Separability of Hilbert Spaces

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SUMMARY

The separability of Hilbert spaces is crucial in Quantum Mechanics due to the necessity of finite-dimensional observations, even when dealing with large but unknown dimensions. Rigged Hilbert spaces, which are separable, provide a mathematical framework to manage these observations. The Stone-von Neumann theorem further emphasizes that irreducible unitary realizations of canonical commutation relations can only occur in separable spaces, specifically in the context of the standard realization in the separable space L²(R³). This foundational concept is essential for understanding both non-relativistic and relativistic quantum mechanics.

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  • Understanding of Hilbert spaces and their properties
  • Familiarity with Rigged Hilbert spaces
  • Knowledge of the Stone-von Neumann theorem
  • Basic concepts of quantum mechanics and unitary operators
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Quantum physicists, mathematicians specializing in functional analysis, and students studying advanced quantum mechanics concepts will benefit from this discussion.

Andre' Quanta
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Why we require the separability of Hilbert spaces in Quantum Mechanics?
 
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Andre' Quanta said:
Why we require the separability of Hilbert spaces in Quantum Mechanics?

In reality any actual observation is from a finite dimensional space - but sometimes of a large but unknown dimension. To handle that a limit is taken and you end up with Rigged Hilbert spaces which are separable.

To be specific the space is of vectors of finite dimension but of any size. Mathematically we take the dual which is the Rigged Hilbert space of this space. It is separable - but convergent only under a very weak topology. Such a large space isn't actually required in practice and part of the art of using Rigged Hilbert spaces is figuring out exactly what subset is needed:
http://arxiv.org/abs/quant-ph/0502053Thanks
Bill
 
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Because of results like the Stone-von Neumann theorem. In non-relativistic QM, this theorem asserts that any irreducible unitary realization of the (integrated form of the) canonical commutation relations on a complex Hilbert space ##H## (in principle, not necessarily separable) is unitarily equivalent to the standard realization in the separable space ##L^{2}(R^{3})##, i.e., only in a separable space you can get one such irreducible unitary realizations. Similar results hold for the representation theory of the Poincaré group in relativistic QM.
 
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Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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