Projection onto the kernel of a matrix

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SUMMARY

The discussion centers on the properties of projection operators onto the kernel of a matrix M, particularly in finite and infinite-dimensional vector spaces. It establishes that a unique projection operator P exists such that ker P equals Img M and Img P equals ker M, even in the absence of an inner product. The conversation also highlights that while the projection operator is not necessarily orthogonal, it is linear, self-adjoint, and idempotent. The participants seek clarity on the uniqueness of this operator in infinite dimensions and its standard nomenclature in mathematical literature.

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  • Understanding of linear operators and vector spaces
  • Familiarity with concepts of kernel and image of a matrix
  • Knowledge of finite and infinite-dimensional spaces
  • Basic principles of linear algebra, including self-adjoint and idempotent operators
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  • Research the properties of linear operators in infinite-dimensional spaces
  • Study the concept of projection operators in functional analysis
  • Explore the uniqueness of projection operators in various mathematical contexts
  • Investigate standard terminology used for projection operators in advanced mathematics
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Mathematicians, linear algebra students, and researchers in functional analysis who are exploring projection operators and their properties in both finite and infinite-dimensional vector spaces.

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If we have a matrix M with a kernel, in many cases there exists a projection operator P onto the kernel of M satisfying [P,M]=0. It seems to me that this projector does not in general need to be an orthogonal projector, but it is probably unique if it exists. My question: is there a standard name for such a projector among math people?
 
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What do you mean by "projection operator" (or "projector") if not an orthogonal projector?

If V is a finite-dimensional vector space and U is a subspace of V, every x in V can be uniquely expressed as x=y+z, with y in U, and z in the orthogonal complement of U. The map x\mapsto y is the projection operator associated with the subspace U. It's linear, self-adjoint and idempotent (P2=P).

Let P be any linear, self-adjoint and idempotent operator. Its range W is a subspace. So every x in V can be uniquely expressed as x=y+z, with y in W and z in the orthogonal complement. Since the decomposition is unique, and x=Px+(1-P)x, we have y=Px and z=(1-P)x. So P is the projection operator associated with W.

This means that the two standard ways to define a projection operator are equivalent. So if you're using either of these definitions, there's only one projection operator associated with ker M. Are you using some other definition?
 
Dear Fredrik,
Thank you for the reply. I think I was not sufficiently clear about the concept I am considering.

I want to consider a linear operator M on a vector space V whose image is linearly independent from its Kernel.

On a finite dimensional vector space, this implies that V = ker M + Img M.
In this case, there is a unique projector P such that ker P = Img M and Img P = ker M. It can be considered the natural projector onto the kernel of M. It is not necessarily an orthogonal projector---note that I have not specified any notion of inner product on V.

If the vector space is infinite dimensional, in general we do not have
V = ker M +Img M. But suppose that ker M is a closed subspace of V, so there is a projection P onto the kernel of M: ker M = Img P. If we in addition require P M =0, this is a natural infinite dimensional analogue of the projection operator defined in the last paragraph.

My question is twofold:
1) Is the projection operator defined above unique in the infinite dimensional case?
2) Is there a standard way to refer to this projection operator among mathematically knowledgeable?

Thank you!
 
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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