拉曼散射 Raman scattering In 1928, Indian scientists C. V. Raman use a narrowband filter and sunlight to create a monochromatic light. He discovered that when light traverses a transparent material, some of the deflected light changes in wavelength, This phenomenon was then termed as the raman scattering. Raman spectroscopy is a light scattering technique, a photon of incident interacts with a sample to produce scattered light, most of the scattered light and incident light having the same wavelength, known as Rayleigh scattering. Also, the wavelength of a small amount of scattered light is different from the incident light, it's intensity of scattered light is about 10-7, which changes the wavelength determined by the chemical structure of the scattering material, known as Raman scattering.

1928年，印度科學家C. V. Raman利用太陽光和一個窄帶濾波器製造出單色光。他發現光穿過一個透明的物質，一些偏轉光的波長改變，此現象被稱為拉曼效應。
拉曼光譜是一種光散射技術，入射光子和樣品相互作用產生了散射光子，大多數散射光與入射光具有相同的波長，稱為瑞利散射。還有極小一部分散射光的波長與入射光不同，散射光強度大約是總散射光強度的10-7，其波長的改變由散射物質的化學結構所決定，稱為拉曼散射。

拉曼光譜原理 Theory of Raman The spontaneous raman effect is the incident photon exciting the molecule from ground state into a virtual energy state, When the virtual energy state emit a photon and relax back down to the ground state is different from a rotating or vibrating state, the difference in energy between the ground state and the virtual energy state leads to a shift in the emitted photon's frequency away from the excitation wavelength. If the final vibrational state of the molecule is more energetic than the initial state, the inelastically scattered photon will be shifted to a lower frequency for the total energy of the system to remain balanced. This shift in frequency is designated as a Stokes shift. If the final vibrational state is less energetic than the initial state, then the inelastically scattered photon will be shifted to a higher frequency, and this is designated as an anti-Stokes shift. Stokes shift is the larger raman scattering, Due to the fact that most molecules will be found in the ground state at room temperature.

自發拉曼效應是光子將分子從基態激發到一個虛擬的能量狀態，當激發態的分子放出一個光子後並返回到一個不同於基態的旋轉或振動狀態，在基態與新狀態間的能量差會使得釋放光子的頻率與激發光的不同。如果最終振動狀態的分子比初始狀態時能量高，所激發出來的光子頻率則較低，以確保系統的總能量守衡。這一個頻率的改變被稱為史托克位移。如果最終振動狀態的分子比初始狀態時能量低，所激發出來的光子頻率則較高，這一個頻率的改變被稱為反史托克位移。史托克位移的拉曼散射強度較大，這是因為大部分分子將在室溫下的基態中找到。

拉曼光譜應用 Applications of Raman Raman spectrum is commonly used in chemistry, since vibrational information is specific to the chemical bonds and symmetry of molecules. It provides a fingerprint by which the molecule can be identified. Raman spectrum is a very efficient and non-destructive method for analysis of a wide range of materials and system.

拉曼光譜(Raman)中的訊號提供了化學鍵、官能基的資訊， 也可以用來確認結構資訊 (例如:    甲、乙醇的化學結構差異)， 手持式拉曼光譜儀， 設計了複雜的光學路徑與組件， 利用雷射光源照射在樣品表面上, 即得到光譜資訊, 再利用儀器內部的數據庫比對物質分析結果。