Does an irreducible representation acting on operators imply....

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Discussion Overview

The discussion revolves around the relationship between irreducible representations acting on operators and the implications for states transforming under those representations, particularly in the context of quantum field theory (QFT). Participants explore whether the irreducibility of one representation necessarily implies the irreducibility of the other, with examples drawn from symmetry transformations and Lagrangians.

Discussion Character

  • Debate/contested
  • Technical explanation

Main Points Raised

  • One participant questions whether an irreducible representation acting on operators implies that the corresponding representation acting on states is also irreducible.
  • Another participant asserts that the irreducibility of the operator representation does not imply the irreducibility of the state representation, providing examples from relativistic QFT where the state representation is infinite-dimensional and not irreducible.
  • A subsequent reply clarifies that the implication does not hold in the opposite direction either, indicating that irreducibility of the state representation does not guarantee irreducibility of the operator representation.
  • Further discussion highlights the distinction between finite-dimensional and infinite-dimensional representations, noting that compact groups have finite-dimensional irreducible representations but lack infinite-dimensional irreducible representations.
  • Participants emphasize that the relevant Hilbert spaces in QFT are typically infinite-dimensional, which complicates the relationship between the representations.

Areas of Agreement / Disagreement

Participants generally disagree on the implications of irreducibility between the representations of operators and states. There is no consensus on whether one implies the other, and the discussion remains unresolved regarding the broader implications in different contexts.

Contextual Notes

Participants note limitations related to the dimensionality of representations and the nature of the groups involved, particularly the distinction between compact and non-compact groups. The discussion also highlights the complexity of representations in quantum field theory, where the relevant representations may not be irreducible.

hideelo
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Ok, so my question is "Does an irreducible representation acting on operators imply that the states also transform in an irreducible representation?" and what I mean by that is the following. If I have an operator transforming in an irreducible transformation of some group, I get a corresponding symmetry transformation on my states, is this representation acting on my states also irreducible?For example, suppose I had a lagrangian that was ##L = \phi^\mu \phi_\mu## then I can see that that it has SO(n) symmetry in the following sense. Let ##R(\omega)## be a rotation (in the fundamental representation) then if I send ##\phi_\mu \mapsto R(\omega)_\mu^\nu \phi_\nu## the lagrangian remains invariant. Corresponding to this I get a representation acting on the states by ##R(\omega)_\mu^\nu \phi_\nu = U(\omega)^{-1} \phi_\mu U(\omega)##

Now I know that the ##R(\omega)_\mu^\nu## is in the fundamental so that is necessarily an irreducible representation. However can I somehow conclude that the ##U(\omega)## representation is irreducible as well?

P.S. I know that in general states and operators don't even need to have the same symmetry group. I'm more interested in whether irreducibility of one implies irreducibility of the other
 
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hideelo said:
can I somehow conclude that the ##U(\omega)## representation is irreducible as well?
No. Irreducibility of R does not imply that of U. In fact, in relativistic QFT: \begin{align*}U : & \ T(4) \rtimes SL(2, \mathbb{C}) \to U( \mathcal{H}) \\ & \ \ \ \ \ \ ( a , A ) \mapsto U( a , A) , \end{align*} the representation U(a,A) is faithful, unitary and infinite-dimensional but not irreducible. While the representation D : SL(2, \mathbb{C}) \to GL( V^{(j_{1} , j_{2})}) is non-unitary, finite-dimensional and irreducible.
 
samalkhaiat said:
No. Irreducibility of R does not imply that of U. In fact, in relativistic QFT: \begin{align*}U : & \ T(4) \rtimes SL(2, \mathbb{C}) \to U( \mathcal{H}) \\ & \ \ \ \ \ \ ( a , A ) \mapsto U( a , A) , \end{align*} the representation U(a,A) is faithful, unitary and infinite-dimensional but not irreducible. While the representation D : SL(2, \mathbb{C}) \to GL( V^{(j_{1} , j_{2})}) is non-unitary, finite-dimensional and irreducible.

I think you're saying that the implication does not go the other way. i.e. in my example irreducibility of the U(\omega) representation would not imply irreducibility of the R(\omega) representation. Am I understanding you correctly?
 
hideelo said:
Am I understanding you correctly?
No.
Is U( \omega ) in your example finite-dimensional or (the important) infinite-dimensional unitary representation? The relevant “Hilbert” spaces in QFT’s are infinite-dimensional.
For some reason you considered SO(n) which is a compact group. A compact group has, among others, also finite-dimensional, irreducible, unitary representations; however, it does not have infinite-dimensional, irreducible unitary representation.
In the transformation law (of a relativistic field theory) U^{\dagger}(g) \varphi_{a} U(g) = D_{a}{}^{b}(g) \varphi_{b} , \ \ a = 1,2, \cdots , n
D : G \to GL (V^{n}) is a finite-dimensional irreducible representation of the “symmetry” group G (since we always take our fields to be irreducible) and U : G \to U( \mathcal{H}) is the corresponding (mostly infinite-dimensional) unitary representation of G in the Hilbert space \mathcal{H}.
So, the irreducibility of D does not imply that U is also irreducible(in QFT, the relevant U's are not irreducible). Also, the field space V^{n} is a finite-dimensional vector space, this does not mean that the Hilbert space \mathcal{H} is also finite-dimensional.
 

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