Separability of Hilbert Spaces

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The separability of Hilbert spaces is crucial in Quantum Mechanics as it allows for the application of the Stone-von Neumann theorem, which ensures that any irreducible unitary representation of canonical commutation relations can be realized in a separable space. While actual observations occur in finite-dimensional spaces, Rigged Hilbert spaces, which are separable, are utilized to manage potentially infinite dimensions. These spaces converge under weak topology, facilitating the identification of necessary subsets for practical applications. The discussion highlights the mathematical foundation and implications of using separable spaces in both non-relativistic and relativistic quantum theories. Understanding these concepts is essential for advancing quantum mechanics and its applications.
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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