Hermitian Operators in Dirac Equation

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SUMMARY

The discussion centers on the necessity of Hermitian operators in the context of the Dirac equation, specifically regarding the term proportional to \(\alpha p\). It is established that \(\alpha\) must be a Hermitian operator to ensure the Hamiltonian remains Hermitian. The participants clarify that while the product \((\alpha p)^\dagger\) results in a change of order, the commutation of the operators \(\alpha\) and \(p\) allows for the preservation of Hermitian properties. This understanding is crucial for maintaining the physical validity of quantum mechanical systems described by the Dirac equation.

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Higgsono
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In the dirac equation we have a term which is proportional to \alpha p. In the book they say that
\alpha must be an hermitian operator in order for the Hamiltonian to be hermitian.

As I understand, we require this because we want (\alpha p)^\dagger = \alpha p.

But (\alpha p)^\dagger = p^\dagger \alpha^\dagger = p \alpha, and so the order of the operators still change.

So if we just require both operators to be hermitian their product will still change if we take the hermitian conjugate.
 
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##p## acts on spatial part whereas ##\alpha## on spin part so the two operators commute.
 
blue_leaf77 said:
##p## acts on spatial part whereas ##alpha## on spin part so the two operators commute.

ok, thanks!
 

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