Operators and eigenstates/values

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Homework Help Overview

The discussion revolves around the properties of Hermitian operators in quantum mechanics, specifically focusing on the representation of an operator in terms of its eigenstates and eigenvalues. The original poster is tasked with demonstrating a specific form for the operator based on its eigenstates and eigenvalues.

Discussion Character

  • Conceptual clarification, Mathematical reasoning

Approaches and Questions Raised

  • The original poster attempts to start with the action of the operator on an arbitrary state but expresses confusion about the next steps. Some participants suggest considering the identity operator and its relation to the eigenstates. Others inquire about the completeness theorem and its relevance to the problem.

Discussion Status

Participants are exploring different aspects of the problem, including the completeness theorem and its implications for the operator's representation. Some guidance has been offered regarding the identity operator and its decomposition into eigenstates, but there is no explicit consensus on the approach to take.

Contextual Notes

There is a mention of the original poster seeking help from an instructor, indicating possible constraints in understanding the material. The discussion also touches on the completeness theorem, which may be a key concept in resolving the problem.

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Homework Statement


Let the Hermitian operator A^ corresponding to the observable A have two eigenstates |a1> and |a2> with eigenvalues a1 and a2, respectively, where a1 ≠ a2. Show that A^ can be written in the form A^ = a1|a1><a1| + a2|a2><a2|.

Homework Equations

The Attempt at a Solution


I reached out the instructor for some guidance but I am still confused.
To my understanding i should start with A^|ψ>. Where |ψ> is some arbitrary spin state.
and i don't know where to go from there.
 
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The identity operator can be written as

$$
1 = |1\rangle \langle 1| + |2\rangle \langle 2| \\
$$

For example suppose ##|\psi\rangle = c_1 |1\rangle + c_2|2\rangle##
$$ |\psi \rangle = 1|\psi \rangle = |1\rangle \langle 1|\psi\rangle + |2\rangle \langle 2| \psi \rangle \\
= |1\rangle c1 + |2\rangle c2 \\
= |\psi \rangle
$$

Suppose you tried putting "1" on both sides of your operator?
 
Have you heard about completeness theorem?
 
Thank you zhaos, that's actually a lot of help.

Blue leaf, I have not heard of completeness theorem. But I will give it a Google!
 
Completeness theorem is exactly what zhaos wrote in the first equation in his post.
 

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