Hermitian operator proof

In summary: Since a and a' are arbitrary vectors, this holds true for all vectors in the vector space, and thus, the operator O is Hermitian.In summary, we have proven that if for an arbitrary vector a in the vector space, the operator O satisfies the condition (a,Oa) = (Oa, a), then O is Hermitian. I hope this helps you better understand the concept of a Hermitian operator. Keep up the good work!
  • #1
Lchan1
39
0

Homework Statement


A Hermitian operator is such that, for arbitrary vectors ai and aj
in a vector space,we have (ai,Oaj) = (Oai, aj).
Prove that if for an arbitrary vector a in the vector space, the operator O satisfies
(a,Oa) = (Oa, a),
then O is Hermitian


Homework Equations





The Attempt at a Solution



Our prof gave us a hint:
let a=a1+z1a2 and a=a1+z2a2. and find the appropriate zs to satisfy the proof. I tried doing the inner product using the different a. and got myself no where.
 
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  • #2


Dear student,

Thank you for your post. It is great to see that you are seeking help with your work. I am a scientist and I would be happy to assist you in solving this problem. Let's start by defining a Hermitian operator. A Hermitian operator is a linear operator that satisfies the condition (ai,Oaj) = (Oai, aj) for all arbitrary vectors ai and aj in a vector space. This means that the operator O is symmetric with respect to the inner product of the vectors ai and aj. In other words, the order of the vectors in the inner product does not matter when the operator O is applied.

Now, let us consider the given condition (a,Oa) = (Oa, a) for an arbitrary vector a in the vector space. We want to prove that this condition implies that the operator O is Hermitian. To do this, we can use the hint given by your professor. Let us define two vectors a1 and a2 such that a = a1 + za2. Substituting this into the given condition, we get:

(a,Oa) = (Oa, a)
(a,a1 + za2) = (Oa, a1 + za2)
(a,a1) + z(a,a2) = (Oa, a1) + z(Oa, a2)

Now, let us define another vector a' = a1 + z'a2, where z' is a different value of z. Substituting this into the condition, we get:

(a',Oa') = (Oa', a')
(a',a1 + z'a2) = (Oa', a1 + z'a2)
(a',a1) + z'(a',a2) = (Oa', a1) + z'(Oa', a2)

Since a' and a are arbitrary vectors, we can equate the terms in the above two equations to get:

(a,a1) + z(a,a2) = (a',a1) + z'(a',a2)
(a,a1) = (a',a1)
z(a,a2) = z'(a',a2)

Since z and z' are different values, this can only be true if (a,a2) = (a',a2). This implies that the operator O is symmetric with respect to the inner product of the vectors a and
 

1. What is a Hermitian operator?

A Hermitian operator is a mathematical object that describes a physical observable in quantum mechanics. It is a linear operator that is equal to its own adjoint (Hermitian conjugate).

2. How do I prove that an operator is Hermitian?

To prove that an operator is Hermitian, you need to show that it is equal to its own adjoint. This can be done by taking the complex conjugate of the operator and comparing it to the original operator.

3. Why is it important to determine if an operator is Hermitian?

In quantum mechanics, Hermitian operators represent physical observables, such as position, momentum, and energy. These operators have important properties that allow us to make predictions about the behavior of a quantum system.

4. What are some properties of Hermitian operators?

Some properties of Hermitian operators include that their eigenvalues are real, their eigenvectors are orthogonal, and they can be diagonalized by a unitary transformation.

5. Can a non-Hermitian operator be used in quantum mechanics?

Yes, non-Hermitian operators can be used in quantum mechanics, but they do not represent physical observables. They may be used in certain mathematical calculations or to model non-physical systems.

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