diff --git a/paper/others/default.typ b/paper/others/default.typ
index 1d00d0e..d13e8bd 100644
--- a/paper/others/default.typ
+++ b/paper/others/default.typ
@@ -3,3 +3,4 @@
 #include "table-bec.typ"
 #include "掺杂晶格变化.typ"
 #include "晶格变化导致的频率变化.typ"
+#include "table-nopol-full.typ"
diff --git a/paper/others/table-nopol-full.typ b/paper/others/table-nopol-full.typ
new file mode 100644
index 0000000..26fd345
--- /dev/null
+++ b/paper/others/table-nopol-full.typ
@@ -0,0 +1,67 @@
+#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 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: 22, align: center + horizon, inset: (x: 3pt, y: 5pt),
+    m2[*Number of Mode*],
+      // E2  E2     E1     2B1       A1     E1     E2     E2     A1      2B1
+      m2[1], m2[2], m2[3], [4], [5], m2[6], m2[7], m2[8], m2[9], m2[10], [11], [12],
+    //                         E2        E2        E1        2B1 A1   E1        E2        E2        A1 2B1
+    m2[*Vibration Direction*], [x], [y], [x], [y], [x], [y], m(4)[z], [x], [y], [x], [y], [x], [y], m(4)[z],
+    table.cell(rowspan: 2)[*Representation*],
+      [C#sub[6v]], m2(E2), m2(E2), m2(E1), B1, B1, m2(A1), m2(E1), m2(E2), m2(E2), m2(A1), B1, B1,
+      //           E2      E2      E1      2B1     A1      E1      E2       E2     A1      2B1
+      [C#sub[2v]], A2, A1, A2, A1, B2, B1, B1, B1, m2(A1), B2, B1, A2, A1, A2, A1, m2(A1), B1, B1,
+    // TODO: 重新检查数据是否正确（主要是正负号）
+    table.cell(rowspan: 4)[*Raman Tensor*],
+      [Non-zero components],
+        // E2            E2               E1          2B1       A1
+        [xy], [xx, -yy], [xy], [xx, -yy], [xz], [yz], m2[None], [xx, yy], [zz],
+        // E1       E2               E2               A1              2B1
+        [xz], [yz], [xy], [xx, -yy], [xy], [xx, -yy], [xx, yy], [zz], m2[None],
+      [Analysis result (a.u.)],
+        // E2                            E2                        E1                         2B1
+        m2[$2epsilon_2-2zeta_2-4eta_2$], m2[$2epsilon_2-2zeta_2$], m2[$-2epsilon_1-2zeta_1$], m2[-],
+        // A1                         E1                       E2
+        [$-2epsilon_5$], [$-2epsilon_6$], m2[$-2epsilon_1+2zeta_1$], m2[$8a_2+2epsilon_2-2zeta_2-4eta_2$],
+        // E2                      A1                          2B1
+        m2[$-2epsilon_2+2zeta_2$], [$-2zeta_5$], [$-2zeta_6$], m2[-],
+      [Calculation result (a.u.)],
+        // TODO: 改正正负号
+        // E2     E2        E1        2B1    A1              E1        E2         E2        A1              2B1
+        m2[0.17], m2[1.13], m2[2.43], m2[-], [2.83], [1.79], m2[0.09], m2[88.54], m2[0.50], [0.01], [1.78], m2[-],
+      [Experiment result (a.u.)],
+        // TODO: 填充
+        // E2 E2    E1    2B1    A1      E1             E2    E2 A1              2B1
+        m2[], m2[], m2[], m2[-], [], [], m2[Invisible], m2[], m3[Invisible], [], m2[-],
+    table.cell(rowspan: 3)[*Frequency*],
+      [Simulation (cm#super[-1])],
+        // E2       E2          E1          2B1                 A1
+        m2[190.51], m2[197.84], m2[257.35], [389.96], [397.49], m2[591.90],
+        // E1       E2          E2          A1          2B1
+        m2[746.91], m2[756.25], m2[764.33], m2[812.87], [885.68], [894.13],
+      [Experiment (cm#super[-1])],
+        // E2      E2         E1         2B1    A1         E1             E2       E2 A1                   2B1
