[ewald] dudom
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@ -336,6 +336,21 @@ reference "eq:W definition"
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\end_inset
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\end_inset
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-dimensional lattice.
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-dimensional lattice.
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\begin_inset Foot
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status open
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\begin_layout Plain Layout
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Note that
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\begin_inset Formula $d$
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\end_inset
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here is dimensionality of the lattice, not the space it lies in, which
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I for certain reasons assume to be three.
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(TODO few notes on integration and reciprocal lattices in some appendix)
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\end_layout
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\end_inset
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In electrostatics, one can solve this problem with Ewald summation.
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In electrostatics, one can solve this problem with Ewald summation.
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Its basic idea is that if what asymptoticaly decays poorly in the direct
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Its basic idea is that if what asymptoticaly decays poorly in the direct
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space, will perhaps decay fast in the Fourier space.
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space, will perhaps decay fast in the Fourier space.
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@ -366,7 +381,7 @@ The translation operator
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\begin_inset Formula $S$
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\begin_inset Formula $S$
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\end_inset
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\end_inset
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is now a function defined in the whole 3D space;
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is now a function defined in the whole 3d space;
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\begin_inset Formula $\vect r_{\alpha},\vect r_{\beta}$
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\begin_inset Formula $\vect r_{\alpha},\vect r_{\beta}$
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\end_inset
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\end_inset
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@ -561,7 +576,7 @@ Finding a good decomposition
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\end_layout
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\end_layout
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\begin_layout Standard
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\begin_layout Standard
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The remaining challenge is therefore finding a suitable decomposition
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The remaining challenge is therefore finding a suitable decomposition
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\begin_inset Formula $S^{\textup{L}}+S^{\textup{S}}$
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\begin_inset Formula $S^{\textup{L}}+S^{\textup{S}}$
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\end_inset
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\end_inset
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@ -600,12 +615,42 @@ reference "eq:W Long definition"
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absolutely convergent.
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absolutely convergent.
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\end_layout
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\end_layout
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\begin_layout Standard
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The translation operator
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\begin_inset Formula $S$
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\end_inset
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for compact scatterers in 3d can be expressed as
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\begin_inset Formula
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\[
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S_{l',m',t'\leftarrow l,m,t}\left(\vect r\leftarrow\vect 0\right)=\sum_{p}c_{p}^{l',m',t'\leftarrow l,m,t}Y_{p,m'-m}\left(\theta_{\vect r},\phi_{\vect r}\right)z_{p}^{(J)}\left(\left|\vect r\right|\right)
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\]
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\end_inset
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where
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\begin_inset Formula $Y_{l,m}\left(\theta,\phi\right)$
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\end_inset
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are the spherical harmonics,
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\begin_inset Formula $z_{p}^{(J)}\left(r\right)$
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\end_inset
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some of the Bessel or Hankel functions (TODO) and
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\begin_inset Formula $c_{p}^{l,m,t\leftarrow l',m',t'}$
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\end_inset
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are some ugly but known coefficients (Xu 1996, eqs.
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76,77).
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\end_layout
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\begin_layout Section
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\begin_layout Section
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(Appendix) Hankel transform
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(Appendix) Hankel transform
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\end_layout
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\end_layout
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\begin_layout Standard
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\begin_layout Standard
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Acording to Wikipedia page on Hankel transform,
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Acording to (Baddour 2010, eq.
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13) (CHECK FACTORS)
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\begin_inset Formula
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\begin_inset Formula
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\[
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\[
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\uaft f(\vect k)=
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\uaft f(\vect k)=
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