[Q]Eigenfunction of inverse opreator and another question.

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The discussion centers on the eigenfunction of the inverse operator \(\hat{A^{-1}}\) given that \(\hat{A}\varphi = a\varphi\), asserting that the eigenfunction remains \(\varphi\) with eigenvalue \(\frac{1}{a}\). A proof is sought for this relationship, alongside a query about the commutator theorem, which states that if \([A, A^{-1}] = 0\), both operators share a common eigenfunction when eigenvalues are non-degenerate. The conversation also addresses the application of the operators, clarifying that \(AA^{-1} = 1\) holds true, but applying this to functions requires careful consideration of operator equality. Ultimately, it emphasizes that operators are equal if they yield the same result for all functions.
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Hi.

Do you know eigenfunction of inverse operator, for instance \hat{A^{-1}} given that \hat{A}\varphi = a\varphi

textbook said eigenfunction of inverse operator A is the same as \varphi

which eigenvalue is \frac{1}{a}

Can you prove that?

And is it really that [A,A^{-1}] = 0 so both opreatator have a common
eigenfunction if eigenvalue is not degenerate, this theorem is called commutator theorem?
 
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Just operate with A^-1 so you get A^{-1}A\phi =\phi =a A^{-1}\phi.
No need to commute A with its inverse.
Then proving the commutator=0 follows.
 
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The latex doesn't seem to work. The last term is \phi=a A^{-1} \phi.
 
I don't understand why AA^{-1}\varphi = \varphi It is absolute true that

AA^{-1} = 1 But applying AA^{-1} to some function is

different matter. for example we assume A and its inverse can be matrix, function f is also matrix.

A(A^{-1}f) is not (AA^{-1})f right?
 
Hm, yes, the law of association holds for matrices, so those two last expressions are equal.
 
good_phy said:
It is absolute true that

AA^{-1} = 1 But applying AA^{-1} to some function is

different matter.
No, it can't be a different matter. To say that two operators X and Y are equal means that Xf=Yf for all functions f. This is no different from saying that two functions f and g are equal if f(x)=g(x) for all x.
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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