- Department: Physics
- Module co-ordinator: Dr. Yvette Hancock
- Credit value: 10 credits
- Credit level: H
- Academic year of delivery: 2022-23
- See module specification for other years: 2021-22
Pre-requisite modules
- None
Co-requisite modules
- None
Prohibited combinations
Occurrence | Teaching period |
---|---|
A | Autumn Term 2022-23 |
This module aims to:
introduce quantum mechanical commutators and their significance for the compatibility of measurements.
introduce the quantum mechanical treatment of angular momentum
demonstrate co-ordinate transformation from Cartesian to spherical polar co-ordinates and apply this to the angular momentum operators and time-independent Schrodinger equation find solutions of the time-independent Schrodinger equation for a spherically symmetrical potential
solve the time-independent Schroedinger equation for the Hydrogen atom (full analytical solution) and extend quantum mechanics to incorporate spin
introduce matrix mechanics, with particular application to spin-spin operators, Pauli spin matrices
discuss the theory of measurement with the Stern-Gerlach measurement of spin as an example
develop approximate methods for solving the Schrodinger equation when no analytic solutions exist, such as time-independent perturbation theory.
Understand the physical significance of commutators in terms of compatibility of measurements
Perform simple commutator algebra, in order to obtain commutators for operators expressible in terms of the position and momentum operators.
Derive operators for the angular momentum components L_x, L_y, L_z, and for L^2, in terms of position and momentum operators in Cartesian coordinates
Understand how the angular momentum operators are transformed from Cartesian into spherical polar coordinates
Derive the operators for L_z and L^2 in spherical polar co-ordinates
Derive and interpret the eigenvalues and eigenvectors of the operators for angular momentum, L_z, and L^2 in terms of possible measurement results.
Explain the use of the central force theorem for a spherically symmetric potential within the context of the time-independent Schrodinger equation written in spherical polar co-ordinates and applied to hydrogen-like atoms
Discuss the relationship between the operators L_z, L^2 and the above Hamiltonian for a hydrogen-like atom system
Apply the above to solving the full analytical eigensolution for the case of the Hydrogen atom
Reproduce and interpret a labelled diagram showing the energy levels and angular momentum states of the hydrogen atom
Provide a physical interpretation of the quantum numbers n, l and m_l and be able to sketch the wavefunction solutions of the hydrogen atom for a given n, l and m_l )
Understand the matrix formalism of quantum mechanics and apply this to the case of spin
Apply the Pauli spin matrices to find the eigenvalues and eigenvectors of spin operators
Interpret generalised Stern-Gerlach experiments in terms of eigenvector superposition, illustrating the theory of measurement.
Derive the first and second order energy corrections in non-degenerate perturbation theory, and first order eigenvector correction and apply these formulae to simple problems, e.g. anharmonic oscillators
Syllabus
Task | Length | % of module mark |
---|---|---|
Essay/coursework (NS) Quantum Mechanics II Assignment 1 |
N/A | 40 |
Essay/coursework (NS) Quantum Mechanics II Assignment 2 |
N/A | 60 |
Non-reassessable
Task | Length | % of module mark |
---|---|---|
Essay/coursework (NS) Quantum Mechanics II Assignment 1 |
N/A | 40 |
Essay/coursework (NS) Quantum Mechanics II Assignment 2 |
N/A | 60 |
Our policy on how you receive feedback for formative and summative purposes is contained in our Department Handbook.
A I M Rae: Quantum mechanics (McGraw-Hill) ***
R C Greenhow: Introductory quantum mechanics (Taylor & Francis/IoP Publishing) **
B H Bransden and C J Joachain: Introduction to quantum mechanics (Prentice Hall)*