Partial isometries in a star semigroup #
An element u of a star semigroup is a partial isometry when u * star u * u = u. For a bounded
operator on a Hilbert space this is the usual notion: star u * u is then the orthogonal
projection onto the initial space of u, and u is isometric there and zero on its orthogonal
complement. The Hilbert-space characterizations are in
TauCeti/Analysis/InnerProductSpace/PartialIsometry.lean; this file records the purely algebraic
part of the theory.
Main definitions #
TauCeti.IsPartialIsometry u: the elementusatisfiesu * star u * u = u. The predicate only needs a multiplication and a star operation; the structural results below hold in any star semigroup, so in particular in non-unital star rings such as non-unital Cā-algebras.
Main statements #
TauCeti.IsPartialIsometry.star: the adjoint of a partial isometry is a partial isometry.TauCeti.IsPartialIsometry.isStarProjection_star_mul_self: the initial projectionstar u * uof a partial isometry is a star projection;isStarProjection_mul_star_selfis the corresponding statement for the final projectionu * star u.TauCeti.IsPartialIsometry.of_star_mul_self_eq_one,TauCeti.IsPartialIsometry.of_mem_unitary,IsStarProjection.isPartialIsometry: isometries, unitaries and star projections are partial isometries.
References #
- J. B. Conway, A Course in Functional Analysis, 2nd ed., Springer (1990), the treatment of partial isometries and the polar decomposition.
The adjoint of a partial isometry is a partial isometry.
The initial projection star u * u of a partial isometry is a star projection.
The final projection u * star u of a partial isometry is a star projection.
An element is a partial isometry iff its adjoint is.
A coisometry, that is an element with u * star u = 1, is a partial isometry.
The identity is a partial isometry.
Zero is a partial isometry.
A star projection is a partial isometry.