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In [[mathematics]], '''affiliated operators''' were introduced by [[Francis Joseph Murray (mathematician)|Murray]] and [[John von Neumann|von Neumann]] in the theory of [[von Neumann algebras]] as a technique for using [[unbounded operator]]s to study modules generated by a single vector. Later [[Michael Francis Atiyah|Atiyah]] and [[Isadore Singer|Singer]] showed that [[Atiyah-Singer index theorem|index theorems]] for [[elliptic operator]]s on [[closed manifold]]s with infinite [[fundamental group]] could naturally be phrased in terms of unbounded operators affiliated with the von Neumann algebra of the group. Algebraic properties of affiliated operators have proved important in [[L2 cohomology|L<sup>2</sup> cohomology]], an area between [[analysis]] and [[geometry]] that evolved from the study of such index theorems.
 
==Definition==
Let ''M'' be a [[von Neumann algebra]] acting on a [[Hilbert space]] ''H''. A [[closed linear operator|closed]] and densely defined operator ''A'' is said to be '''affiliated''' with ''M'' if ''A'' commutes with every [[unitary operator]] ''U'' in the [[commutant]] of ''M''. Equivalent conditions
are that:
 
*each unitary ''U'' in ''M''' should leave invariant the graph of ''A'' defined by <math> G(A)=\{(x,Ax):x\in D(A)\} \subseteq H\oplus H</math>.
 
*the projection onto ''G''(''A'') should lie in ''M''<sub>2</sub>(''M'').
 
*each unitary ''U'' in ''M''' should carry ''D''(''A''), the [[Domain of a function|domain]] of ''A'', onto itself and  satisfy ''UAU* = A'' there.
 
*each unitary ''U'' in ''M''' should commute with both operators in the [[polar decomposition]] of ''A''.
 
The last condition follows by uniqueness of the polar decomposition. If ''A'' has a polar decomposition
:<math>A=V|A|, \, </math>
it says that the [[partial isometry]] ''V'' should lie in ''M'' and that the positive [[self-adjoint]] operator ''|A|'' should be affiliated with ''M''. However, by the [[spectral theorem]], a positive self-adjoint operator commutes with a unitary operator if and only if each of its spectral projections <math> E([0,N]) </math>
does. This gives another equivalent condition:
 
*each spectral projection of |''A''| and the partial isometry in the polar decomposition of ''A'' should lie in ''M''.
 
== Measurable operators ==
 
In general the operators affiliated with a von Neumann algebra ''M'' need not necessarily be well-behaved under either addition or composition. However in the presence of a faithful semi-finite normal trace &tau; and the standard [[Gelfand&ndash;Naimark&ndash;Segal]] action of ''M'' on ''H''&nbsp;=&nbsp;''L''<sup>2</sup>(''M'',&nbsp;&tau;), [[Edward Nelson]] proved that the '''measurable''' affiliated operators do form a [[*-algebra]] with nice properties: these are operators such that &tau;(''I''&nbsp;&minus;&nbsp;''E''([0,''N'']))&nbsp;<&nbsp;&infin;
for ''N'' sufficiently large. This algebra of unbounded operators is complete for a natural topology, generalising the notion of [[convergence in measure]].
It contains all the non-commutative ''L''<sup>''p''</sup> spaces defined by the trace and was introduced to facilitate their study.
 
This theory can be applied when the von Neumann algebra ''M'' is '''type I''' or '''type II'''. When ''M''&nbsp;=&nbsp;''B''(''H'') acting on the Hilbert space ''L''<sup>2</sup>(''H'') of [[Hilbert–Schmidt operator]]s, it gives the well-known theory of non-commutative ''L''<sup>''p''</sup> spaces ''L''<sup>''p''</sup> (''H'') due to Schatten and [[von Neumann]].
 
When ''M'' is in addition a '''finite''' von Neumann algebra, for example a type II<sub>1</sub> factor, then every affiliated operator is automatically measurable, so the affiliated operators form a [[*-algebra]], as originally observed in the first paper of [[Francis Joseph Murray (mathematician)|Murray]] and von Neumann. In this case ''M'' is a [[von Neumann regular ring]]: for on the closure of its image ''|A|'' has a measurable inverse ''B'' and then ''T''&nbsp;=&nbsp;''BV''<sup>*</sup> defines a measurable operator with ''ATA''&nbsp;=&nbsp;''A''. Of course in the classical case when ''X'' is a probability space and ''M''&nbsp;=&nbsp;''L''<sup>&infin;</sup> (''X''), we simply recover the *-algebra of measurable functions on ''X''.
 
If however ''M'' is '''type III''', the theory takes a quite different form. Indeed in this case, thanks to the [[Tomita–Takesaki theory]], it is known that the non-commutative ''L''<sup>''p''</sup> spaces are no longer realised by operators affiliated with the von Neumann algebra. As [[Alain Connes|Connes]] showed, these spaces can be realised as unbounded operators only by using a certain positive power of the reference modular operator. Instead of being characterised by the simple affiliation relation ''UAU''<sup>*</sup>&nbsp;=&nbsp;''A'', there is a more complicated bimodule relation involving the analytic continuation of the modular automorphism group.
 
