Skip to Main Content

Proceedings of the American Mathematical Society

Published by the American Mathematical Society since 1950, Proceedings of the American Mathematical Society is devoted to shorter research articles in all areas of pure and applied mathematics.

ISSN 1088-6826 (online) ISSN 0002-9939 (print)

The 2020 MCQ for Proceedings of the American Mathematical Society is 0.85.

What is MCQ? The Mathematical Citation Quotient (MCQ) measures journal impact by looking at citations over a five-year period. Subscribers to MathSciNet may click through for more detailed information.

 

Geodesics of projections in von Neumann algebras
HTML articles powered by AMS MathViewer

by Esteban Andruchow PDF
Proc. Amer. Math. Soc. 149 (2021), 4501-4513 Request permission

Abstract:

Let ${\mathcal {A}}$ be a von Neumann algebra and ${\mathcal {P}}_{\mathcal {A}}$ the manifold of projections in ${\mathcal {A}}$. There is a natural linear connection in ${\mathcal {P}}_{\mathcal {A}}$, which in the finite dimensional case coincides with the the Levi-Civita connection of the Grassmann manifold of $\mathbb {C}^n$. In this paper we show that two projections $p,q$ can be joined by a geodesic, which has minimal length (with respect to the metric given by the usual norm of ${\mathcal {A}}$), if and only if \begin{equation*} p\wedge q^\perp \sim p^\perp \wedge q, \end{equation*} where $\sim$ stands for the Murray-von Neumann equivalence of projections. It is shown that the minimal geodesic is unique if and only if $p\wedge q^\perp = p^\perp \wedge q=0$. If ${\mathcal {A}}$ is a finite factor, any pair of projections in the same connected component of ${\mathcal {P}}_{\mathcal {A}}$ (i.e., with the same trace) can be joined by a minimal geodesic.

We explore certain relations with Jones’ index theory for subfactors. For instance, it is shown that if ${\mathcal {N}}\subset {\mathcal {M}}$ are II$_1$ factors with finite index $[{\mathcal {M}}:{\mathcal {N}}]={\mathbf {t}}^{-1}$, then the geodesic distance $d(e_{\mathcal {N}},e_{\mathcal {M}})$ between the induced projections $e_{\mathcal {N}}$ and $e_{\mathcal {M}}$ is $d(e_{\mathcal {N}},e_{\mathcal {M}})=\arccos ({\mathbf {t}}^{1/2})$.

References
Similar Articles
  • Retrieve articles in Proceedings of the American Mathematical Society with MSC (2020): 58B20, 46L10, 53C22
  • Retrieve articles in all journals with MSC (2020): 58B20, 46L10, 53C22
Additional Information
  • Esteban Andruchow
  • Affiliation: Instituto Argentino de Matemática, ‘Alberto P. Calderón’, CONICET, Saavedra 15 3er. piso (1083) Buenos Aires, Argentina; and Universidad Nacional de General Sarmiento, J.M. Gutierrez 1150 (1613), Los Polvorines, Argentina
  • MR Author ID: 26110
  • Email: eandruch@campus.ungs.edu.ar
  • Received by editor(s): November 21, 2020
  • Received by editor(s) in revised form: March 9, 2021
  • Published electronically: July 28, 2021
  • Communicated by: Adrian Ioana
  • © Copyright 2021 American Mathematical Society
  • Journal: Proc. Amer. Math. Soc. 149 (2021), 4501-4513
  • MSC (2020): Primary 58B20, 46L10, 53C22
  • DOI: https://doi.org/10.1090/proc/15568
  • MathSciNet review: 4305999