diff --git a/test-typst/main.typ b/test-typst/main.typ
index 0adf118..85a5e78 100644
--- a/test-typst/main.typ
+++ b/test-typst/main.typ
@@ -731,6 +731,8 @@ Furthermore, we list predicted modes and their Raman tensors, in @table-predmode
   placement: none,
 )<table-singleatom>]
 
+#include "掺杂晶格变化.typ"
+#include "晶格变化导致的频率变化.typ"
 
 // TODO: 这句话放哪里？
 // whose dispersion curves exhibit discontinuity near the #sym.Gamma point (also shown in @phonon),
diff --git a/test-typst/掺杂晶格变化.typ b/test-typst/掺杂晶格变化.typ
new file mode 100644
index 0000000..6b527d7
--- /dev/null
+++ b/test-typst/掺杂晶格变化.typ
@@ -0,0 +1,16 @@
+#figure({
+  set par(justify: false);
+  table(columns: 5, align: center + horizon,
+    table.cell(colspan: 2, rowspan: 2)[*Defect Type*],
+      table.cell(colspan: 3)[*Variation of Lattice Constant (#sym.permille)*], [x], [y], [z],
+    table.cell(rowspan: 2)[N#sub[C]], [h], [-0.47], [-0.48], [-0.70], [k], [-0.60], [-0.62], [-0.38],
+    table.cell(rowspan: 2)[Al#sub[Si]], [h], [0.71], [0.78], [1.02], [k], [0.72], [0.80], [1.01],
+    table.cell(rowspan: 2)[V#sub[C]], [h], [-0.88], [-1.85], [1.92], [k], [-0.47], [-1.02], [0.45],
+    table.cell(rowspan: 2)[V#sub[Si]], [h], [0.53], [0.64], [0.37], [k], [0.49], [0.58], [0.66],
+    table.cell(rowspan: 4)[N#sub[C]+C#sub[Si]],
+      [h, C#sub[3v]], [0.33], [1.44], [3.25], [k, C#sub[3v]], [0.28], [1.22], [3.51],
+      [h, C#sub[v]], [1.86], [0.60], [2.24], [k, C#sub[v]], [2.05], [1.10], [1.63],
+  )},
+  caption: [Variation of Lattice Constant caused by Defects],
+  placement: none,
+)<table-dope>
diff --git a/test-typst/晶格变化导致的频率变化.typ b/test-typst/晶格变化导致的频率变化.typ
new file mode 100644
index 0000000..554f0e0
--- /dev/null
+++ b/test-typst/晶格变化导致的频率变化.typ
@@ -0,0 +1,28 @@
+#page(flipped: true)[#figure({
+  set par(justify: false);
+  table(columns: 12, align: center + horizon, // inset: (x: 3pt, y: 5pt),
+    table.cell(rowspan: 3)[*Variation of Lattice Constant*],
+      table.cell(colspan: 11)[*Variation of Frequency (cm#super[-1])*],
+      table.cell(colspan: 6)[*Negligible-polar Phonons*],
+      table.cell(colspan: 2)[*Strong-polar Phonons (z)*], table.cell(colspan: 3)[*Strong-polar Phonons (y)*],
+      [E#sub[2] at 195.5 cm#super[-1]], [E#sub[2] at 203.3 cm#super[-1]], [E#sub[1] at 269.7 cm#super[-1]],
+      [A#sub[1] at 609.5 cm#super[-1]], [E#sub[2] at 776 cm#super[-1]], [A#sub[1] at 839 cm#super[-1]],
+      [E#sub[1] at 795 cm#super[-1]], [A#sub[2] at 963 cm#super[-1]],
+      [z at 782 cm#super[-1]], [x at 796 cm#super[-1]], [y at ? cm#super[-1]],
+    [In-plane, expand $1 permille$], [0.00], [0.02], [0.05], [-0.75], [-2.21], [-1.17], [-2.14], [-1.30], [-1.00], [-2.14], [-2.35], 
+    [In-plane, shrink $1 permille$], [0.00], [-0.01], [-0.04], [0.76], [2.21], [1.16], [2.13], [1.31], [1.02], [2.13], [2.35], 
+    [Out-of-plane, expand $1 permille$], [-0.03], [-0.09], [0.02], [-0.95], [-0.58], [-1.64], [-0.49], [-1.69], [-1.55], [-0.49], [-0.69], 
+    [Out-of-plane, shrink $1 permille$], [0.00], [0.08], [-0.05], [0.93], [0.57], [1.61], [0.49], [1.69], [1.55], [0.49], [0.69], 
+    [x, expand $1 permille$], [-0.09], [-0.08], [-0.08], [-0.38], [-1.38], [-0.59], [-1.37], [-0.65], [-0.49], [-1.33], [-0.98], 
+    [x, shrink $1 permille$], [-0.09], [-0.10], [-0.12], [0.38], [0.83], [0.58], [0.77], [0.65], [0.53], [1.32], [0.98], 
+  )},
+  caption: ["Raman tensor" caused by single atom],
+  placement: none,
+)<table-dope>]
+
+      // E2        E2           E1           2B1      A1
+      // m(3)[195.5], m(3)[203.3], m(2)[269.7], m(2)[-], m(3)[609.5],
+      // E1    E2         E2 A1           2B1
+      // m(2)[-], m(3)[776], m(5)[-], [839], m(2)[-],
+      //         // z                        y                                 45 y&z
+      // m(2)[776.57], m(3)[933.80], m(3)[761.80], [776.57], [941.33], m(4)[762.76], [776.57], m(4)[940.86],
\ No newline at end of file