SU(2) symmetry of the ammonia molecule?

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Discussion Overview

The discussion revolves around the SU(2) symmetry of the ammonia molecule, exploring its implications in quantum mechanics and group theory. Participants examine the relationship between the molecular states of ammonia and the mathematical structure of SU(2), as well as alternative symmetry perspectives.

Discussion Character

  • Exploratory
  • Debate/contested
  • Technical explanation

Main Points Raised

  • Some participants seek clarification on why the ammonia molecule is associated with SU(2) symmetry, questioning the connection between its symmetric states and the group of 2x2 complex unitary matrices.
  • Others describe the two states of the ammonia molecule, where nitrogen is positioned above or below the hydrogen atoms, noting their degeneracy and the role of orthogonal linear combinations in maintaining energy levels.
  • A participant challenges the notion of symmetry, asking what is being left invariant and whether it pertains to amplitudes.
  • Some express skepticism about the SU(2) classification, suggesting that the symmetry group could also be Z2, emphasizing the need for context.
  • Another participant mentions the C_{3v} symmetry of ammonia, indicating it as an approximate point group symmetry, while also noting the relevance of the inversion mode and its implications for molecular symmetry.
  • Discussion includes references to the ammonia maser and the relationship between the inversion mode and the spin states of hydrogen atoms, highlighting the complexity of the symmetry involved.

Areas of Agreement / Disagreement

Participants express differing views on the appropriate symmetry classification for the ammonia molecule, with some advocating for SU(2) and others suggesting C_{3v} or Z2. The discussion remains unresolved, with multiple competing perspectives presented.

Contextual Notes

There are limitations regarding the assumptions made about the symmetry classifications and the specific conditions under which they apply. The discussion also touches on the complexities of molecular symmetry that may not be fully addressed.

"pi"mp
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Hi,
I'm an undergraduate taking the basic quantum classes and on my own, I'm trying to wrap my mind around how symmetry and group theory applies in Q.M. and theoretical physics in general; it's coming along slowly but surely!

Can someone please explain why the ammonia molecule is said to exhibit SU(2) symmetry? I can't imagine how the two symmetric states of ammonia have anything to do with the group of 2x2 complex unitary matrices of det=1.

Thanks
 
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Where did you hear that?
 
Can someone please explain why the ammonia molecule is said to exhibit SU(2) symmetry? I can't imagine how the two symmetric states of ammonia have anything to do with the group of 2x2 complex unitary matrices of det=1.
The ammonia molecule has two states, the first one |1> in which the N is above the three H's, the other one |2> where the N is below them. Both states have the same energy E (two-fold degeneracy).

Moreover, any orthogonal linear combinations of |1> and |2> will also have the same energy E. The linear combinations can have complex coefficients, but must preserve the norm of the state. In other words, the most general state with energy E is given by U|ψ> where U is a 2x2 matrix and <ψ|UU|ψ> = 1. That is, U is unitary. But the U(2) symmetry is actually SU(2) since one of the transformations just adds a phase factor, which doesn't count!
 
Last edited:
Ah, so why is that considered a "symmetry?" I always thought a symmetry was of the form: "_____ is left invariant upon action by ____" What is being left invariant? Just the amplitudes?
 
I ask again - where did you see that?

You're asking us to explain something that we can't see. This is not going to go well. Bill has a very good answer, but I could just as easily argue that the symmetry group is Z2. We need context.
 
When I think of the symmetry of ammonia, I think C_{3v}.

Clarification would certainly help.
 
Jorriss said:
When I think of the symmetry of ammonia, I think C_{3v}.

Clarification would certainly help.

That's only the approximate point group symmetry of the ammonia molecule which would hold if it were rigid. However, as there is an inversion mode where the N can swing through the plane formed by the H atoms one has to consider the full molecular symmetry group which is a subgroup of the complete nuclear permutation and inversion group (CNPI). In the context of the OP this is not too relevant. It is all about the approximate degeneracy of the symmetric and antisymmetric eigenstates of the inversion mode. If these where really degenerate, there would be an additional SU(2) symmetry, as Bill_K already explained. It is a very old discussion why superpositions of configurations are seldomly observed, especially of enantiomeric states: look out for "Hund's paradox".
 
The ammonia molecule has two states, the first one |1> in which the N is above the three H's, the other one |2> where the N is below them. Both states have the same energy E (two-fold degeneracy).
this is probably treated in feynman lectures quantum mechanics,where he has chosen the above ones as two base states.
 
  • #10
This inversion mode of the ammonia molecule has been studied intensively as it forms the basis of the ammonia maser. One interesting point is that the inversion mode only relates two different states for certain values of the sum of the spins of the three hydrogen atoms (S=1/2). This spin state can be obtained in two different ways, either coupling atom 1 and two into a singlet or coupling 1 and 3 into a singlet (other possibilities can be expressed as a linear combination of the two). The inversion will interconvert these two states
 

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