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# Jastrow
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Information related to the Jastrow factor in trans-correlated calculations.
The main keywords are:
- `j2e_type`
- `j1e_type`
- `env_type`
## j2e_type Options
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1. **None:** No 2e-Jastrow is used.
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2. **Mu:** 2e-Jastrow inspired by Range Separated Density Functional Theory. It has the following shape:
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< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%5Ctau=%5Cfrac%7B1%7D%7B2%7D%5Csum_%7Bi,j%5Cneq%20i%7Du(%5Cmathbf%7Br%7D_i,%5Cmathbf%7Br%7D_j)" >
< / p >
with,
< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%20u(%5Cmathbf%7Br%7D_1,%5Cmathbf%7Br%7D_2)=u(r_%7B12%7D)=%5Cfrac%7Br_%7B12%7D%7D%7B2%7D%5Cleft%5B1-%5Ctext%7Berf%7D(%5Cmu%20r_%7B12%7D)%5Cright%5D-%5Cfrac%7B%5Cexp%5B-(%5Cmu%20r_%7B12%7D)%5E2%5D%7D%7B2%5Csqrt%7B%5Cpi%7D%5Cmu%7D" >
< / p >
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3. **Mu_Nu:** A valence and a core correlation terms are used
< p align = "center" >
< img src = "https://latex.codecogs.com/png.image? \inline&space; \huge&space; \dpi{110} \bg{white}&space;u( \mathbf{r}_1, \mathbf{r}_2)=u( \mu;r_{12}) \,v( \mathbf{r}_1) \,v( \mathbf{r}_2)+u( \nu;r_{12})[1-v( \mathbf{r}_1) \,v( \mathbf{r}_2)]" >
< / p >
with envelop \(v\).
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## env_type Options
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The 2-electron Jastrow is multiplied by an envelope \(v\):
< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%5Ctau=%5Cfrac%7B1%7D%7B2%7D%5Csum_%7Bi,j%5Cneq%20i%7Du(%5Cmathbf%7Br%7D_i,%5Cmathbf%7Br%7D_j)%5C,v(%5Cmathbf%7Br%7D_i)%5C,v(%5Cmathbf%7Br%7D_j)" >
< / p >
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- if `env_type` is **None** : No envelope is used.
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- if `env_type` is **Prod_Gauss** :
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< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%20v(%5Cmathbf%7Br%7D)=%5Cprod_%7BA%7D%5Cleft(1-e%5E%7B-%5Calpha_A(%5Cmathbf%7Br%7D-%5Cmathbf%7BR%7D_A)%5E2%7D%5Cright)" >
< / p >
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- if `env_type` is **Sum_Gauss** :
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< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%20v(%5Cmathbf%7Br%7D)=1-%5Csum_%7BA%7Dc_A%20e%5E%7B-%5Calpha_A(%5Cmathbf%7Br%7D-%5Cmathbf%7BR%7D_A)%5E2%7D" >
< / p >
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Here, \(A\) designates the nuclei, and the coefficients and exponents are defined in the tables `env_coef` and `env_expo` respectively.
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## j1e_type Options
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The 1-electron Jastrow used is:
< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%5Ctau=%5Csum_i%20u_%7B1e%7D(%5Cmathbf%7Br%7D_i)" >
< / p >
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- if `j1e_type` is **None** : No one-electron Jastrow is used.
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- if `j1e_type` is **Gauss** : We use
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< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7Du_%7B1e%7D(%5Cmathbf%7Br%7D)=%5Csum_A%5Csum_%7Bp_A%7Dc_%7Bp_A%7De%5E%7B-%5Calpha_%7Bp_A%7D(%5Cmathbf%7Br%7D-%5Cmathbf%7BR%7D_A)%5E2%7D" >
< / p >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7D%20c_%7Bp_A%7D%5C,%5Ctext%7Band%7D%5C,%5Calpha_%7Bp_A%7D" >
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are defined by the tables `j1e_coef` and `j1e_expo` , respectively.
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- if `j1e_type` is **Charge_Harmonizer** : The one-electron Jastrow factor aims to offset the adverse impact of modifying the charge density induced by the two-electron factor
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< p align = "center" >
< img src = "https://latex.codecogs.com/png.image?%5Cinline%20%5Clarge%20%5Cdpi%7B200%7D%5Cbg%7Bwhite%7Du_%7B1e%7D(%5Cmathbf%7Br%7D_1)=-%5Cfrac%7BN-1%7D%7B2N%7D%5C,%5Csum_%7B%5Csigma%7D%5C,%5Cint%20d%5Cmathbf%7Br%7D_2%5C,%5Crho%5E%7B%5Csigma%7D(%5Cmathbf%7Br%7D_2)%5C,u_%7B2e%7D(%5Cmathbf%7Br%7D_1,%5Cmathbf%7Br%7D_2)" >
< / p >
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- if `j1e_type` is **Charge_Harmonizer_AO** : The one-electron Jastrow factor **Charge_Harmonizer** is fitted by the product of atomic orbitals:
< p align = "center" >
< img src = "https://latex.codecogs.com/png.image? \inline&space; \large&space; \dpi{300} \bg{white}&space;u_{1e}( \mathbf{r})= \sum_{ \alpha, \beta}C_{ \alpha, \beta} \chi_{ \alpha}( \mathbf{r}) \chi_{ \beta}( \mathbf{r})" >
< / p >
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