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Chapter 5: Quantum Mechanics
Limitations of the Bohr atom necessitate a more general approach de Broglie waves –> a “new” wave equation “probability” waves classical mechanics as an approximation Wave Function Y probability amplitude
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Mathematical properties of the wave function
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More mathematical properties of the wave function
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The classical wave equation as an example of a wave equation:
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Time dependent Schrödinger Equation
linear (in Y) partial differential equation
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Expectation values (average values)
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If the potential energy U is time independent,
Schrödinger equation can be simplified by “factoring” separation of variables Total energy can have a constant (and well defined) value Consider plane wave: An eigenvector, eigenvalue problem!
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The time independent Schrödinger equation
Allowed values for (some) physical quantities such as energy are related to the eigenvalues/eigenvectors of differential operators eigenvalues will depend on the details of the wave equation (especially in U) and on the boundary conditions
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Particle in a box: (infinite) potential well
U Particle in a box: (infinite) potential well L V0 x
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Wavefunction normalization
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Example Find the probability that a particle trapped in a box L wide can be found between .45L and .55L for the ground state and for the first excited state. Example 5.4 Find <x> for a particle trapped in a box of length L
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Particle in a box: finite potential well
U Particle in a box: finite potential well L V0 E x I II III
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U Boundary Conditions L V0 E x I II III
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c = 4 c = 100 c = 1600
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Tunneling U L V0 E x I II III
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U Boundary Conditions L V0 E x I II III
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Example 5. 5: Electrons with 1. 0 eV and 2
Example 5.5: Electrons with 1.0 eV and 2.0 eV are incident on a barrier 10.0 eV high and 0.50 nm wide. (a) Find their respective transmission probabilities. (b) How are these affected if the barrier is doubled in width?
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Harmonic Oscillator: classical treatment
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Quantum Oscillator
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Quantum Harmonic Oscillator Solutions
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Operators
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Example 5. 6: An eigenfunction of the operator d 2 /dx 2 is y = e2x
Example 5.6: An eigenfunction of the operator d 2 /dx 2 is y = e2x. Find the corresponding eigenvalue.
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Chapter 5 exercises: 4, 5, 6, 11, 23
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