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Harmonic Oscillator and Rigid Rotator
Yao-Yuan Chuang
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Outline Classical Harmonic Oscillator
Conservation of Energy of a Classical Oscillator Harmonic Oscillator Model of a Diatomic Molecule The Harmonic Oscillator Approximation The Energy Levels of a Quantum Mechanical Harmonic Oscillator Infrared Spectra of Diatomic Molecules
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E. Bright Wilson, Jr. ( ) Studied with Linus Pauling. Wrote 3 famous books, Introduction to Q.M., Molecular Vibrations, and Introduction to Scientific research. His son Kenneth was awarded Nobel Prize in 1982.
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Molecular Motion Particle in the box is useful for understanding how translational motion in various potentials. Vibration – Harmonic Oscillator Rotation – Rigid Rotator
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Harmonic Oscillator Consider a mass m connected to a wall by a spring
stretched compressed
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Example Show the general solution can be written in the form Solution:
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Total Energy
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Harmonic Oscillator of a Diatomic Molecule
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Harmonic Oscillator of a Diatomic Molecule
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Internuclear Potential
Only lowest one or two vibrational energy levels are occupied for most molecules for ~300K harmonic Anharmonic i.e. Morse Bond Length V(x) = ½ k x2 k: force constant
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Force Constants
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Quantum Harmonic Oscillator
The Schrodinger Equation for a one-dimensional harmonic oscillator is
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Wave Functions The wave functions corresponding to the eigenvalues for a harmonic oscillator are nondegenerate
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Quantum Harmonic Oscillator
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Wave Functions
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Wave Functions
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Example Problem 18.1
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Example Problem 18.2
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Example Show that Y0 and Y1 are normalized and orthogonal to each other
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Useful Integrals
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Spherical Coordinates
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Spherical and Cartesian
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Integration
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Integration
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Example
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Solid Angle The solid enclosed by the surface that connects the origin and the area DA is called solid angle
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Example
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Molecular Motion
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Classical Rigid Rotor
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Classical Rigid Rotator
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Quantum Rigid Rotor in 2D
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Exmaple Problem 18.4
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Rigid rotor in 2D
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Rigid rotor in 2D
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Rigid Rotator in 3D
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Rigid Rotor in 3D
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Quantization of Angular Momentum
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Quantization of Angular Momentum
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Spherical Harmonic Functions
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Spherical Harmonics Y(0,0) Y(1,0) Y(1,1) Y(1,-1)
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Spherical Harmonics Y(2,1) Y(2,0) Y(2,2) Y(2,-2) Y(2,-1)
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Spherical Harmonics Y(3,2) Y(3,-2) Y(3,1) Y(3,-1) Y(3,0) Y(3,3)
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Spherical Harmonic Functions
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Spatial Quantization
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Classical Mechanics Assume a particle with mass (m) moving with velocity (v) in a circular path (radius r) with linear momentum p (=mv) v m r Conservation of angular momentum
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Orbital Angular Momentum in Quantum Mechanics and Vector Model
md=0,=90 md=+1, =65.9 md=+2, =35.3 md=-1, =114 md=-2, =144.7
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Total Angular Momentum
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Addition and Conservation of Angular Momentum in Quantum Mechanics
d1 and d2 are not coupled, each precesses about the z axis independently. d1,d2,m1,m2 are good quantum numbers, and they are separately obseravable. d d2 m d1 and d2 are coupled to form d and they precess together in phase, no longer have constant z component, d1,d2,m1,m2 are not good quantum numbers d1
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Angular Momentum Operator
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Notation Orbital angular momentum of an electron in an atom (l and ml)
Spin angular momentum of an electron (s and ms) Total angular momentum of an electron (j and mj) For more than one electron (L,ML,S,MS,J,MJ) Nucleus (I and MI) Diatomic molecules (J and MJ) Molecule (R and MR)
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Example
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Example
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Example
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Angular momentum operator
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Commutator of Angular momentum operator
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Commutator of Angular momentum operator
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Commutator of Angular momentum operator
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