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Quantum mechanics I Fall 2012
Physics 451 Quantum mechanics I Fall 2012 Sep 14, 2012 Karine Chesnel
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Homework Friday Sep 14 by 7pm: HW # 5 pb 2.4, 2.5, 2.7, 2.8
Quantum mechanics Homework Friday Sep 14 by 7pm: HW # 5 pb 2.4, 2.5, 2.7, 2.8 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
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No student assigned to the following transmitters
Quantum mechanics No student assigned to the following transmitters 1E2B2F1A 1E5C6E2C 1E71A9C6 Please register your i-clicker at the class website!
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Infinite square well Quantum mechanics Ch 2.2
Properties of the wave functions yn: 1.They are alternatively even and odd around the center Excited states 2. Each successive state has one more node 3. They are orthonormal Ground state a x 4. Each state evolves in time with the factor
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Infinite square well Pb 2.4 Pb 2.5 Quantum mechanics Ch 2.2
Particle in one stationary state Pb 2.5 Particle in a combination of two stationary states evolution in time? oscillates in time expressed in terms of E1 and E2
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Quiz 7a Could this function be the wave function
Quantum mechanics Quiz 7a Could this function be the wave function of a particle in an infinite square well at a given time? x a Yes No Pb. 2.7
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Decomposition of any wave function
Quantum mechanics Ch 2.2 Infinite square well Decomposition of any wave function At time t = 0 Fourier’s series expansion
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How to find the coefficients cn?
Quantum mechanics Ch 2.2 Infinite square well How to find the coefficients cn? Dirichlet’s theorem Pb. 2.7 & 2.8
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Expectation value for the energy:
Quantum mechanics Ch 2.2 Infinite square well Expectation value for the energy: The probability that a measurement yields to the value En is Normalization
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Quiz 7b Could this function be a solution for the wave function
Quantum mechanics Quiz 7b Could this function be a solution for the wave function of a particle in an infinite square well at a given time? x a Yes No
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Quantum mechanics Ch 2.3 Harmonic oscillator x V(x)
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Solving the Schrödinger equation:
Quantum mechanics Ch 2.3 Harmonic oscillator Solving the Schrödinger equation: x V(x)
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Harmonic oscillator Quantum mechanics Ch 2.3
x V(x) Expressing the Hamiltonian in terms of convenient operators: Commutator: or
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Harmonic oscillator Quantum mechanics Ch 2.3 Ladder operators:
If y is a solution the Schrödinger equation for energy E Then is a solution the Schrödinger equation for energy Quantization of energy And is a solution the Schrödinger equation for energy We can built all the solutions just starting from one solution (ground level)
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Starting from ground state
Quantum mechanics Ch 2.3 Harmonic oscillator Ladder operators: Raising operator: Lowering operator: Starting from ground state
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