systems properties, i.e. the expectation value $`\langle
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@@ -53,7 +53,7 @@ crystal into three steps: (i) compute the scattering properties of free
Lippmann-Schwinger equation, (ii) construct the multiple scattering via
the structural Green function from systems geometry and (iii) construct
the Green from the in (i) obtained wavefunctions and single-site
$`t$`-matrix and the in thep (ii) computed structural GF.
$`t`$-matrix and the in thep (ii) computed structural GF.
### (i) Single-site problem
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@@ -115,8 +115,8 @@ positions vanish, i.e. $`\Delta t=0`$. This allows us to embed the
impurity in a finite real space cluster into the host system. The
calculation is then done as follows.
- Compute the host systems Green function and write out the structural Green function as well as the single-site $`t`$ matrix of the host $`t_{\mathrm{host}}`$.
- From the impurity potential compute the $t$-matrix of the impurity and construct $`\Delta t=t_{\mathrm{host}}-t_{\mathrm{imp}}`$
- Solve the impurity Dyson equation: $`\underline{\underline{G}}=\underline{\underline{G}}_{\mathrm{host}}+\underline{\underline{G}}_{\mathrm{host}}\Delta t\underline{\underline{G}}`$
- Compute the new impurity potential from the Green function and update the input potential
- Repeat steps 2.-4. until the impurity potential converges
*Compute the host systems Green function and write out the structural Green function as well as the single-site $`t`$ matrix of the host $`t_{\mathrm{host}}`$.
*From the impurity potential compute the $`t`$-matrix of the impurity and construct $`\Delta t=t_{\mathrm{host}}-t_{\mathrm{imp}}`$
*Solve the impurity Dyson equation: $`\underline{\underline{G}}=\underline{\underline{G}}_{\mathrm{host}}+\underline{\underline{G}}_{\mathrm{host}}\Delta t\underline{\underline{G}}`$
*Compute the new impurity potential from the Green function and update the input potential
*Repeat steps 2.-4. until the impurity potential converges