+        m2[195.5], m2[203.3], m2[269.7], m2[-], m2[609.5], m2[Invisible], m2[776], m(3)[Invisible], [839], m2[-],
+      //           E2       E2       E1       2B1    A1       E1     E2       E2 A1           2B1
+      [Error (%)], m2[2.6], m2[2.7], m2[4.6], m2[-], m2[2.9], m2[-], m2[2.5], m(3)[-], [3.1], m2[-],
+    table.cell(rowspan: 2)[*FWHM* (cm#super[-1])],
+      //            E2        E2        E1        2B1    A1        E1        E2        E2        A1        2B1
+      [Simulation], m2[0.08], m2[0.09], m2[0.08], m2[-], m2[0.61], m2[3.97], m2[4.62], m2[4.01], m2[0.89], m2[-],
+      // TODO: 选取合适的实验并填充数据
+      [Experiment, zxxz],
+        // E2     E2        E1        2B1    A1        E1             E2        E2 A1              2B1
+        m2[2.61], m2[2.09], m2[1.98], m2[-], m2[2.64], m2[Invisible], m2[3.27], m3[Invisible], [], m2[-],
+    //              E2 E2       E1        2B1       A1 E1       E2 E2       A1          2B1
+    m2[*Polarity*], m(4)[None], m2[Weak], m2[None], m(4)[Weak], m(4)[None], m2[Weak], m2[None],
+  )},
+  caption: [Negaligible-polarized Phonons at $Gamma$ Point.],
+)<table-nopol-full>]
diff --git a/paper/result/perfect/non-polar/figure-raman.typ b/paper/result/perfect/non-polar/figure-raman.typ
index 272765f..e77a139 100644
--- a/paper/result/perfect/non-polar/figure-raman.typ
+++ b/paper/result/perfect/non-polar/figure-raman.typ
@@ -1,5 +1,5 @@
 #figure(
-  image("/画图/拉曼整体图/main.svg"),
+  image("/画图/拉曼整体图/embed.svg"),
   caption: [
     (a) Phonon dispersion of 4H-SiC along the A–#sym.Gamma–K high-symmetry path.
       Gray lines represent negligible-polar phonon modes,
diff --git a/paper/result/perfect/non-polar/table-nopol.typ b/paper/result/perfect/non-polar/table-nopol.typ
index c9f52c6..dfa84de 100644
--- a/paper/result/perfect/non-polar/table-nopol.typ
+++ b/paper/result/perfect/non-polar/table-nopol.typ
@@ -4,64 +4,39 @@
   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]];
-  table(columns: 22, align: center + horizon, inset: (x: 3pt, y: 5pt),
-    m2[*Number of Mode*],
-      // E2  E2     E1     2B1       A1     E1     E2     E2     A1      2B1
-      m2[1], m2[2], m2[3], [4], [5], m2[6], m2[7], m2[8], m2[9], m2[10], [11], [12],
-    //                         E2        E2        E1        2B1 A1   E1        E2        E2        A1 2B1
-    m2[*Vibration Direction*], [x], [y], [x], [y], [x], [y], m(4)[z], [x], [y], [x], [y], [x], [y], m(4)[z],
-    table.cell(rowspan: 2)[*Representation*],
-      [C#sub[6v]], m2(E2), m2(E2), m2(E1), B1, B1, m2(A1), m2(E1), m2(E2), m2(E2), m2(A1), B1, B1,
-      //           E2      E2      E1      2B1     A1      E1      E2       E2     A1      2B1
-      [C#sub[2v]], A2, A1, A2, A1, B2, B1, B1, B1, m2(A1), B2, B1, A2, A1, A2, A1, m2(A1), B1, B1,
-    // TODO: 重新检查数据是否正确（主要是正负号）
-    table.cell(rowspan: 4)[*Raman Tensor*],
-      [Non-zero components],
-        // E2            E2               E1          2B1       A1
-        [xy], [xx, -yy], [xy], [xx, -yy], [xz], [yz], m2[None], [xx, yy], [zz],
-        // E1       E2               E2               A1              2B1
-        [xz], [yz], [xy], [xx, -yy], [xy], [xx, -yy], [xx, yy], [zz], m2[None],
-      [Analysis result (a.u.)],
-        // E2                            E2                        E1                         2B1
