Understanding Raman Mode Representation at Specific Wave Numbers

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Discussion Overview

The discussion centers on the representation of Raman modes at specific wave numbers, particularly the labeling conventions such as E1, A1, and A2 in the context of molecular point groups and crystalline materials. Participants explore the terminology and underlying principles governing these designations in Raman spectroscopy.

Discussion Character

  • Technical explanation
  • Conceptual clarification
  • Debate/contested

Main Points Raised

  • Some participants explain that the labels E1, A1, and A2 refer to representations of the molecular point group, with the vibrational ground state transforming as A1 and excited states corresponding to other representations.
  • One participant questions why certain modes are assigned specific labels at particular wave numbers, seeking clarification on the terminology and reasoning behind these assignments.
  • Another participant notes that in crystalline media, the labels correspond to the representation of the little group associated with the wavevector k, emphasizing the standardization of these labels based on the point group.
  • A participant mentions that the assignment of symmetry labels to wavelengths is linked to the fixed energy of one quantum of vibration.
  • One participant raises a specific case regarding Aluminium Nitride, questioning why certain modes cannot be interchanged at different wave numbers.
  • Another participant suggests that the representation can be determined experimentally through the polarization and intensity of incident and scattered light.

Areas of Agreement / Disagreement

Participants express differing views on the assignment of Raman mode labels at specific wave numbers, indicating that multiple competing perspectives remain unresolved regarding the interchangeability of these labels.

Contextual Notes

There are limitations in the discussion regarding the assumptions made about the symmetry of the vibrational modes and the specific conditions under which these labels apply. The discussion does not resolve the mathematical or conceptual steps involved in the assignments.

Who May Find This Useful

This discussion may be of interest to those studying Raman spectroscopy, crystallography, or molecular symmetry, particularly in the context of material science and solid-state physics.

sajid husain
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Why we describe Raman modes At perticular wave number by E1 or A1,A2 or other
If E1 say at 645cm-1, Why we cannot describe A1 at this wave number.
How we write the representation at perticlar wave number. Please reply.
 
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These labels refer to the representation of the molecular point group.

The vibrational ground state always transforms as A1 and the excited state with one vibrational quantum transforms as some representation of the molecular symmetry group, e.g. E1. Then the excitation of one quantum of this vibration corresponds to an energy difference
##\Delta E=E_\mathrm{E1}-E_\mathrm{A1}=hc \tilde{\nu} ## where ##\tilde{\nu}## is the wavenumber of the Raman transition.
 
Actually i am discussing about the space group symmetry of crystalline material how this mode assign for this name i.e, E1,A1, at particular wave number. Why these mods name come and what terminology behind this.Please clarify
 
In crystalline media, the labels refer to the representation of the little group pertaining to the wavevector k. In Raman spectroscopy k=0, and that little group is identical to the crystallographic point group. The labels of the irreducible representations depend on the point group and are standardized. You have to look them up. For example A is a one-dimensional representation, E two dimensional and T three dimensional.
In Raman spectroscopy they refer to the symmetry of the vibration being exited. One quantum of vibration has a fixed energy, hence the asignment of a symmetry label to a wavelength.
 
Ok Sir i agree with you...But For my System Aluminium Nitride There Are Number of mode in which A1,E1,E2 are raman active and E1 at 624 cm-1 and A1 546 cm-1, Why E1 cannot written at the place of 546 and A1 at 624?
 
I think the representation can be worked out experimentally from the polarisation and intensity of the incident and scattered light.
For details you should have a look at some book on IR and Raman spectroscopy.
 

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