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  Group theory and quantum optics

+ 4 like - 0 dislike
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This is a question about application of group theory to physics.

The starting point is the group SU(n). I have a representation R of SU(n) that takes values on the unitary group on an infinite dimensional separable Hilbert space H. This representation can be written as the direct sum of finite-dimensional irreducible representations. Let me write R(g)=jRj(g) for gSU(n). The space Hj of each irreducible representation is finite-dimensional. I denote as Pj the projector on Hj. For those who are familiar with the subject, what I have in mind is the representation of SU(n) obtained when applying to a set of n bosonic modes the canonical transformations that are linear and preserve the photon-number operator. In this setting, the subspaces Hj are the subspaces with j photons, with j=0,1,..,.

My question is the following:

From the representation R given above we can define another representation: RR:gR(g)R(g). What is the commutant (also known as centralizer) of the representation RR?

It is easy to see that the commutant of the representation R is given by the projectors Pj's. It is also easy to check that the following operators belong to the commutant of RR:

  • PiPj, for i,j=0,1,...,

  • Sjj

where Sjj is the "swap" operator in the subspace HjHj. I wonder if there are other operators in the commutant. How can I check it?

Thanks a lot and please accept my apologies if my notation is not very clear.


This post imported from StackExchange Physics at 2015-11-02 22:08 (UTC), posted by SE-user Cosmo Lupo

asked Jan 26, 2015 in Theoretical Physics by Cosmo Lupo (20 points) [ revision history ]
edited Nov 2, 2015 by Dilaton
Worth noting that apparently "commutant" is another word for "centralizer," for those who were confused like me. Maybe this is a regional thing?

This post imported from StackExchange Physics at 2015-11-02 22:08 (UTC), posted by SE-user Chris White

commutant is used in functional analysis, centralizer in group theory.

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