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TauCeti.Algebra.Star.PartialIsometry

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 #

Main statements #

References #

def TauCeti.IsPartialIsometry {R : Type u_1} [Mul R] [Star R] (u : R) :

An element u of a type with a multiplication and a star operation is a partial isometry when u * star u * u = u.

Instances For
    theorem TauCeti.isPartialIsometry_iff {R : Type u_1} [Mul R] [Star R] {u : R} :

    Unfold the definition of a partial isometry.

    theorem TauCeti.IsPartialIsometry.mul_star_mul_self {R : Type u_1} [Mul R] [Star R] {u : R} (hu : IsPartialIsometry u) :
    u * star u * u = u

    The defining equation u * star u * u = u of a partial isometry.

    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.

    @[simp]

    An element is a partial isometry iff its adjoint is.

    An isometry, that is an element with star u * u = 1, is a partial isometry.

    A coisometry, that is an element with u * star u = 1, is a partial isometry.

    A unitary element is a partial isometry.

    The identity is a partial isometry.

    Zero is a partial isometry.

    A star projection is a partial isometry.