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CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators
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CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

Dec 19, 2015

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Page 1: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

CHEM 515Spectroscopy

Lecture # 8

Quantum Mechanical Solution for Harmonic Oscillators

Page 2: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

2

Harmonic Oscillator Model

This kind of motion is called simple harmonic motion and the system a simple harmonic oscillator.

Page 3: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

3

Potential Energy for Harmonic Oscillator

• The oscillator has total energy equal to kinetic energy + potential energy.

• when the oscillator is at A, it is momentarily at rest, so has no kinetic energy

U=0

Page 4: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

4

Energy Levels for a Quantum Mechanical Harmonic Oscillator

Page 5: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Harmonic Oscillator Potential Curves

Morse potential

Harmonic oscillator

Page 6: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Morse Potential

It is a better approximation for the vibrational structure of the molecule than the quantum harmonic oscillator because it explicitly includes the effects of bond breaking, such as the existence of unbound states. It also accounts for the anharmonicity of real bonds.

Page 7: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Morse Potential

The dissociation energy De is larger than the true

energy required for dissociation D0 due to

the zero point energy of the lowest (v = 0) vibrational level.

Page 8: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Vibrational Wave Functions (ψvib)

Page 9: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Vibrational Wave Functions (ψvib)

Page 10: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Vibrational Wave Functions (ψvib)

Page 11: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Probability Distributions for the Quantum Oscillator (ψ2

vib)

The square of the wave function gives the probability of finding the oscillator at a particular value of x.

Page 12: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Probability Distributions for the Quantum Oscillator (ψ2

vib)

there is a finite probability that the oscillator will be found outside the "potential well" indicated by the smooth curve. This is forbidden in classical physics.

Page 13: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Vibrational-Rotational Energy Levels

Page 14: CHEM 515 Spectroscopy Lecture # 8 Quantum Mechanical Solution for Harmonic Oscillators.

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Various Types of Infrared Transition