Quantum mechanics unit 1

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321 Quantum Mechanics Unit 1 Quantum mechanics unit 1 Foundations of QM Photoelectric effect, Compton effect, Matter waves The uncertainty principle The Schrödinger eqn. in 1D Square well potentials and 1D tunnelling The harmonic oscillator

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Quantum mechanics unit 1. Foundations of QM Photoelectric effect, Compton effect, Matter waves The uncertainty principle The Schr ö dinger eqn. in 1D Square well potentials and 1D tunnelling The harmonic oscillator. Last time. Photons Photoelectric effect Compton effect - PowerPoint PPT Presentation

Transcript of Quantum mechanics unit 1

Page 1: Quantum mechanics unit 1

321 Quantum Mechanics Unit 1

Quantum mechanics unit 1• Foundations of QM• Photoelectric effect, Compton effect, Matter waves

• The uncertainty principle

• The Schrödinger eqn. in 1D

• Square well potentials and 1D tunnelling

• The harmonic oscillator

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Last time• Photons• Photoelectric effect• Compton effect

• Matter waves• de Broglie relations• Electron diffraction• Waves related to probability

www.le.ac.uk/physics -> people -> Mervyn Roy

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321 Quantum Mechanics Unit 1

Heisenberg uncertainty principle• Fundamental property of quantum systems• Course 3210 Unit 3, Rae Chapter 4

• Inherent uncertainties in predictions – or average spread of a set of repeated measurements

∆ 𝑥 ∆𝑝𝑥≥12ℏ

∆𝐸 ∆ 𝑡≥ 12 ℏ

Heisenberg - formulation of QM 1927, Nobel prize 1932

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Example• The position of a proton is known to within 10-11 m.

Calculate the subsequent uncertainty in its position 1 second later.

km

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321 Quantum Mechanics Unit 1

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321 Quantum Mechanics Unit 1

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321 Quantum Mechanics Unit 1

Example• An atom in an excited state emits a photon of

characteristic frequency, n. The average time between excitation and emission is 10-8 s. Calculate the irreducible linewidth of the transition.

Hz

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Schrödinger equation

• Developed by induction

• Tested against experiment for over 80 years

• is the wavefunction. This is essentially complex – cannot be identified with any one physical property of the system

Schrödinger - formulation of QM 1925-26, Nobel prize 1933

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Schrödinger equation • related to probability

dx

• Wavefunction must be normalised

= 1

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Time independent Schrödinger equation

eigenfunction

eigenvalue

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Constraints• The wavefunction and its first derivative must be:

• Single valued

• Finite

• Continuous