The time evolution operator (QM) Algebraic properties

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SUMMARY

The discussion centers on the time evolution operator in quantum mechanics, specifically using the Hamiltonian defined as H = -ħω/2 σ_y, where σ_y is the Pauli Y matrix. The time evolution operator U(t) is derived from the time-dependent Schrödinger equation, resulting in U(t) = e^(iωt/2 σ_y). Participants explore the mathematical treatment of this operator, particularly focusing on the exponential of a finite matrix and the identities that facilitate moving operators out of the exponent.

PREREQUISITES
  • Understanding of quantum mechanics principles, particularly the Schrödinger equation.
  • Familiarity with Hamiltonians and their role in quantum systems.
  • Knowledge of matrix exponentiation and properties of finite matrices.
  • Proficiency in using Pauli matrices in quantum mechanics.
NEXT STEPS
  • Study the derivation of the time evolution operator in quantum mechanics.
  • Learn about the properties of matrix exponentials, specifically for finite matrices.
  • Explore the implications of the Pauli Y matrix in quantum state transformations.
  • Investigate identities that allow manipulation of operators within exponentials.
USEFUL FOR

This discussion is beneficial for quantum mechanics students, physicists working with quantum systems, and researchers interested in the algebraic properties of time evolution operators.

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Homework Statement



The hamiltonian for a given interaction is

H=-\frac{\hbar \omega}{2} \hat{\sigma_y}

where

\sigma_y = \left( \begin{array}{cc} 0 & i \\ -i & 0 \end{array} \right)

the pauli Y matrix

Homework Equations

The Attempt at a Solution



So from the time dependent Schrödinger equation we, can take the time dependence and put it into the time evolution operator U(t)

HU(t)\left|\Psi(r,0)\right>=i\hbar \frac{d}{dt}U(t)\left|\Psi(r,0)\right>

becomes

i\hbar\frac{d}{dt}U(t) = HU(t)

so for a non time dependent Hamiltonian H, this means:

U(t) = e^{-\frac{i}{\hbar}H t}

so we have then:

U(t) = e^{\frac{i\omega t}{2}\hat{\sigma_y}}

How do you treat this? Is there any particular identity that allows you to move the operator out of the exponent?
 
Last edited:
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edit: changed the matrix to the correct form
 
Do you know how the exponential of a finite matrix is defined? If so, use the definition.
 

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