大量小调整

paper/others/table-pol-full.typ

@@ -0,0 +1,41 @@
+  #figure({
+    set text(size: 9pt);
+    set par(justify: false);
+    let m(n, content) = table.cell(colspan: n, content);
+    let m2(content) = table.cell(colspan: 2, content);
+    let m3(content) = table.cell(colspan: 3, content);
+    let A1 = [A#sub[1]];
+    let A2 = [A#sub[2]];
+    let B1 = [B#sub[1]];
+    let B2 = [B#sub[2]];
+    let E1 = [E#sub[1]];
+    let E2 = [E#sub[2]];
+    let NA = [Not Applicable]
+    let lopc = [Yes#linebreak() (LOPC)];
+    let overf = [Yes#linebreak() (overfocused)];
+    table(columns: 19, align: center + horizon, inset: (x: 3pt, y: 5pt),
+      m2[*Incident Direction*], m(4)[z], m(5)[y], m(8)[between z and y, 20#sym.degree to z],
+      m2[*Vibration Direction*],
+        // TODO: check LO-TO mixed
+        [TO (x)], [TO (y)], m2[LO (z)], m3[TO (z)], [TO (x)], [LO (y)], m3[TO (y-z mixed)], [TO (x)], m(4)[LO (y-z mixed)],
+      table.cell(rowspan: 2)[*Representation*],
+        [C#sub[6v]], m2(E1), m2(A1), m(13, NA), [C#sub[2v]], B2, B1, m2(A1), m2(A1), B2, B1, m(9, NA),
+      table.cell(rowspan: 2)[*Raman Tensor*],
+        [Non-zero components],
+          [xz], [yz], [xx, yy], [zz],                         // z
+          [xx, yy], [zz], [xz], [yz],                         // y
+          [xx], [yy], [yz], [zz], [xz], [xx], [yy], [yz], [zz], // 25 y&z
+      [Simulation Result (a.u.)],
+        // TODO: raman intensity, or raman tensor?
+        m2[53.52], [58.26], [464.69],                                   // z
+        [58.26], [454.09], [53.52], [53.55],                              // y
+        m2[53.71], [3.20], [425.98], [53.56], m2[3.60], [50.36], [27.99], // 45 y&z
+      m2[*Visible in Common Raman Experiment*], m(17)[Yes],
+      m2[*Wavenumber (Simulation) (cm#super[-1])*],
+        // z                        y                                 45 y&z
+        m2[776.57], m2[933.80], m2[761.80], [776.57], [941.33], m(4)[762.76], [776.57], m(4)[940.86],
+      m2[*Electrical Polarity*], m(17)[Strong]
+    )},
+    caption: [Strong-polarized phonons near $Gamma$ point],
+  )
+<table-pol>

paper/others/table-rep.typ

@@ -0,0 +1,24 @@
+#figure({
+  set text(size: 9pt);
+  set par(justify: false);
+  let m2(content) = table.cell(colspan: 2, content);
+  let A1 = [A#sub[1]];
+  let A2 = [A#sub[2]];
+  let B1 = [B#sub[1]];
+  let B2 = [B#sub[2]];
+  let E1 = [E#sub[1]];
+  let E2 = [E#sub[2]];
+  table(columns: 8, align: center + horizon,
+    table.cell(rowspan: 2)[*Representation*],
+      [C#sub[6v]], A1, B1, m2(E1), m2(E2),
+      [C#sub[2v]], A1, B1, B2, B1, A2, A1,
+    m2[*Vibration Direction*], [z], [z], [x], [y], [x], [y],
+    m2[*Raman Tensor*],
+      [$mat(a,,;,a,;,,b)$], [$0$],
+      [$mat(,,a;,,;a,,;)$], [$mat(,,;,,a;,a,;)$], [$mat(,a,;a,,;,,;)$], [$mat(a,,;,-a,;,,;)$],
+  )},
+  caption: [
+    Irreducible representations and raman tensors of phonons in 4H-SiC.
+  ],
+  placement: none,
+)<table-rep>

