Probability Amplitude and Time Evolution Operator

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SUMMARY

The discussion focuses on the evaluation of the probability amplitude in quantum physics, specifically transitioning between two time-dependent states, \Psi_{1} and \Psi_{2}, using the time evolution operator derived from the Hamiltonian \hat{H} = \frac{1}{2m}\partial^2/x^2 + V(x). The operation to find the probability amplitude is expressed as <\Psi_{2}|exp(-i\hat{H}(t2-t1))|\Psi_{1}>. The user seeks clarification on evaluating exp(\hat{H})\Psi_{1}, which can be approached through the Taylor series expansion of the exponential function of the operator, leading to the conclusion that if \Psi is an eigenfunction of \hat{H}, then exp(\hat{H})\Psi = exp(E)\Psi.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly time-dependent states.
  • Familiarity with Hamiltonian operators and their role in quantum physics.
  • Knowledge of eigenfunctions and eigenvalues in the context of quantum operators.
  • Basic grasp of Taylor series expansions and their application to operator functions.
NEXT STEPS
  • Study the derivation and applications of the time evolution operator in quantum mechanics.
  • Learn about the implications of Hamiltonian operators in quantum systems.
  • Explore the concept of eigenstates and eigenvalues in quantum mechanics.
  • Investigate advanced techniques for evaluating functions of operators, including perturbation theory.
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Students and professionals in physics, particularly those studying quantum mechanics, as well as engineers seeking to understand quantum principles and their applications in technology.

erkokite
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Hello,

I am fairly new to quantum physics (I'm actually an engineer, not a physicist). I think I am getting a decent grasp on things, but I have a question.

Suppose you have two time dependent states: [tex]\Psi_{1}[/tex] and [tex]\Psi_{2}[/tex].

Also, suppose that we have a constant potential, represented in our Hamiltonian as V.

Our Hamiltonian is thus represented as: [tex]\hat{H}=1/(2m)\partial^2/x^2+V(x)[/tex]

Now suppose that we want to find the probability amplitude to go from state 1 to the 2nd state in a time interval t1 to t2.

It is my understanding that the following operation is used:

[tex]<\Psi_{2}|exp(-i\hat{H}(t2-t1))|\Psi_{1}>[/tex]

This is of course equal to

[tex]\int\Psi_{2}*exp(-i\hat{H}(t2-t1))\Psi_{1}dx[/tex]

However, how do I evaluate the following operation?

[tex]exp(\hat{H})\Psi_{1}[/tex]

Many thanks.
 
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The general idea of evaluating a function of an operator is to expand the function...

exp(H) = 1 + H + H^2/2 + H^3/6 + ...

If Psi is an eigenfunction of H with eigenvalue E, then it is not hard to show that exp(H) Psi = exp(E) Psi.
 

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