Study
guide for Physics 410 Final Exam
Dec
17, 2010 8 a.m.-10a.m. in P-149
Fine print: although
this guide is intended to help you, it is not guaranteed to cover or prepare you for every question
on the exam.
The structure of the exam will be very similar to previous
exams. There will be emphasis on material covered since Exam II. Open books, open notes, no calculators.
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Interpretation of coordinate-space wavefunction ψ(x) as probability.
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Set up expectation values in one spatial dimension (x).
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Set up expectation values in spherical coordinates (r, θ,φ)
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The form of the momentum operator in coordinate space.
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Commutation relations.
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The uncertainty principle and what it means.
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The time-dependent Schrodinger equation in 1 dimension.
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The time-independent
Schrodinger equation in 1 dimension, and how to derive it from the
time-dependent Schrodinger equation.
- The time-independent Schrodinger
equation as an eigenvalue-eigenfuction equation.
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The solutions (wavefunctions and eigenenergies) for the infinite square well.
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The energy spectrum of the 1-dim harmonic oscillator and how it depends on the
principal quantum number N.
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The ground state wavefunction of the 1-dim harmonic oscillator.
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Nodal structure of one-dimension wavefunctions.
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Scattering states: transmission and reflection coefficients (derived by
matching wfns at boundaries).
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Orthogonality of states and superposition of states.
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Expansion of a vector in an arbitrary basis; how to find the expansion
coefficients.
For
example, given an arbitrary function f(x) defined on an interval 0 < x < a, do you
know how to expand in terms of the eigenstaets of the infinite square well?
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Properties of a Hermitian matrix (operator)
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similarity and unitary transformations
Do
you know how to recognize a unitary matrix? When are you guaranteed a unitary
transformation? Do you know the difference between a unitary matrix and a
Hermitian matrix?
(over)
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Òmatrix elementsÓ of an operator in a specified basis.
- General solutions of the time-dependent
equation using the solutions of the time-independent equation.
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General statistical interpretation; ÒcollapseÓ of the wavefunction and the
probability to find particle in a measured eigenstate.
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examples in 2x2 matrices; finding eigenvalues; eigenvectors of a 2x2 matrix.
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Quantum numbers for orbital angular momentum, l and m: how to interpret them, and what
values they can have.
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Spherical harmonics.
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the Òradial Schrodinger equationÓ
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The Coulomb potential and the hydrogen atom:
Principal
quantum number N and its relation to l, n (the radial nodal quantum number)
Cartoons
of radial wfns
Dependence
of bound state energies on N.
The
Bohr radius.
Radial
wavefunctions for the hydrogen atom.
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Extra credit: Variational theory