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 g∈SU(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: R⊗R:g→R(g)⊗R(g). What is the commutant (also known as centralizer) of the representation R⊗R?
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 R⊗R:
-
Pi⊗Pj, for i,j=0,1,...,∞
-
Sjj
where Sjj is the "swap" operator in the subspace Hj⊗Hj. 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