Expectation value of an operator to the power of n

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SUMMARY

The discussion centers on proving the equality \( \langle A^{n} \rangle = \langle A \rangle^{n} \) for an operator \( A \). The proof provided by the user demonstrates that both sides equal \( \lambda^{n} \) when \( \Psi \) is an eigenstate of \( A \) with eigenvalue \( \lambda \). However, it is noted that this equality does not hold in general, particularly when considering the variance for \( n = 2 \), where \( \sigma^2(A) = \langle A^2 \rangle - \langle A \rangle^2 \) can be non-zero. A more general approach involves using the Binomial Theorem to expand \( \langle [A - \langle A \rangle]^n \rangle \).

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Quantum mechanics students, physicists, and researchers interested in operator theory and statistical properties of quantum systems.

patric44
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Homework Statement
prove that : <A^n>=<A>^n
Relevant Equations
<A^n>=<A>^n
hi all
how do I prove that
$$
<A^{n}>=<A>^{n}
$$
It seems intuitive but how do I rigorously prove it, My attempt was like , the LHS can be written as:
$$
\bra{\Psi}\hat{A}.\hat{A}.\hat{A}...\ket{\Psi}=\lambda^{n} \bra{\Psi}\ket{\Psi}=\lambda^{n}\delta_{ii}=\lambda^{n}
$$
and the RHS equal:
$$
<A>^{n}=[\bra{\Psi}A\ket{\Psi}]^{n}=\lambda^{n}[\bra{\Psi}\ket{\Psi}]^{n}=\lambda^{n}[\delta_{ii}]^{n}=\lambda^{n}
$$
Is my proof rigurus enough or there are other formal proof for that
 
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A counter example. For ground state of a partricle in a box [-a,a],
<x>=0 but &lt;x^2&gt; \ \ &gt;\ \ &lt;x&gt;^2=0

Your proof seems to be all right only when ##\Psi## is an eigenstate of A with eigenvalue ##\lambda##.
 
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patric44 said:
Homework Statement: prove that : <A^n>=<A>^n
Note that for ##n = 2##, the variance is not necessarily zero:
$$\sigma^2(A) =\langle A^2 \rangle - \langle A \rangle^2 \ne 0$$In general, you can derive an expression for ##\langle A^n \rangle - \langle A \rangle^n## by starting with:
$$\langle[A - \langle A \rangle]^n \rangle$$And expanding using the Binomial Theorem.
 
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