Raman Spectroscopy is the technique that provides detailed information about chemical structure, phase and polymorphy, crystallinity, and molecular interactions.
Raman Effect in Raman Spectroscopy
When the light of a definite frequency is passed through a gas, liquid, or solid and the scattered light is observed at right angles to the incident light, the scattered light is found to contain some additional frequency over and above that of incident frequency. The series of lines in the scattered light is the Raman spectrum (lines) and the phenomenon is known as Raman Effect.
Raleigh Scattering or Raleigh Line in Raman Spectroscopy
In Raman spectroscopy, for the scattered light, the line which has the same frequency as that of incident light is known as Raleigh Lines and in such scattering is known as Raleigh Scattering.
Stoke Line and Anti-Stoke Lines in Raman Spectroscopy
In the scattered light, the lines which have frequencies lower (longer wavelength) than that of incident light are called Stokes Lines, and the lines which have frequencies higher (shorter wavelength ) than that of the incident are called Anti-Stoke Lines.
If Vi represents the frequency of incident light and Vs represents the frequency of scattered light, then the difference (Vi-Vs) is a constant characteristic of the substance exposed to light and is independent of the frequency of the incident light.
This difference (Vi-Vs) is called the Raman Frequency or Raman Shift.
It was also found that the energy change i.e. hc (Vi-Vs) corresponding to Raman Frequency always corresponds to the energy changes accompanying rotational and vibrational transitions in a molecule.
Raman Spectroscopy on the basis of Quantum Theory
According to quantum theory, Raman Spectra may be regarded as a collision between the molecules of reactants and that of photons of radiations. The collisions are of the following types,
In this collision, when the photons collide with molecules, there is neither gain nor loss of energy.
This is a perfectly elastic collision and the scattered radiations will have the same frequency as that of incident radiation. This is known as Raleigh Scattering.
There are two possibilities,
- At the time of the collision, photons lose their energy to molecules scattered.
Thus the scattered radiation is called stokes radiation has less energy and frequency than the incident radiation.
The corresponding lines produced are called stokes lines.
2. At the time of the collision, molecules lose their energy to photons. Thus, the scattered radiations called Anti-Stoke radiations have more energy and frequency than the incident radiation. The corresponding lines produced are called Anti-stokes lines.
The principles of conservation of energy can be applied to the photons molecule collision.
i.e. Total energy before collision. = Total energy after the collision.
hv + E = hv1 + E1
Where v = frequency of the incident photon.
E = energy of molecule before the collision.
v1=frequency of the incident photon.
E1= energy of molecule after the collision.
On rearranging, we get
hv1= hv + (E-E1)
v1= v = (E-E1) /h
There are following three possibilities,
[a] If E = E1, v1= v . It is Raleigh Scattering.
[b] If E < E1,v1< v .Here the scattered photons have a lower frequency. It is Stokes Lines.
[c] If E > E1,v1> v. Here the scattered photons have a higher frequency. It is Anti-Stokes Lines.
Rule of Mutual Exclusion
It is a very important rule about IR and Raman Spectra.
- The Rule of mutual exclusion states that “If a molecule has center o symmetry, then its Raman active vibrations are IR inactive and vice versa”.
- The converse of this rule is also true i.e. If for a molecule Raman and IR spectra do not have common lines then the molecules must have a center of symmetry. But if there are some common lines that coincide, then the molecule has no center of symmetry.
- The rule of mutual exclusion can be best explained by studying the example of CO2 molecule
CO2 molecules show four vibrations viz,
Symmetrical Stretching Vibrations.
- It shows an absorption band in the Raman Spectral region a 1300cm-1 and it has zero dipole moment
- Thus, it is Raman active and IR inactive.
Asymmetrical Stretching Vibrations
- It has a resultant dipole moment and shows IR absorption band at 2350 cm-1.
- But there is no change in the polarizability of the molecule.
Thus, it is IR active and Raman inactive.
Pair of Degenerate Bending Vibrations: (Symmetric)
- They differ only in direction and have the same frequency and energy hence it shows only one resultant absorption band in the IR region.
- However, during bending the polarizability of the molecule remains the same.
- Thus, it is IR active and Raman inactive.
Who discovered Raman Spectroscopy?
Sir Chandrasekhara Venkata Raman was a famous Indian physicist well known for his work in the field of scattering light defines Raman Spectroscopy. He was born on 7 November 1888 at Tiruchirappalli and died on 21 November 1970 in Bengaluru.
Raman Spectroscopy is a non-destructive chemical analysis technique that provides detailed information about chemical structures and their properties. This technique is used to detect vibrational, rotational, and other states in a molecular system, capable of probing the chemical composition of materials.
What are the three basic types of spectroscopy?
The following are basically three types of spectroscopy, atomic absorption spectroscopy (AAS), atomic emission spectroscopy (AES), and atomic fluorescence spectroscopy (AFS)
What is spectroscopy?
Spectroscopy is the study of the interaction between matter and radiation. When the light has been absorbed by the molecule there is some change in the behaviors of the molecule observed.