-        m2[$2epsilon_2-2zeta_2-4eta_2$], m2[$2epsilon_2-2zeta_2$], m2[$-2epsilon_1-2zeta_1$], m2[-],
-        // A1                         E1                       E2
-        [$-2epsilon_5$], [$-2epsilon_6$], m2[$-2epsilon_1+2zeta_1$], m2[$8a_2+2epsilon_2-2zeta_2-4eta_2$],
-        // E2                      A1                          2B1
-        m2[$-2epsilon_2+2zeta_2$], [$-2zeta_5$], [$-2zeta_6$], m2[-],
-      [Calculation result (a.u.)],
-        // TODO: 改正正负号
-        // E2     E2        E1        2B1    A1              E1        E2         E2        A1              2B1
-        m2[0.17], m2[1.13], m2[2.43], m2[-], [2.83], [1.79], m2[0.09], m2[88.54], m2[0.50], [0.01], [1.78], m2[-],
-      [Experiment result (a.u.)],
-        // TODO: 填充
-        // E2 E2    E1    2B1    A1      E1             E2    E2 A1              2B1
-        m2[], m2[], m2[], m2[-], [], [], m2[Invisible], m2[], m3[Invisible], [], m2[-],
+  table(columns: 12, align: center + horizon,
+    m2[*Notation of Mode*],
+      [E#sub[2]-1], [E#sub[2]-2], [E#sub[1]-1], m2[A#sub[1]-1],
+      [E#sub[1]-2], [E#sub[2]-3], [E#sub[2]-4], m2[A#sub[1]-2],
     table.cell(rowspan: 3)[*Frequency*],
       [Simulation (cm#super[-1])],
-        // E2       E2          E1          2B1                 A1
-        m2[190.51], m2[197.84], m2[257.35], [389.96], [397.49], m2[591.90],
-        // E1       E2          E2          A1          2B1
-        m2[746.91], m2[756.25], m2[764.33], m2[812.87], [885.68], [894.13],
+        // E2     E2        E1        A1          E1        E2        E2        A1
+        [190.51], [197.84], [257.35], m2[591.90], [746.91], [756.25], [764.33], m2[812.87],
       [Experiment (cm#super[-1])],
-        // E2      E2         E1         2B1    A1         E1             E2       E2 A1                   2B1
-        m2[195.5], m2[203.3], m2[269.7], m2[-], m2[609.5], m2[Invisible], m2[776], m(3)[Invisible], [839], m2[-],
-      //           E2       E2       E1       2B1    A1       E1     E2       E2 A1           2B1
-      [Error (%)], m2[2.6], m2[2.7], m2[4.6], m2[-], m2[2.9], m2[-], m2[2.5], m(3)[-], [3.1], m2[-],
-    table.cell(rowspan: 2)[*FWHM* (cm#super[-1])],
-      //            E2        E2        E1        2B1    A1        E1        E2        E2        A1        2B1
-      [Simulation], m2[0.08], m2[0.09], m2[0.08], m2[-], m2[0.61], m2[3.97], m2[4.62], m2[4.01], m2[0.89], m2[-],
-      // TODO: 选取合适的实验并填充数据
-      [Experiment, zxxz],
-        // E2     E2        E1        2B1    A1        E1             E2        E2 A1              2B1
-        m2[2.61], m2[2.09], m2[1.98], m2[-], m2[2.64], m2[Invisible], m2[3.27], m3[Invisible], [], m2[-],
-    //              E2 E2       E1        2B1       A1 E1       E2 E2       A1          2B1
-    m2[*Polarity*], m(4)[None], m2[Weak], m2[None], m(4)[Weak], m(4)[None], m2[Weak], m2[None],
+        // E2    E2       E1       A1         E1           E2     E2           A1
+        [195.5], [203.3], [269.7], m2[609.5], [Invisible], [776], [Invisible], m2[839],
+      //           E2     E2     E1     A1       E1   E2     E2   A1
+      [Error (%)], [2.6], [2.7], [4.6], m2[2.9], [-], [2.5], [-], m2[3.1],
+    // TODO: 重新检查数据是否正确（主要是正负号）
+    table.cell(rowspan: 4)[*Raman Tensor*],
+    [Non-zero components],
