Normal, self-adjoint and positive definite operators

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SUMMARY

This discussion focuses on the properties of self-adjoint and positive definite operators in finite dimensional inner product spaces. It establishes that if U is a self-adjoint operator and T is a positive definite operator, then both UT and TU are diagonalizable with real eigenvalues. Additionally, it confirms that for normal operators T and U that commute, the relationship UT* = T*U holds, and there exists an orthonormal basis consisting of eigenvectors for both operators.

PREREQUISITES
  • Understanding of finite dimensional inner product spaces
  • Knowledge of self-adjoint operators
  • Familiarity with positive definite operators
  • Concept of normal operators and their properties
NEXT STEPS
  • Study the spectral theorem for self-adjoint operators
  • Learn about diagonalization of operators in linear algebra
  • Explore the implications of commuting operators in functional analysis
  • Investigate the properties of eigenvalues and eigenvectors in inner product spaces
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Mathematicians, physics students, and anyone studying linear algebra or functional analysis, particularly those interested in operator theory and its applications in quantum mechanics.

steinmasta
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I have two questions:

1. Let V be a finite dimensional inner product space. Show that if U: V--->V is self-adjoint and T: V---->V is positive definite, then UT and TU are diagonalizable operators with only real eigenvalues.

2. Suppose T and U are normal operators on a finite dimensional complex inner product space V such that TU = UT

a) Show that UT* = T*U
b) show that there is an orthonormal basis for V consisting of vectors that are eigenvectors for both T and U
 
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What have you tried? We cannot help you before you have shown your work.
 
What do you know about positive, definite operators, and self-adjoint operators? Do you happen to know what field you're working with?
 
Regarding 1, I have tried to show that UT is self-adjoint with respect to the inner product <x,y>' = <T(x),y> but I've had trouble unwinding definitions.

Regarding 2a, I tried to show that if U commutes with T, then U commutes with T*. This corollary to the spectral theorem is useful: If F = C, T is normal iff T* = g(T) for some polynomial g, but I can't seem to make it work.

Regarding 2b, I am not sure where even to begin.
 
woah woah woah, don't forget the J in this if you don't know about that then you need a degree and if you've got one...
you need another one
 
1. Let V be a finite dimensional inner product space. Show that if U: V--->V is self-adjoint and T: V---->V is positive definite, then UT and TU are diagonalizable operators with only real eigenvalues.

Well you know that U:V--->V is self-adjoint, and therefore has an orthonormal basis of eigenvectors... you know that T:V---->V is Positive, and therefore also self-adjoint, and must also have an orthonormal basis of eigenvectors.

I believe you could also show that UT and TU are Self-adjoint operators from Inner Product algebra.

<Uv,u>=<v,Uu>
<Tv,u>=<v,Tu> and <Tv,v> > 0 for all v in V.
<UTv,u>=<v,(UT)*u>
<UTv,u>=<v,T*U*u>
<UTv,u>=<v,TUu>

(UT)* = T*U*=TU
(TU)*= U*T* = UT

Since U and T are both self-adjoint, TU=UT (Chose the orthonormal basis of eigenvectors, it's the product of the diagonal entries of the respective matrices, and diagonal matrices commute)

I hope that helps. (I might be mistaken, so if anything seems fishy let me know. I'm a freshman and just finished this stuff like three weeks ago... so yeah ;p)
 

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