Make an operator to be hermitian

In summary, the conversation discusses the properties of operators in quantum mechanics, specifically the Hermitian property and its relationship to continuous transformations and symmetry. It is mentioned that any operator can be written in the form H = A + iB where A and B are Hermitian, and this allows for the use of the Born Rule in calculations. The reason for using Hermitian operators is due to the properties of continuous transformations and symmetry, as proven by Wigner's theorem. Finally, it is noted that in order to associate an observation with the operator, it must be divided by i, leading to a real operator.
  • #1
masoodsa
1
0
I have an operator which isnot Hermitian is there any way to make it hermitian ?
 
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  • #2
add its hermitian conjugate and redefine it.
 
  • #3
Any operator can be written of the form H = A + iB where A and B are Hermitian.

In fact one could base QM on any operator using that result via the obvious extension to the Born Rule E(H) = E(A) + i E(B)

Interestingly in proving the Born rule via Gleason that's what one does.

So why does one stick with Hermitan operators? The reason is the properties of continuous transformations between states and symmetry. Wigners Theroem implies such must be Unitary:
http://en.wikipedia.org/wiki/Wigner's_theorem

If U is such a transformation dependant on t (not necessarily time) and we consider Δt small. U(Δt) = 1 + D Δt. UU(bar) = 1 + DΔt + D(bar)Δt = 1 or D = -D(bar) which means D is pure imaginary. If we want to associate D with an observation, which from symmetry considerations you want to do because it leads to the same equations as classical physics (see Ballentine chapter 3), then its expectation would be imaginary as well which would be a rather strange thing. So what we do is define divide D by i and use that operator which is of course real.

Thanks
Bill
 

1. What does it mean for an operator to be hermitian?

Being hermitian means that the operator is equal to its own conjugate transpose, or in simpler terms, it is symmetric about the main diagonal.

2. Why is it important for an operator to be hermitian?

Hermitian operators have many important properties, including that their eigenvalues are real and their eigenvectors are orthogonal. This makes them useful in quantum mechanics and other areas of physics.

3. How can an operator be made hermitian?

An operator can be made hermitian by taking its conjugate transpose and multiplying it by a constant factor. This ensures that the operator is equal to its own conjugate transpose and thus, hermitian.

4. What happens if an operator is not hermitian?

If an operator is not hermitian, then its eigenvalues may not be real and its eigenvectors may not be orthogonal. This can cause problems in calculations and may not accurately represent physical systems.

5. Can any operator be made hermitian?

No, not all operators can be made hermitian. Only operators that satisfy certain conditions, such as being linear and having a symmetric matrix representation, can be made hermitian.

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