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#import "@preview/physica:0.9.5": pdv, super-T-as-transpose
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#show: super-T-as-transpose
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== Approximation of Raman tensor of 4H-SiC
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== Approximation of Raman tensor of 4H-SiC <appd-predict>
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近似的核心思路。
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@@ -7,7 +7,7 @@ The phonons at the #sym.Gamma point in 4H-SiC (space group P6#sub[3]mc)
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and negligible-polar modes (2A#sub[1] + 4B#sub[1] + 2E#sub[1] + 4E#sub[2]).
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The form of the Raman tensors for each representation is well known and summarized in @table-rep.
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#include "table-rep.typ"
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// #include "table-rep.typ"
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By further decomposing the doubly degenerate modes (E#sub[1] and E#sub[2] of C#sub[6v] group)
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into the C#sub[2v] point group,
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@@ -1,24 +0,0 @@
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#figure({
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set text(size: 9pt);
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set par(justify: false);
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let m2(content) = table.cell(colspan: 2, content);
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let A1 = [A#sub[1]];
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let A2 = [A#sub[2]];
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let B1 = [B#sub[1]];
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let B2 = [B#sub[2]];
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let E1 = [E#sub[1]];
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let E2 = [E#sub[2]];
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table(columns: 8, align: center + horizon,
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table.cell(rowspan: 2)[*Representation*],
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[C#sub[6v]], A1, B1, m2(E1), m2(E2),
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[C#sub[2v]], A1, B1, B2, B1, A2, A1,
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m2[*Vibration Direction*], [z], [z], [x], [y], [x], [y],
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m2[*Raman Tensor*],
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[$mat(a,,;,a,;,,b)$], [$0$],
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[$mat(,,a;,,;a,,;)$], [$mat(,,;,,a;,a,;)$], [$mat(,a,;a,,;,,;)$], [$mat(a,,;,-a,;,,;)$],
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)},
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caption: [
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Irreducible representations and raman tensors of phonons in 4H-SiC.
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],
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placement: none,
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)<table-rep>
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