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On Murray-von Neumann algebras—I: topological, order-theoretic and analytical aspects

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Abstract

For a countably decomposable finite von Neumann algebra \({\mathscr {R}}\), we show that any choice of a faithful normal tracial state on \({\mathscr {R}}\) engenders the same measure topology on \({\mathscr {R}}\) in the sense of Nelson (J Funct Anal 15:103–116, 1974). Consequently it is justified to speak of ‘the’ measure topology of \({\mathscr {R}}\). Having made this observation, we extend the notion of measure topology to general finite von Neumann algebras and denominate it the \({\mathfrak {m}}\)-topology. We note that the procedure of \({\mathfrak {m}}\)-completion yields Murray-von Neumann algebras in a functorial manner and provides them with an intrinsic description as unital ordered complex topological \(*\)-algebras. This enables the study of abstract Murray-von Neumann algebras avoiding reference to a Hilbert space. Furthermore, it makes apparent the appropriate notion of Murray-von Neumann subalgebras, and the intrinsic nature of the spectrum and point spectrum of elements, independent of their ambient Murray-von Neumann algebra. In this context, we show the well-definedness of the Borel function calculus for normal elements and use it along with approximation techniques in the \({\mathfrak {m}}\)-topology to transfer many standard operator inequalities involving bounded self-adjoint operators to the setting of (unbounded) self-adjoint operators in Murray-von Neumann algebras. On the algebraic side, Murray-von Neumann algebras have been described as the Ore localization of finite von Neumann algebras with respect to their corresponding multiplicative subset of non-zero-divisors. Our discussion reveals that, in addition, there are fundamental topological, order-theoretic and analytical facets to their description.

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Notes

  1. Although the theory is developed in the more general setting of semifinite von Neumann algebras with a faithful normal semifinite trace, we are primarily concerned with the case of finite von Neumann algebras since our interest is in Murray-von Neumann algebras.

  2. For example, let \(\tau _1, \tau _2\) be normal states on \(L^{\infty }({\mathbb {R}}; \mu )\) (\(\mu\) being the Lebesgue measure) corresponding to integration with respect to two distinct Gaussian probability measures.

  3. A linear map between topological vector spaces is Cauchy-continuous if and only if it is continuous.

  4. By an ordered complex \(*\)-algebra, we mean a complex \(*\)-algebra whose Hermitian elements form an ordered real vector space.

  5. For operators in \({\mathscr {R}} _{\text {aff}}\) (acting on the Hilbert space \({\mathscr {H}}\)), this coincides with the usual definition of spectrum and point spectrum.

  6. For \(A, B \in {\mathscr {R}} _{\text {aff}}\), \(A \, {\hat{+}} \,B := \overline{A+B}, A \, {{\hat{\cdot }}} \,B := {\overline{AB}}\).

  7. We think of \({\mathfrak {m}}\) as ‘measure’ or ‘measure-theoretic’.

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Acknowledgements

I would like to thank Dmitri Pavlov for his illuminating answers on the website MathOverflow (in particular, [3]) and sharing his study of the opposite category of commutative von Neumann algebras in [14]. I am also grateful to Zhe Liu and Raghavendra Venkatraman for helpful discussions, and to K. V. Shuddhodan for valuable feedback that helped improve the exposition of the paper.

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Correspondence to Soumyashant Nayak.

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Communicated by Maria Joita.

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Nayak, S. On Murray-von Neumann algebras—I: topological, order-theoretic and analytical aspects. Banach J. Math. Anal. 15, 45 (2021). https://doi.org/10.1007/s43037-021-00129-7

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