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Quantum mechanics I Fall 2012

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Presentation on theme: "Quantum mechanics I Fall 2012"— Presentation transcript:

1 Quantum mechanics I Fall 2012
Physics 451 Quantum mechanics I Fall 2012 Sep 17, 2012 Karine Chesnel

2 Monday: Review- Practice test Plan to work on your selected problem
Quantum mechanics Announcements Homework this week: Tuesday Sep 18 by 7pm: HW # 6 pb 2.10, 2.11, 2.12, 2.13, 2.14 Thursday Sep 20 by 7pm: HW # 7 pb 2.19, 2.20, 2.21, 2.22 Monday: Review- Practice test Plan to work on your selected problem with your group and prepare the solution to be presented in class (~ 5 to 7 min)

3 No student assigned to the following transmitters
Quantum mechanics No student assigned to the following transmitters 17A79020 1E71A9C6 Please register your i-clicker at the class website!

4 Harmonic oscillator Quantum mechanics Ch 2.3
x V(x) Solving the Schrödinger equation: Expressing the Hamiltonian in terms of convenient operators: or

5 In this definition, the states
Quantum mechanics Ch 2.3 Harmonic oscillator Ladder operators: Raising operator: Lowering operator: In this definition, the states are normalized

6 Quiz 8a Quantum mechanics What will be the final state of the particle
after applying this operator? (ignore the coefficients)

7 Harmonic oscillator Quantum mechanics Ch 2.3 Stationary states
The ground state is given by the condition Ground energy

8 Harmonic oscillator Pb 2.10 Quantum mechanics Ch 2.3 Stationary states
The stationary states are orthonormal Hermite polynomials Pb 2.10 Building and Checking the orthogonality

9 Quantum mechanics Ch 2.3 Harmonic oscillator Energy levels x V(x)

10 Expressing x, p and H in terms of ladder operators:
Quantum mechanics Ch 2.3 Harmonic oscillator Expressing x, p and H in terms of ladder operators: Operator position Operator momentum Operator Hamiltonian

11 Harmonic oscillator Pb 2.11, 2.12 Quantum mechanics Ch 2.3
x V(x) Expectation values Pb 2.11, 2.12

12 Quiz 8b True False Pb 2.13 Quantum mechanics
Since the operators a+ and a- are shifting the stationary states from one level to another, and since the stationary states are all orthogonal, the expectations values for x and p on any state will ALWAYS be zero! True False Pb 2.13


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