diff --git a/paper/method/experiment/default.typ b/paper/method/experiment/default.typ
index cd494a8..b7ef53b 100644
--- a/paper/method/experiment/default.typ
+++ b/paper/method/experiment/default.typ
@@ -29,6 +29,8 @@ A 100 μm confocal pinhole was used for normal incidence to enhance axial (z-dir
 The integration time was set to 60 seconds for normal and edge incidence,
   while it was extended to 300 seconds for grazing incidence due to the weaker Raman signal.
 
+// 对应于入射配置的位置，计算为 1.0263158 E-3 A-1
+
 偏振的配置？
 
 #include "figure-incidence.typ"
diff --git a/paper/others/data.ods b/paper/others/data.ods
new file mode 100644
index 0000000..ec4d5c4
Binary files /dev/null and b/paper/others/data.ods differ
diff --git a/paper/result/perfect/non-polar/default.typ b/paper/result/perfect/non-polar/default.typ
index 27a944e..ab6b9ec 100644
--- a/paper/result/perfect/non-polar/default.typ
+++ b/paper/result/perfect/non-polar/default.typ
@@ -104,10 +104,11 @@ Thus, it was not typically observed in normal incidence Raman experiments (cite)
 相比于正入射，肩入射时，E2-1与E2-2的间距会减小、E2-2会展宽；E2-3会展宽，同时略微蓝移动。
 我们的计算结果为xxx，实验结果为xxx。
 
-// 198.43184855558061
+// 186.38835388124227
+// 201.84270995851526
+
+// 191.77252066290447
 // 199.03816532139587
-// 257.87910853505343
-// 258.4149982771832
 
 
 // 其它峰在其它章节中解释。
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--- a/画图/声子不连续/freq_at_edge.csv
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index 433acba..8cbce8c 100644
--- a/画图/声子不连续/freq_at_normal.csv
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