Continuous inverses of shifts of partial linear maps #
For a partial linear map A on a module over a ring, LinearPMap.IsResolventAt
says that a continuous linear map inverts lambda • I - A on the domain of A. The inverse
is unique, and its existence defines LinearPMap.resolventSet and the chosen map
LinearPMap.resolvent. Its complement is LinearPMap.spectrum. These notions require only a
topology on the module, with no norm or continuity assumptions on addition or scalar multiplication.
Over a noncommutative ring, the scalar expression x ↦ lambda • x - A x need not be linear.
The predicate still requires its inverse to be linear over the full scalar ring; a parameter
whose shift is not linear therefore does not belong to the resolvent set.
This file gives the graph characterization, the two inverse identities, the fact that a point of
the resolvent set is not an eigenvalue, and the fact that an operator has no proper extension
sharing a resolvent point. The pointwise resolvent identity
holds over rings. Over division rings resolvents commute, and the resolvent at lambda acts on
an eigenvector for the eigenvalue c as multiplication by (lambda - c)⁻¹. For topological
additive groups, an invertible continuous linear perturbation gives another resolvent. Over
commutative rings with continuous scalar multiplication by constants, the resolvent of an
everywhere defined continuous linear operator agrees with Mathlib's algebraic resolvent, and their
spectra agree.
On normed spaces over nontrivially normed fields the continuous linear inverse is bounded;
Neumann perturbations and openness of the resolvent set are developed in
TauCeti.Analysis.Normed.Operator.Resolvent.Unbounded.
References #
Engel--Nagel, One-Parameter Semigroups for Linear Evolution Equations, Section IV.1; Pazy, Semigroups of Linear Operators and Applications to Partial Differential Equations, Chapter 1.
Inverting lambda • I - A #
IsResolventAt A lambda R says that the continuous operator R : X →L[𝕜] X inverts
lambda • I - A : D(A) → X: it takes its values in D(A), is a right inverse of
lambda • I - A on all of X, and is a left inverse of it on D(A).
For an unbounded A this replaces the algebraic condition
IsUnit (algebraMap 𝕜 (X →L[𝕜] X) lambda - A) behind Mathlib's resolventSet, which cannot be
formed because A is not an element of X →L[𝕜] X. The two conditions agree when A is a
continuous linear operator read as an everywhere defined LinearPMap; see
ContinuousLinearMap.mem_resolventSet_toPMap_top_iff.
The inverse takes its values in the domain of
A.Ris a right inverse:(lambda • I - A) (R y) = yfor everyy : X.Ris a left inverse:R ((lambda • I - A) x) = xfor everyx ∈ D(A).
Instances For
An inverse of lambda • I - A is unique: a left inverse and a right inverse of the same
map agree.
lambda • I - A is injective on D(A) whenever it has a left inverse.
lambda • I - A maps D(A) onto X whenever it has a right inverse.
lambda • I - A : D(A) → X is a bijection at a point of the resolvent set.
The graph form of IsResolventAt: R inverts lambda • I - A exactly when every
(R y, lambda • R y - y) lies on the graph of A, and R (lambda • x - w) = x for every point
(x, w) of that graph. This form transfers along any construction described by its graph.
The resolvent set and the resolvent #
The resolvent set of an unbounded operator A : X →ₗ.[𝕜] X: those lambda : 𝕜 for which
lambda • I - A : D(A) → X is a bijection with continuous linear inverse.
Instances For
Membership in the resolvent set unfolds to the existence of a continuous linear inverse of
lambda • I - A.
The spectrum of a partial linear map consists of the scalars whose shifts do not admit continuous linear two-sided inverses.
Instances For
Membership in the partial-operator spectrum is failure of resolvent membership.
Exhibiting an inverse puts lambda in the resolvent set.
The resolvent R(lambda, A) = (lambda • I - A)⁻¹ of an unbounded operator, as a
continuous linear operator on X.
Off the resolvent set the value is an unspecified junk value; every lemma below carries the
hypothesis lambda ∈ resolventSet A. Uniqueness of the inverse
(LinearPMap.IsResolventAt.unique) makes the choice immaterial on the
resolvent set: LinearPMap.resolvent_eq_of_isResolventAt identifies it with
any inverse one can exhibit.
Instances For
On the resolvent set, resolvent A lambda really does invert lambda • I - A.
Any exhibited inverse of lambda • I - A is the resolvent.
The resolvent takes its values in D(A).
The right-inverse identity (lambda • I - A) R(lambda) y = y.
The left-inverse identity R(lambda) (lambda • x - A x) = x on D(A).
The right-inverse identity solved for A: A R(lambda) y = lambda • R(lambda) y - y.
At a point of the resolvent set, lambda • I - A : D(A) → X is a bijection.
A point of the resolvent set is not an eigenvalue: A x = lambda • x forces x = 0.
An operator has no proper extension sharing a resolvent point. If A ≤ B and some
lambda lies in the resolvent set of both, then A = B.
A vector y ∈ D(B) has lambda • y - B y = lambda • x - A x for a unique x ∈ D(A), by
surjectivity for A; injectivity for B then forces y = x, so D(B) ⊆ D(A).
This is the step that upgrades "A is a restriction of the generator" to "A is the
generator" in the generation theorems.
The resolvent commutes with A on D(A): R(lambda) (A x) = A (R(lambda) x).
The resolvent identity #
Pointwise form of the resolvent identity
R(lambda) - R(mu) = (mu - lambda) R(lambda) R(mu).
The resolvent identity R(lambda) - R(mu) = (mu - lambda) R(lambda) R(mu), as an
equality of continuous linear maps.
Resolvents at two points of the resolvent set commute.
The resolvent acts on an eigenvector of A for the eigenvalue c as multiplication by
(lambda - c)⁻¹. For c = lambda both sides vanish: a point of the resolvent set is not an
eigenvalue, so the eigenvector is zero.
Invertible perturbations #
The common invertible perturbation witness. If lambda lies in the resolvent set of A
and I - B R(lambda, A) is invertible, then
R(lambda, A) (I - B R(lambda, A))⁻¹ inverts lambda • I - (B + A).
This is the lower-level construction shared by bounded perturbations and perturbations of the spectral parameter.
The bridge to Mathlib's algebraic resolvent #
A continuous linear operator T : X →L[𝕜] X becomes an everywhere defined partial linear map
(T : X →ₗ[𝕜] X).toPMap ⊤. Its resolvent set and resolvent agree with Mathlib's
resolventSet 𝕜 T and resolvent T, computed in the algebra X →L[𝕜] X.
An inverse of lambda • I - T in the partial-map sense is a two-sided inverse in the algebra
X →L[𝕜] X, so lambda • I - T is a unit there.
A unit lambda • I - T of the algebra X →L[𝕜] X inverts lambda • I - T in the
partial-map sense, with the algebra inverse as the resolvent.
The continuous-operator bridge, membership half. For a continuous linear operator T,
the partial-map resolvent set and Mathlib's algebraic resolvent set agree.
For a continuous linear operator on the full domain, the partial-operator spectrum agrees
with Mathlib's algebraic spectrum in X →L[𝕜] X.
The continuous-operator bridge, value half. For a continuous linear operator, the partial-map resolvent is Mathlib's algebraic resolvent.