paper/result/perfect/default.typ

@@ -3,14 +3,14 @@
 不同方向入射光的声子位置不同。
 
 声子的性质与它们在倒空间中的位置（即波矢）有关，而参与拉曼散射的声子波矢则由激光波长和拉曼入射配置（正入射、掠入射、边入射）决定。
-在我们的实验（绿光）中，参与拉曼散射的声子都位于 Gamma 点附近（距离仅 xxx 埃），而与 Gamma 点的相对方向则根据入射配置而定。
+在我们的实验（绿光）中，参与拉曼散射的声子都位于 Gamma 点附近（距离仅约 0.005 埃），而与 Gamma 点的相对方向则根据入射配置而定。
 对于正入射，声子大致位于 Gamma-A 线上；对于边入射，声子大致位于 Gamma-K 线上。对于掠入射，声子不位于任何高对称线上。
 
 The properties of phonons depend on their positions in reciprocal space (i.e., their wavevectors),
   and the wavevectors of phonons participating in a Raman scattering process
   are determined by the Raman experiment configuration.
 In our experiments (back-scattering with 532 nm laser light),
-  the phonons involved are located very close to the #sym.Gamma point (approximately $5.13 times 10^(-3) angstrom$),
+  the phonons involved are located very close to the #sym.Gamma point (approximately $5 times 10^(-3) angstrom$),
   and direction relative to the #sym.Gamma point is determined by the incidence configurations.
 For normal and edge incidence,
   the relevant phonons lie approximately along the #sym.Gamma–A and #sym.Gamma–K lines, respectively,