paper/result/perfect/default.typ

@@ -1,7 +1,5 @@
 == Phonons in Perfect 4H-SiC
 
-// 第一段：弱极性与强极性声子模式表现截然不同。如图所示，弱极性声子模式几乎不依赖于波矢方向，而强极性声子模式则表现出显著的各向异性。
-
 Raman-active phonon modes were categorized into two groups,
   according to the distinct behaviors arising from different electrical polarities,
   including eight negligible-polarity modes (possessing zero or very weak polarity),
@@ -51,6 +49,8 @@ However, the E#sub[1]-2 mode was observable in our experiments of y(zx)#overline
 Our experiments reported the observation of the E#sub[1]-2 peak for the first time,
   and explained the discrepancy among previous experiments and ours with the help of our calculations.
 
+#include "figure-raman.typ"
+
 It is noteworthy that the large variation in Raman tensor magnitudes among different modes
   was not yet theoretically understood.
 For example, the Raman tensor of the E#sub[2]-3 mode was substantially larger
@@ -72,103 +72,19 @@ Notably, the E#sub[2]-3 mode was the only mode that retains the $a_i$ term,deter
 This stood in contrast to other negligible-polarity modes where such contributions tend to cancel out,
   explaining the exceptionally high Raman tensor magnitude observed for the E#sub[2]-3 mode.
 
+#page(flipped: true)[
+#include "table-nopol.typ"
+#include "table-pol.typ"
+]
+
 The mode frequency dependence on the wavevector were thoroughly investigated,
-  including both thoretical calculations (@figure-rev a), experimental measurements (@figure-rev b)
-  and their comparisons (@figure-rev c).
+  including both thoretical calculations (@figure-rev a), experimental measurements (left part of @figure-rev b) and their comparisons (right part of @figure-rev b).
 The E#sub[2]-3 mode frequency was calculated to remaine distinct in all incidence geometries (@figure-rev a),
   making it an ideal calibration reference for experiments.
 Meanwhile,
   the E#sub[2]-1, E#sub[2]-2 and A#sub[1]-1 mode showed a relatively larger dependence on the incidence direction,
-  which is in good agreement with our experimental observations (@figure-rev c).
-
-
-// TODO: 图中标注强调是拉曼活性的模式
-// TODO: b 图的标题歪了
-
-#include "figure-raman.typ"
-
-#include "table-nopol.typ"
-
-#include "table-pol.typ"
-
-// TODO: 合并两个表格到一页，删除 polar 中的多余信息
-
-
-
-
-
-
+  which is in good agreement with our experimental observations (@figure-rev b).
 
 #include "figure-rev.typ"
 
