Question about hermitian operators

In summary, the spectral theorem states that every Hermitian operator has at least one basis consisting of its orthonormal eigen vectors. This basis is diagonal and the eigenvalues are the diagonal entries. The theorem applies to selfadjoint operators in a Hilbert space and is a fundamental result in functional analysis. There are different versions of the theorem for different types of operators, with varying levels of complexity in their proofs. The most general version is able to handle even momentum eigenstates but requires a deep understanding of functional analysis, topology, and measure theory.
  • #1
O.J.
199
0
Theorem: For every Hermitian operator, there exists at least one basis consisting of its orthonormal eigen vectors. It is diagonal in this basis and has its eigenvalues as its diagonal entries.

The theory is apparently making an assumption that every Hermitian operator must have eigen values/vectors. Am I missing something here? Should ALL hermitian operators have eigen values/vectors?
 
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  • #2
Yes, that is the essential content of the spectral theorem for selfadjoint operators in a Hilbert space which is one of the most widely known results of functional analysis.
 
  • #3
Is there a proof? Can you link me to one? =)
 
  • #4
There's no proof that can be fully understood by a typical physics student in less than a year. However, most linear algebra books contains a proof of the finite-dimensional case. (Look for the words "spectral theorem" in any of them).

There's a spectral theorem for compact normal operators that has a proof that can be understood by someone who's good at linear algebra and topology, and only covers a few pages. You might be interested in that, but you will need to learn a non-negligible amount of topology.

The spectral theorem for bounded normal operators is the really hard one. You need lots of functional analysis, topology and measure theory for that one. The two simpler theorems mentioned above are special cases of this one.

However, the one for bounded normal operators is a special case of the one for arbitrary (not necessarily bounded) normal operators, and even that one can't handle things like momentum eigenstates. For that you need an even more general spectral theorem.
 

Related to Question about hermitian operators

1. What is a hermitian operator?

A hermitian operator is a type of linear operator in quantum mechanics that has a special property where the adjoint of the operator is equal to the operator itself.

2. What is the significance of hermitian operators in quantum mechanics?

Hermitian operators are important in quantum mechanics because they represent physical observables, such as energy, momentum, and position. They also have real eigenvalues, which correspond to the measurable values of these observables.

3. How do you determine if an operator is hermitian?

To determine if an operator is hermitian, you need to take the adjoint of the operator and see if it is equal to the original operator. If they are equal, then the operator is hermitian.

4. Can non-hermitian operators exist?

Yes, non-hermitian operators can exist, but they do not have physical significance in quantum mechanics. They do not have real eigenvalues and do not represent physical observables.

5. What is the difference between hermitian and unitary operators?

While hermitian operators have the property that their adjoint is equal to the operator itself, unitary operators have the property that their adjoint is equal to the inverse of the operator. Unitary operators are important in quantum mechanics as they represent transformations that preserve the normalization of quantum states.

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