Undergrad What conditions are needed to raise a linear operator to some power?

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SUMMARY

For a power of a linear operator to exist, the operator's domain must remain invariant under the operation. Specifically, the range of the operator must be included in the domain to facilitate consecutive applications. An example is provided with the differentiation operator on the space of continuously differentiable functions, where the second power of the operator is well-defined despite the range not being contained in the original domain. This concept is crucial for discussing generalized eigenspaces of unbounded operators, particularly in relation to the Borel Functional Calculus.

PREREQUISITES
  • Understanding of linear operators and their domains
  • Familiarity with vector spaces and subspaces
  • Knowledge of the Borel Functional Calculus
  • Basic concepts of eigenvalues and eigenspaces
NEXT STEPS
  • Research the properties of linear operators and their domains
  • Study the Borel Functional Calculus in detail
  • Explore the concept of generalized eigenspaces for unbounded operators
  • Examine examples of differentiation operators in functional analysis
USEFUL FOR

Mathematicians, particularly those specializing in functional analysis, linear algebra, and operator theory, will benefit from this discussion.

fxdung
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Each operator has a domain, so for a power of an operator to exist, the domain of the operator must remain invariant under the operation.

Is that correct?

mentor note: edited for future clarity
 
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fxdung said:
Each operator has a domain, so for a power of an operator to exist, the domain of the operator must remain invariant under the operation.

Is that correct?

mentor note: edited for future clarity
The range must be included in the domain, simply to allow a consecutive application.
 
fresh_42 said:
The range must be included in the domain, simply to allow a consecutive application.
This is the wrong approach if ##D(A)## is a proper subspace of a vector space ##X##.

For example, take ##X = C[0,1]## and ##D(A) = C^1[0,1]## and ##A : D(A) \to X## differentiation. Then the range of ##A## is not contained in its domain, but ##A^2## is well-defined with
$$
D(A^2) = C^2[0,1] = \{f \in D(A)\,:\,Af \in D(A)\}.
$$
(This also suggests the general definition.) This is important if one wants to talk about the generalized eigenspace of an unbounded operator, which is defined in terms of positive integer powers of ##\lambda I - A##, where ##I## is the identity on ##X## and ##\lambda## is an eigenvalue.
 
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Look up the Borel Functional Calculus. It formalizes the general idea of applying general Mathematical operations to linear operators.
 
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I am studying the mathematical formalism behind non-commutative geometry approach to quantum gravity. I was reading about Hopf algebras and their Drinfeld twist with a specific example of the Moyal-Weyl twist defined as F=exp(-iλ/2θ^(μν)∂_μ⊗∂_ν) where λ is a constant parametar and θ antisymmetric constant tensor. {∂_μ} is the basis of the tangent vector space over the underlying spacetime Now, from my understanding the enveloping algebra which appears in the definition of the Hopf algebra...

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