangle trex.json
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"amplitude": {
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"single" : [ "float sparse", [ "mo.num", "mo.num" ] ]
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, "single_exp" : [ "float sparse", [ "mo.num", "mo.num" ] ]
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, "double" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num" ] ]
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, "double_exp" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num" ] ]
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, "triple" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num" ] ]
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, "triple_exp" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num" ] ]
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, "quadruple" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num" ] ]
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, "quadruple_exp" : [ "float sparse", [ "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.num", "mo.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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** Reduced density matrices (rdm group)
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The reduced density matrices are defined in the basis of molecular
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The reduced density matrices are defined in the basis of molecular
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