-#include "figure-discont.typ"
-
-
-The E#sub[2]-3 peak was calculated to be having virtually invariant frequency,
-  and thus served as a calibration reference under various experiments.
-The peek of E#sub[2]-1, E#sub[2]-2, A#sub[1]-1 and TO-zOx modes were observable in both normal and edge incidence,
-  thus was uesd to compare the frequency shifts between different incidence configurations.
-
-// TODO: 增加图例：各种入射激光
-// TODO: 增加 TO-zOx 的讨论
-// TODO: 条形图画成两个方向的
 // TODO: 换个方案拟合，考虑不对称，看能不能把这个误差填上
-
-// 第二段：我们具体计算了模式对极性的依赖。可以看到，弱极性声子的变化极小。与实验比较，也验证了我们实验的准确性。
-
-// 第三段：有两个弱极性模式还没有在实验上看到过。我们通过计算知道了它们的强度，并看到了其中一个。
-
-// 第四段：声子模式的强度可以从理论上得到解释。
-
-=== Negligible-polarity Phonons
-
-
-
-
-
-
-
-
-To achieve a more precise investigation of the Raman spectra
-    and prepare for analyzing impurity and charge carrier effects,
-  the analysis of negligible-polarity phonons off the #sym.Gamma point was conducted
-  by comparing experimental and calculated results under various lazer incidence directions.
-The E#sub[2]-3 peak searved as a calibration reference under various experiments,
-  since its position was calculated to be virtually invariant between normal and edge incidence
-  (with a shift of only #sym.tilde 0.004 cm#super[-1]).
-The E#sub[2]-1, E#sub[2]-2, and A#sub[1]-1 modes exhibited observable shifts,
-  and the experimental results were in good agreement with our calculations, as shown in fig.
-Our results further confirmed the accuracy of both our experiments and calculations.
-
-=== Strong-polarity Phonons
-
-The Strong-polarity phonon modes participated in Raman scattering
-  exhibited significant variations depending on the incidence configurations
-  (see the intersection of colored solid lines and orange dashed lines in @figure-discont b and c).
-For incident light propagating along the z direction,
-  the C#sub[6v] point group applied and two modes were present,
-  marked as normal-TO and normal-LO,
-  and they were corresponding to the E#sub[1] and A#sub[1] representations
-    and vibrations along the basle plane and z direction, respectively.
-The normal-LO would subsiquently couple with plasmons to form LOPC modes in n-type 4H-SiC.
-For incident light propagating along other directions,
-  the C#sub[6v] group no longer held and three modes were present.
-Specifically, for incident light propagating along x direction, the C#sub[2v] group applied,
-  and the three modes was named as edge-TO-z, edge-TO-y and edge-LO,
-  which were corresponding to A#sub[1], B#sub[2] and B#sub[1] representations
-  and vibrations along z, y and x directions, respectively.
-
-E1 的情况。
-
-注意到在正入射中，理论上不能被观察到的E#sub[1]-1模式也被观察到了。
-与弱极性的 E1-1 模式类似，我们也认为这是由于入射光并非完全沿 z 轴入射所致。
-但与弱极性 E1-1 模式不同的是，强极性 E1-1 模式在 xy 的偏振下并没有更强反而更弱。
-这是因为E1这时不再是严格的E1模式，而是分裂成了两个相近的模式。
-我们的计算表明，在2度的入射角下，E1分裂的两个模式非常接近。
-其中某个模式会怎样怎样，另一个会怎样怎样。
-
-// 我们预测，随着入射方向偏移，LO 峰会向着高频方向移动。此外，我们也注意到 LO 也会与载流子产生影响。
-// 在 n 型半导体中，LOPC 模式将代替 LO 模式；在 p 型半导体中，LO 模式仍然单独存在，但它的半高宽会受到载流子浓度的影响。
-
-
-

paper/result/perfect/figure-raman.typ

@@ -1,7 +1,7 @@
 #figure(
   image("/画图/拉曼整体图/embed.svg"),
   caption: [
-    Phonon modes and corresponding Raman spectra of 4H-SiC.
+    Raman-active phonon modes and corresponding Raman spectra of 4H-SiC.
     (a)-(b) Raman spectra with (a) normal and (b) edge incidence configurations.
   ],
   placement: none

paper/result/perfect/figure-rev.typ

@@ -1,18 +1,10 @@
 #figure(
   image("/画图/入射角度与偏移/embed.svg"),
   caption: [
-    Phonon modes and corresponding Raman spectra of 4H-SiC.
-    (a)-(b) Raman spectra with (a) normal and (b) edge incidence configurations.
+    Frequency shifts of Raman-active modes depending on wavevectors.
+    (a) Calculated results.
+    (b) Experimental results and theoretical comparison.
   ],
   placement: none
 )<figure-rev>
 
-// #figure(
-//   image("/画图/弱极性不同方向偏移/embed.svg"),
-//   caption: [
-//     Frequency shifts of negligible-polar phonon modes under different incidence configurations.
-//     (a) Experimental results under z(yy)#overline[z] and x(yy)#overline[x] configurations. Solid lines and dots represent distribution and value of experimental data, respectively.
-//     (b) Comparison between experimental and calculated frequency shifts. The baby blue bars and error bars represent the mean and standard deviation of experimental results, respectively; the purple bars represent theoretical calculations.
-//   ],
-//   placement: none
-// )<fig-nopo-diff>