== References ==
* A. Connes, ''Non-commutative geometry'', ISBN 0-12-185860-X
* J. Dixmier, ''Von Neumann algebras'', ISBN 0-444-86308-7 [Les algèbres d'opérateurs dans l'espace hilbertien: algèbres de von Neumann, Gauthier-Villars (1957 & 1969)]
* W. Lück, ''L<sup>2</sup>-Invariants: Theory and Applications to Geometry and K-Theory'', (Chapter 8: the algebra of affiliated operators) ISBN 3-540-43566-2
* F. J. Murray and J. von Neumann, ''Rings of Operators'', Annals of Math. '''37''' (1936), 116&ndash;229 (Chapter XVI).
* E. Nelson, ''Notes on non-commutative integration'', J. Funct. Anal. '''15''' (1974), 103&ndash;116.
* M. Takesaki, ''Theory of Operator Algebras I, II, III'', ISBN 3-540-42248-X ISBN 3-540-42914-X ISBN 3-540-42913-1
 
[[Category:Operator theory]]
[[Category:Von Neumann algebras]]

Revision as of 16:06, 15 March 2013

In mathematics, affiliated operators were introduced by Murray and von Neumann in the theory of von Neumann algebras as a technique for using unbounded operators to study modules generated by a single vector. Later Atiyah and Singer showed that index theorems for elliptic operators on closed manifolds with infinite fundamental group could naturally be phrased in terms of unbounded operators affiliated with the von Neumann algebra of the group. Algebraic properties of affiliated operators have proved important in L2 cohomology, an area between analysis and geometry that evolved from the study of such index theorems.

Definition

Let M be a von Neumann algebra acting on a Hilbert space H. A closed and densely defined operator A is said to be affiliated with M if A commutes with every unitary operator U in the commutant of M. Equivalent conditions are that:

  • the projection onto G(A) should lie in M2(M).
  • each unitary U in M' should carry D(A), the domain of A, onto itself and satisfy UAU* = A there.

The last condition follows by uniqueness of the polar decomposition. If A has a polar decomposition

it says that the partial isometry V should lie in M and that the positive self-adjoint operator |A| should be affiliated with M. However, by the spectral theorem, a positive self-adjoint operator commutes with a unitary operator if and only if each of its spectral projections does. This gives another equivalent condition:

  • each spectral projection of |A| and the partial isometry in the polar decomposition of A should lie in M.

Measurable operators

In general the operators affiliated with a von Neumann algebra M need not necessarily be well-behaved under either addition or composition. However in the presence of a faithful semi-finite normal trace τ and the standard Gelfand–Naimark–Segal action of M on H = L2(M, τ), Edward Nelson proved that the measurable affiliated operators do form a *-algebra with nice properties: these are operators such that τ(I − E([0,N])) < ∞ for N sufficiently large. This algebra of unbounded operators is complete for a natural topology, generalising the notion of convergence in measure. It contains all the non-commutative Lp spaces defined by the trace and was introduced to facilitate their study.

This theory can be applied when the von Neumann algebra M is type I or type II. When M = B(H) acting on the Hilbert space L2(H) of Hilbert–Schmidt operators, it gives the well-known theory of non-commutative Lp spaces Lp (H) due to Schatten and von Neumann.

When M is in addition a finite von Neumann algebra, for example a type II1 factor, then every affiliated operator is automatically measurable, so the affiliated operators form a *-algebra, as originally observed in the first paper of Murray and von Neumann. In this case M is a von Neumann regular ring: for on the closure of its image |A| has a measurable inverse B and then T = BV* defines a measurable operator with ATA = A. Of course in the classical case when X is a probability space and M = L (X), we simply recover the *-algebra of measurable functions on X.

If however M is type III, the theory takes a quite different form. Indeed in this case, thanks to the Tomita–Takesaki theory, it is known that the non-commutative Lp spaces are no longer realised by operators affiliated with the von Neumann algebra. As Connes showed, these spaces can be realised as unbounded operators only by using a certain positive power of the reference modular operator. Instead of being characterised by the simple affiliation relation UAU* = A, there is a more complicated bimodule relation involving the analytic continuation of the modular automorphism group.

References

  • A. Connes, Non-commutative geometry, ISBN 0-12-185860-X
  • J. Dixmier, Von Neumann algebras, ISBN 0-444-86308-7 [Les algèbres d'opérateurs dans l'espace hilbertien: algèbres de von Neumann, Gauthier-Villars (1957 & 1969)]
  • W. Lück, L2-Invariants: Theory and Applications to Geometry and K-Theory, (Chapter 8: the algebra of affiliated operators) ISBN 3-540-43566-2
  • F. J. Murray and J. von Neumann, Rings of Operators, Annals of Math. 37 (1936), 116–229 (Chapter XVI).
  • E. Nelson, Notes on non-commutative integration, J. Funct. Anal. 15 (1974), 103–116.
  • M. Takesaki, Theory of Operator Algebras I, II, III, ISBN 3-540-42248-X ISBN 3-540-42914-X ISBN 3-540-42913-1