Hermitian Operators: Meaning & Showing Properties

In summary, an operator is said to be hermitian if it is included in its adjoint, represented by the dagger. To prove that an operator is hermitian, you can assume a basis for the operators and look at how the matrix elements transform. In order to show that O+O' , i(O-O') and OO' are hermitian, you would need to consider the domain of the operators and use the definition of the adjoint.
  • #1
sunsun
2
0
1.What does it mean for an operator to be hermitian?

Note: the dagger is represented by a '
2. How do I show that for any operator ie/ O' that O + O' , i(O-O') and OO' are hermitian?

Thanks in advanced
 
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  • #2
It means to be included in its adjoint. By definition

[tex] A\subseteq A^{\dagger} \ \mbox{means that A is hermitian/symmetric} [/itex]

As for the second part, I'm sure the question is ill posed, as there's no mentioning of domains for the operators. you can simplify it by assuming the involved operators are bounded, hence defined on all the Hilbert space.
 
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  • #3
Typically in a quantum mechanics course, you can assume a basis for your operators that they will span. To prove that the above operators are Hermitian, you'd want to look at how the matrix elements transform:

[tex]\langle n | \left ( \mathcal{O} | m \rangle \right ) = \left ( \langle n | \mathcal{O}^\dagger \right ) | m \rangle = \langle m | \left ( \mathcal{O}| n \rangle \right ) ^*[/tex]
by definition. But if [tex]\mathcal{O}^\dagger = \mathcal{O}[/tex], what does that mean about the matrix elements?
 
  • #4
Im sorry, I don't really get that.

How would I go around starting to answer the Q2? I know that O' = O
But how would I show that O+O' is hermitian?
 
  • #5
sunsun said:
Im sorry, I don't really get that.

How would I go around starting to answer the Q2? I know that O' = O
But how would I show that O+O' is hermitian?

I'll let you figure out the domain issues, but

[tex] (O+O^{\dagger})^{\dagger}\supseteq O^{\dagger}+O^{\dagger\dagger} \supseteq O^{\dagger}+O [/tex] ,

since [itex] O\subseteq O^{\dagger\dagger} [/itex]
 

FAQ: Hermitian Operators: Meaning & Showing Properties

What is the definition of a Hermitian operator?

A Hermitian operator is a mathematical object used in quantum mechanics to represent observable quantities such as energy or momentum. It is defined as an operator that is equal to its own adjoint, or conjugate transpose.

How do you show that an operator is Hermitian?

To show that an operator is Hermitian, you must take its adjoint (conjugate transpose) and compare it to the original operator. If they are equal, then the operator is Hermitian. This can also be represented mathematically as A=A*.

What are the properties of Hermitian operators?

Hermitian operators have several important properties, including being self-adjoint, having real eigenvalues, and having orthogonal eigenvectors. They also have the property that the expectation value of an observable quantity represented by the operator is always a real number.

Why are Hermitian operators important in quantum mechanics?

Hermitian operators are important in quantum mechanics because they represent observable quantities, which are the fundamental building blocks of the theory. They also have several important properties that make them useful in calculations and predictions of quantum systems.

How are Hermitian operators related to the uncertainty principle?

The uncertainty principle, which states that certain pairs of physical properties cannot be known simultaneously with perfect accuracy, is related to Hermitian operators through the commutation relation. This relation governs how two operators representing different physical quantities behave mathematically, and it is a key concept in understanding the uncertainty principle.

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