修改第一段

paper/method/experiment/default.typ

@@ -89,4 +89,6 @@ This was confirmed by the results under different polarization configurations an
 
 对齐：正入射、xyyx 使用 E23 对齐，其它则无法对齐，看情况处理。
 
+只考虑了沿 zOx 平面入射的情况。
+
 #include "figure-e1.typ"

paper/result/perfect/default.typ

@@ -2,26 +2,29 @@
 
 // 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。
 
-Owing to the distinct behaviors arising from different electrical polarities of Raman-active phonon modes,
-  they were categorized into two groups:
-  negligible-polarity phonons (i.e., having zero or very weak electrical polarity),
-  and strong-polarity phonons.
-The negligible-polarity phonons exhibited minimal dependence on the wavevector direction
-  (see the intersection of gray solid lines and orange dashed lines in @figure-discont b and c,
-  where the frequency only differed #sym.tilde 0.1 cm#super[-1] across different incidence configurations),
-  and were therefore usually analyzed at the #sym.Gamma point regardless of the incidence configurations;
-specifically, there were eight such modes
-  labeled A#sub[1]-1 to A#sub[1]-2, E#sub[1]-1 to E#sub[1]-2, and E#sub[2]-1 to E#sub[2]-4,
-  according to their irreducible representations in the C#sub[6v] group and in order of increasing frequency.
-In contrast, the strong-polarity phonons displayed significant anisotropy
-  (see the intersection of colored solid lines and orange dashed lines in @figure-discont b and c,
-  where the frequency differed #sym.tilde 10 cm#super[-1] across different incidence configurations),
-  and required analysis under specific incidence configurations.
-In this paper, we focused on incidence within the zOx plane,
-  where three modes were present and named according to their vibration directions:
-  TO-zOx (vibrating in the zOx plane and roughly perpendicular to the incidence direction),
+Raman-active phonon modes were categorized into two groups,
+  according to the distinct behaviors arising from different electrical polarities,
+  including eight negligible-polarity modes (i.e., having zero or very weak electrical polarity),
+  and three strong-polarity modes.
+The negligible-polarity modes exhibited minimal dependence on the wavevector direction,
+  while the strong-polarity modes showed significant anisotropy.
+This distinction was clearly illustrated in @figure-discont,
+  where the phonon dispersion relations of negligible-polarity modes (gray solid lines)
+    were roughly continuous and flat at the #sym.Gamma point,
+  leading to only #sym.tilde 0.1 cm#super[-1] frequency variations and similar vibration patterns
+    across different incidence configurations.
+In contrast, the strong-polarity modes (colored solid lines) displayed discontinuities at the #sym.Gamma point,
+  resulting in #sym.tilde 1 cm#super[-1] frequency shifts and distinct different vibration patterns
+  under different incidence configurations.
+Consequently, the negligible-polarity modes were named
+  according to their irreducible representations at the #sym.Gamma point and in order of increasing frequency,
+  including A#sub[1]-1 to A#sub[1]-2, E#sub[1]-1 to E#sub[1]-2, and E#sub[2]-1 to E#sub[2]-4.
+In contrast, the strong-polarity modes were named according to their vibration directions and incidence configurations,
+  including TO-zOx (vibrating in the zOx plane and roughly perpendicular to the incidence direction),
   TO-y (vibrating along the y-axis), and LO (vibrating roughly parallel to the incidence direction).
 
+#include "figure-discont.typ"
+
 In order to further investigate the frequencies dependence on the wavevector,
   and to confirm the accuracy of both our experiments and calculations,
   we analyzed the negligible-polarity phonons off the #sym.Gamma point
@@ -36,7 +39,7 @@ The E#sub[2]-3 peak served as a calibration reference under various experiments,
 
 === Negligible-polarity Phonons
 
-#include "figure-discont.typ"
+
 #include "figure-raman.typ"
 
 Peaks corresponding to seven Raman-active negligible-polarity phonons were observed in our experiments