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Lecture 15: Time-Dependent Perturbation

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1 Lecture 15: Time-Dependent Perturbation
Source: D. Griffiths, Introduction to Quantum Mechanics (Prentice Hall, 2004) R. Scherrer, Quantum Mechanics An Accessible Introduction (Pearson Int’l Ed., 2006) R. Eisberg & R. Resnick, Quantum Physics of Atoms, Molecules, Solids, Nuclei and Particles (Wiley, 1974)

2 Two-Level Systems and are eigenstates of an unperturbed Hamiltonian
These states are orthonormal. Any state can be written as: Time-dependent expression in the absence of perturbation: Probability that a measurement of energy would yield the value Ea. Normalization of the function:

3 Perturbed System Time-Dependent Perturbations
Time-Dependent Schroedinger Equation

4 Perturbed System Take inner product with Ψa, and use orthogonality of Ψa and Ψb. Multiply through by

5 Perturbed System

6 Example: Problem 9.1

7 Example: Problem 9.1

8 Time-Dependent Perturbation Theory
If H’ is small, the above equations can be solved by successful approximations. Suppose Particle starts from lower state Zeroth order: First order: Second Order:

9 Interaction of Light with Atoms
Absorption Stimulated Emission. Laser: Light amplification by stimulated emission of radiation. Population Inversion: Majority of atoms in upper state. Spontaneous Emission: An atom in the excited state makes a transition downwards, release a photon without any applied EM field to initiate process. 9

10 Sinusoidal Perturbation
Assume: Transition Probability: The probability that a particle which started out in state Ya will be found at time t, in the state Yb.

11 Sinusoidal Perturbation
Transition probability as a function of driving frequency. The probability of transition is greatest at wo.

12 Emission and Absorption of Radiation: EM Waves
Therefore, the diagonal matrix elements of H’ vanish.

13 Probability of Transition
If atom starts out in lower state Ya, a polarized monochromatic is shone on it, the probability of transition to upper level (absorption): The probability of transition to lower level (emission): The probabilities are equal, it just switching from a to b , and b to a.

14 Problem 1

15 Problem 2


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