+        // E2          E2             E1        A1
+        [xy, xx, -yy], [xy, xx, -yy], [xz, yz], [xx, yy], [zz],
+        // E1     E2             E2             A1
+        [xz, yz], [xy, xx, -yy], [xy, xx, -yy], [xx, yy], [zz],
+    [Analysis result (a.u.)],
+    // E2                          E2                      E1                       A1  
+    [$2epsilon_2-2zeta_2-4eta_2$], [$2epsilon_2-2zeta_2$], [$-2epsilon_1-2zeta_1$], [$-2epsilon_5$], [$-2epsilon_6$],
+    // E1                    E2                                  E2                       A1  
+    [$-2epsilon_1+2zeta_1$], [$8a_2+2epsilon_2-2zeta_2-4eta_2$], [$-2epsilon_2+2zeta_2$], [$-2zeta_5$], [$-2zeta_6$],
+    [Calculation result (a.u.)],
+      // TODO: 改正正负号
+      // E2   E2      E1      A1              E1      E2       E2      A1
+      [0.17], [1.13], [2.43], [2.83], [1.79], [0.09], [88.54], [0.50], [0.01], [1.78],
+    [Experiment result (a.u.)],
+      // TODO: 填充
+      // E2 E2 E1 A1      E1           E2  E2           A1
+      [], [], [], [], [], [Invisible], [], [Invisible], [Invisible], [],
   )},
   caption: [Negaligible-polarized Phonons at $Gamma$ Point.],
 )<table-nopol>]
diff --git a/slide/main.typ b/slide/main.typ
index 38f8c7e..e634481 100644
--- a/slide/main.typ
+++ b/slide/main.typ
@@ -82,8 +82,6 @@
 - 由于SiC的折射率较大，导致略入射中，起作用的散射角只有大约 25#sym.degree。
 - 由于对焦困难，掠入射的情况下，光谱精细度远远不如其它两种情况（尽管已将积分时间大大延长）。
 
-// TODO: 旋转坐标轴
-
 #figure(
   image("/画图/入射方向/main.svg"),
   placement: none,
@@ -121,10 +119,13 @@
   - 强极性模式，长程库伦相互作用导致声子性质对波矢方向敏感，Gamma 点附近不连续，不同方向的散射结果有明显差别。
 
 #figure(
-  image("/画图/声子不连续/embed.svg"),
+  image("/画图/声子不连续/embed.svg"), 
   placement: none,
 )<figure-discont>
 
+#figure(
+  image("/画图/拉曼整体图/embed.svg"),
+)
 
 // 文章结构如下：
 // 
@@ -157,10 +158,13 @@
   - 缺少的 1E#sub[1]+1E#sub[2] 可以解释为，被附近非常强的峰淹没了。
   - 缺少的 1A#sub[1] 对基平面内偏振光的散射很弱、但对 c 轴偏振的散射光较强，因此可以在肩入射/掠入射中看到。
 
+表格见文章。
+
+// TODO: 画一个图，表明峰高的差别；或者，和前面的图合并。
+
 == 极性模式
 
 - 极性模式的散射强度都比较大。
 - 在不同入射方向下，极性模式最多会呈现出三个峰。
 
-
 // TODO: 拟合时不考虑fano共振，结果有些不好。是否将它考虑进去再拟合？
diff --git a/画图/入射方向/main.svg b/画图/入射方向/main.svg
index 797d1b3..503c3f3 100644
--- a/画图/入射方向/main.svg
+++ b/画图/入射方向/main.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:507618b7e7d114b9d67b283e0f51e8f16c864907f425b0cef7be0f51cdbdb0ef
-size 22534
+oid sha256:ec7145ec8750ad73ad9bae4581f720702cec52c830fb3295e787320744d64638
+size 20832
diff --git a/画图/声子不连续/embed.svg b/画图/声子不连续/embed.svg
index 79d8af8..d5172ab 100644
--- a/画图/声子不连续/embed.svg
+++ b/画图/声子不连续/embed.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:c00e3a1a7487057ae3b7885612d97d3c3e4117d025ad2c26a2e6c72cde5989b1
-size 612543
+oid sha256:b8adade703512323dd047f177c7f5814742532f5defcb42576a0344664c3d497
+size 614965
diff --git a/画图/声子不连续/main.svg b/画图/声子不连续/main.svg
index 9833d5f..e2e6810 100644
--- a/画图/声子不连续/main.svg
+++ b/画图/声子不连续/main.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:ee1b54c9c46a1ef6f7c4f022f149bc76a9064b4ef7f6b31879bc9471ee5e04d8
-size 61206
+oid sha256:4fe2a73d591b053db1a729fb61c7145619cc5a219d037d41478fd2a45a8175a0
+size 94855
diff --git a/画图/声子不连续/plot.ipynb b/画图/声子不连续/plot.ipynb
index e95dc30..431815a 100644
--- a/画图/声子不连续/plot.ipynb
+++ b/画图/声子不连续/plot.ipynb
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:90d336081e53ed0044e771e3840f4ded861f99a1b3988d8f58c60783094547bb
-size 355984
