「Theory」の版間の差分
ナビゲーションに移動
検索に移動
| 5行目: | 5行目: | ||
[[File:Light.png|500px]] | [[File:Light.png|500px]] | ||
: | : The experimental geometry is described by the two-layer model in the above Figure, where phase $i$ and phase $j$ represent the substrate and sample, respectively. | ||
The incident light in phase <math>i</math> and transmitted light in phase <math>j</math> are related by Snell's law | |||
: <math> n_i \sin \theta_i = n_j \sin \theta_j </math> | |||
: | |||
---- | ---- | ||
2022年1月20日 (木) 06:36時点における版
Calculated reflectance of ATR-IR from complex refractive index
- The experimental geometry is described by the two-layer model in the above Figure, where phase $i$ and phase $j$ represent the substrate and sample, respectively.
The incident light in phase 構文解析に失敗 (MathML、ただし動作しない場合はSVGかPNGで代替（最新ブラウザーや補助ツールに推奨）: サーバー「https://wikimedia.org/api/rest_v1/」から無効な応答 ("Math extension cannot connect to Restbase."):): {\displaystyle i} and transmitted light in phase 構文解析に失敗 (MathML、ただし動作しない場合はSVGかPNGで代替（最新ブラウザーや補助ツールに推奨）: サーバー「https://wikimedia.org/api/rest_v1/」から無効な応答 ("Math extension cannot connect to Restbase."):): {\displaystyle j} are related by Snell's law
- 構文解析に失敗 (MathML、ただし動作しない場合はSVGかPNGで代替（最新ブラウザーや補助ツールに推奨）: サーバー「https://wikimedia.org/api/rest_v1/」から無効な応答 ("Math extension cannot connect to Restbase."):): {\displaystyle n_i \sin \theta_i = n_j \sin \theta_j }
Fitting procedure| How to Fit the ATR-IR spectra
Automatically determine the initial parameters in fitting procedure