3 ms·
Quoting from the link (emphasis mine): > symmetrized __tensor product__ of n single-particle Hilbert spaces H And clarifying your statement by copying from t
by krastanov 6y ago
Quoting from the link (emphasis mine):
> symmetrized __tensor product__ of n single-particle Hilbert spaces H
And clarifying your statement by copying from the wiki page (emphasis mine):
> direct sum of the symmetric or antisymmetric tensors in the __tensor powers__ of a single-particle Hilbert space
(which is very different from the direct sum you suggest in your comment)
I work with all of this in my day job and the research work I produce (which does deal a lot with quantum description of multiples modes of light) is usually perceived as correct by my academic colleagues. I am honestly trying to see how to interpret what you are saying differently, in a way that does not clash with the established knowledge on the topic, but I can not, even though I have non-negligible experience in the field. At best, I assume we are talking past each other while describing the same thing, but I am certainly uncomfortable with your use of "subspace" and "direct sum".
Going to the very first comment of yours that started this: My claim is that a mode (something that has a creation operator) can very well contain one, or two photons, or a coherent state, or anything else from its Hilbert space. There is no correspondence between plane waves and Fock states. We can use Fock states with other modes instead of plane waves, and we can have plane waves with a quantum state that is a coherent state for instance.
- pdonis 6y ago> which is very different from the direct sum you suggest in your comment I don't see how. I suspect that we are interpreting ordinary language words differently and talking past each other. > a mode (something that has a creation operator) And a corresponding annihilation operator. Yes, that's basically the definition I've been using. > from its Hilbert space But, as I said before, all of these states you describe are obtained by applying the creation operator for the mode to the vacuum state some number of times (and then, in some cases, forming linear combinations of states so obtained). But this process for all modes starts with the same vacuum state. There are not different vacuum states for different modes. So ultimately, all of these states belong to the same Hilbert space, since they're all obtained starting from the same vacuum state; and this Hilbert space will also contain states that have more than one "mode" in them--states obtained by applying creation operators for different modes to the vacuum state, or linear combinations of states so obtained.