paper/result/perfect/table-nopol.typ

@@ -1,5 +1,5 @@
 // 拟合结果位于 画图/拉曼结果拟合/250923
-#page(flipped: true)[#figure({
+#figure({
   set text(size: 9pt);
   set par(justify: false);
   let m(n, content) = table.cell(colspan: n, content);
@@ -50,8 +50,7 @@
   )},
   caption: [
     Negaligible-polarized Phonons at $Gamma$ Point.
-    The calculated phonon frequencies had a slight underestimation of 2-5% comparing to experimental values,
-    which might be attributed to the known tendency of the PBE functional underestimating interatomic forces (cite).
+    // The calculated phonon frequencies had a slight underestimation of 2-5% comparing to experimental values,
+    // which might be attributed to the known tendency of the PBE functional underestimating interatomic forces (cite).
   ],
-)<table-nopol>]
-
+)<table-nopol>

paper/result/perfect/table-pol.typ

@@ -1,10 +1,10 @@
-#page(flipped: true)[
   #figure({
     set text(size: 9pt);
     set par(justify: false);
     let m(n, content) = table.cell(colspan: n, content);
-    let m2(content) = table.cell(colspan: 2, content);
-    let m3(content) = table.cell(colspan: 3, content);
+    let m2(content) = m(2, content);
+    let m3(content) = m(3, content);
+    let m4(content) = m(4, content);
     let A1 = [A#sub[1]];
     let A2 = [A#sub[2]];
     let B1 = [B#sub[1]];
@@ -15,12 +15,12 @@
     let lopc = [Yes#linebreak() (LOPC)];
     let overf = [Yes#linebreak() (overfocused)];
     table(columns: 19, align: center + horizon, inset: (x: 3pt, y: 5pt),
-      m2[*Incident Direction*], m(4)[z], m(5)[y], m(8)[between z and y, 20#sym.degree to z],
-      m2[*Vibration Direction*],
-        // TODO: check LO-TO mixed
-        [TO (x)], [TO (y)], m2[LO (z)], m3[TO (z)], [TO (x)], [LO (y)], m3[TO (y-z mixed)], [TO (x)], m(4)[LO (y-z mixed)],
+      m2[*Incident Direction*], m4[z], m4[x], m(9)[between z and x, 20#sym.degree to z],
+      m2[*Notation of Mode*], [TO-x], [TO-y], m2[LO], m2[TO-z], [TO-y], [LO], m4[TO-xz], [TO-y], m4[LO],
       table.cell(rowspan: 2)[*Representation*],
-        [C#sub[6v]], m2(E1), m2(A1), m(13, NA), [C#sub[2v]], B2, B1, m2(A1), m2(A1), B2, B1, m(9, NA),
+        [C#sub[6v]], m2(E1), m2(A1), m4(NA), table.cell(rowspan: 2, colspan: 9, NA),
+        [C#sub[2v]], B1, B2, m2(A1), m2(A1), B2, B1,
+// TODO: 以下数据需要重新计算，因为x和y换过一次
       table.cell(rowspan: 2)[*Raman Tensor*],
         [Non-zero components],
           [xz], [yz], [xx, yy], [zz],                         // z
@@ -31,12 +31,10 @@
         m2[53.52], [58.26], [464.69],                                   // z
         [58.26], [454.09], [53.52], [53.55],                              // y
         m2[53.71], [3.20], [425.98], [53.56], m2[3.60], [50.36], [27.99], // 45 y&z
-      m2[*Visible in Common Raman Experiment*], m(17)[Yes],
       m2[*Wavenumber (Simulation) (cm#super[-1])*],
         // z                        y                                 45 y&z
-        m2[776.57], m2[933.80], m2[761.80], [776.57], [941.33], m(4)[762.76], [776.57], m(4)[940.86],
-      m2[*Electrical Polarity*], m(17)[Strong]
+        m2[776.57], m2[933.80], m2[761.80], [776.57], [941.33], m(4)[762.76], [776.57], m(4)[940.86]
     )},
     caption: [Strong-polarized phonons near $Gamma$ point],
   )
-<table-pol>]
+<table-pol>