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The comparisons show that the best overall prediction of the exact Green function is given by the asymmetric approximation which remains accurate down to a Strouhal number of 1/2.
where the local Green function is given by (2.11).
end{aligned} (11) Here, the non-interacting impurity Green function is given by begin{aligned} {G}_{mathrm{imp}}^{R 0)} omega)^{-1}=omega+ mu-Delta omega).
Here, the non-interacting impurity Green function is given by begin{aligned} {G}_{mathrm{imp}}^{R 0)} omega)^{-1}=omega+ mu-Delta omega).
Similar(56)
where Green's function is given by (1.5).
The retarded Green's function is given by G = [ E + S − H − Σ L − Σ R ] − 1 (5).
Taking an average of the above two expressions and noting, we obtain (1.4), where Green's function is given by (A11).
The Green's function is given by: Gleft(mathbf{r}-{mathbf{r}}^{mathbf{prime}}right)=frac{ exp left ikleft|mathbf{r}-{mathbf{r}}^{mathbf{prime}}right|right)}{4pi left ikleft|mathbf{r}-{mathbf{r}bf{prime}}right|} (5).
Then, according to [21], a definition and properties of the ordinary Green's function are given.
The extensive treatments of the ARPES data in terms of Green's function are given elsewhere[10].
In [10 15] and [20 22], only an upper bound of corresponding Green's function was given and thus only a one-side Lyapunov inequality could be obtained.
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Justyna Jupowicz-Kozak
CEO of Professional Science Editing for Scientists @ prosciediting.com