The generator of time translation

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SUMMARY

The Hamiltonian operator, denoted as \(\hat{H}\), serves as the generator of time translation in quantum mechanics (QM), specifically through the relationship \(e^{-i\hat{H}t/\hbar}\). This relationship illustrates how the Hamiltonian generates the time evolution of quantum states. The discussion emphasizes that while the exponential of the Hamiltonian represents time evolution, the Hamiltonian itself is the generator of this transformation, aligning with the principles of Lie groups and algebras. The momentum operator similarly generates spatial translations, while angular momentum operators generate rotations, reinforcing the connection between quantum mechanics and group theory.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly wave functions and operators.
  • Familiarity with Hamiltonian mechanics and its role in time evolution.
  • Basic knowledge of Lie groups and Lie algebras.
  • Concept of exponential maps in mathematical physics.
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  • Study the mathematical foundations of Lie groups and Lie algebras in quantum mechanics.
  • Explore the implications of the Hamiltonian as a generator of time evolution in various quantum systems.
  • Investigate the relationship between momentum operators and spatial translations in quantum mechanics.
  • Learn about the role of angular momentum operators in generating rotations within quantum systems.
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Physicists, quantum mechanics students, and researchers interested in the mathematical foundations of quantum theory and its applications in understanding time evolution and symmetries in physical systems.

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It is not hard to show that for QM what takes the wave function from t->t+Δt is the exponential of the hamiltonian. Yet for some mysterious reason my book decides to note the Hamiltonian as the generator of time translation rather than the exponential of it. What is the reason for this?
 
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In the theory of lie groups a generator is defined as the element of the tangential lie algebra that generates the group element. The map from the lie algebra to the lie group is the exponential, so the generator of time evolution is the hamiltonian and the one dimensional subgroup it generates is the time evolution exp(i H t).

You find the same situation for the momentum operator and the spatial translation group it generates. And angular momentum operators generate rotations.
 
Books on QM tend to speak from the perspective of group theory, even though they don't/may not contain chapters on Lie groups/algebras and their applications to quantum physics.
 
The lie algebra has to do with what happens close to the identity. We can take what is given: e^{-i\hat{H}t} is the generator of finite time translations, and see how this portrays the Hamiltonian.
<br /> e^{-i\hat{H}\epsilon / \hbar}\psi(x,t) = \psi(x,t+\epsilon)<br />
now for \epsilon \approx 0 we can write
<br /> \psi(x,t)-\frac{i\hat{H}\epsilon}{\hbar}\psi(x,t) +\mathcal{O}(\epsilon^2) = \psi(x,t)+ \left. \frac{\partial \psi(x,t)}{\partial t}\right|_{t=\epsilon}\epsilon +\mathcal{O}(\epsilon^2)<br />
thus
<br /> \hat{H} = i\hbar \frac{\partial}{\partial t}<br />
 

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