+oid sha256:89fcc1ca9cd49b4f3f4c8741981ab37c31752319921b4b7ee0a4ba595feb5a5d
+size 355758
diff --git a/画图/声子不连续/放大.svg b/画图/声子不连续/放大.svg
index f49df45..e39fb0c 100644
--- a/画图/声子不连续/放大.svg
+++ b/画图/声子不连续/放大.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:86bc50be54f2e8fccb2d93b58d300455a6b3048c2fc586c5fa397d0e11f63582
-size 37202
+oid sha256:187d7218cd738bfe19aba7dd6d11c5cfa6eb1c89c44564c5333e520e02e15717
+size 24384
diff --git a/画图/声子不连续/整体图.svg b/画图/声子不连续/整体图.svg
index ece5ed8..860efb0 100644
--- a/画图/声子不连续/整体图.svg
+++ b/画图/声子不连续/整体图.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:6e030b833644b1e898ddf6bc243f95c2e685bdc4d4410bc0c79238e5f4e12bc7
-size 102660
+oid sha256:d9160e442f037d10e2f9b82ab0d0750e4701dd52cc212a43503e9659e0cfda7b
+size 102764
diff --git a/画图/声子不连续/部分图.svg b/画图/声子不连续/部分图.svg
index 6b24dd1..6b66441 100644
--- a/画图/声子不连续/部分图.svg
+++ b/画图/声子不连续/部分图.svg
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
-oid sha256:dbc27205e4483744f310a3282950264e9aa76d1656678e8ad0e3114be2ab4fbd
-size 60295
+oid sha256:dee3155cf5ac61da83c0da15b68a106a91e0e150d9bb0e49401ec08844f98261
+size 60625
diff --git a/画图/拉曼整体图/embed.svg b/画图/拉曼整体图/embed.svg
new file mode 100644
index 0000000..f533e09
--- /dev/null
+++ b/画图/拉曼整体图/embed.svg
@@ -0,0 +1,3 @@
+version https://git-lfs.github.com/spec/v1
+oid sha256:5b5d843346152705c2797a03819493fa7ddc4b88d30751dd967a0299940f2a9d
+size 2203248
diff --git a/画图/拉曼整体图/export_png.py b/画图/拉曼整体图/export_png.py
index 2e66638..9d02eff 100755
--- a/画图/拉曼整体图/export_png.py
+++ b/画图/拉曼整体图/export_png.py
@@ -21,6 +21,7 @@ def export(mode_id):
   renderView1 = CreateView('RenderView')
   renderView1.ViewSize = [432, 733]
   renderView1.AxesGrid = 'Grid Axes 3D Actor'
+  renderView1.OrientationAxesVisibility = 0
   renderView1.CenterOfRotation = [0.7733228206634521, 0.8970721662044525, 4.6205607652664185]
   renderView1.StereoType = 'Crystal Eyes'
   renderView1.CameraPosition = [23.272381554100093, -35.17841635119482, 17.0208663979609]
diff --git a/画图/拉曼整体图/main.svg b/画图/拉曼整体图/main.svg
index 5d7764a..9ce73b9 100644
--- a/画图/拉曼整体图/main.svg
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diff --git a/画图/拉曼整体图/plot.ipynb b/画图/拉曼整体图/plot.ipynb
index d8b3d93..7236a04 100644
--- a/画图/拉曼整体图/plot.ipynb
+++ b/画图/拉曼整体图/plot.ipynb
@@ -1,3 +1,3 @@
 version https://git-lfs.github.com/spec/v1
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-size 1792977
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+size 1822743
diff --git a/画图/拉曼整体图/readme.md b/画图/拉曼整体图/readme.md
new file mode 100644
index 0000000..e69de29
diff --git a/画图/拉曼整体图/view.py b/画图/拉曼整体图/view.py
index 3f6d07e..69121f0 100644
--- a/画图/拉曼整体图/view.py
+++ b/画图/拉曼整体图/view.py
@@ -16,6 +16,7 @@ paraview.simple._DisableFirstRenderCameraReset()
 renderView1 = CreateView('RenderView')
 renderView1.ViewSize = [432, 733]
 renderView1.AxesGrid = 'Grid Axes 3D Actor'
+renderView1.OrientationAxesVisibility = 0
 renderView1.CenterOfRotation = [0.7733228206634521, 0.8970721662044525, 4.6205607652664185]
 renderView1.StereoType = 'Crystal Eyes'
 renderView1.CameraPosition = [23.272381554100093, -35.17841635119482, 17.0208663979609]
diff --git a/画图/拉曼整体图/拉曼-报告.svg b/画图/拉曼整体图/拉曼-报告.svg
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--- a/画图/拉曼整体图/拉曼-报告.svg
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