Hermitian Operators: Meaning & Showing Properties

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A Hermitian operator is defined as one that is equal to its adjoint, meaning A is contained within its adjoint A†. To show that combinations of operators like O + O†, i(O - O†), and OO† are Hermitian, one must consider the properties of their matrix elements and the assumption of bounded operators over the Hilbert space. The transformation of matrix elements under the adjoint operation is crucial, as it reveals that if O† = O, then the matrix elements must also satisfy specific symmetry conditions. The discussion emphasizes the importance of understanding operator domains and the implications of operator adjoints in quantum mechanics. Overall, the properties of Hermitian operators are foundational in quantum theory.
sunsun
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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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It means to be included in its adjoint. By definition

A\subseteq A^{\dagger} \ \mbox{means that A is hermitian/symmetric} [/itex]<br /> <br /> As for the second part, I&#039;m sure the question is ill posed, as there&#039;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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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:

\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 ) ^*
by definition. But if \mathcal{O}^\dagger = \mathcal{O}, what does that mean about the matrix elements?
 
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?
 
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

(O+O^{\dagger})^{\dagger}\supseteq O^{\dagger}+O^{\dagger\dagger} \supseteq O^{\dagger}+O ,

since O\subseteq O^{\dagger\dagger}
 
Time reversal invariant Hamiltonians must satisfy ##[H,\Theta]=0## where ##\Theta## is time reversal operator. However, in some texts (for example see Many-body Quantum Theory in Condensed Matter Physics an introduction, HENRIK BRUUS and KARSTEN FLENSBERG, Corrected version: 14 January 2016, section 7.1.4) the time reversal invariant condition is introduced as ##H=H^*##. How these two conditions are identical?

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