NNSP neutron summer course, 2021 (online)
Description of intro session: Math and Physics for approx. 35 non-proficient students
Kim Lefmann, Pia J. Ray
Original document for 2019 school by KL, September 8, 2019. Edited by PJR, October 12, 2021.
Day 1 Thursday, October 14, 2021
- Introduction and Motivation (0.5 h) (blackboard + slides) (Kim)
- Intro to course
- Plan for intro days
- Scattering picture: 1 and N atoms
- Mathematical background (6 h) (short lectures + individual teaching with KhanAcad.) (Kim)
- Trigonometry
- Exponential functions
- Complex numbers
- Integrals
Day 2 Friday, October 15, 2021
- Wave Physics (3 h) (lecture + individual) (Kim)
- Definition: wave = media + disturbance
- Wave descriptors, λ, k, ω, ν, c / Demonstration with a string/spring
- Wave field sine/cosine
- Superposition, interference
- Complex wave description
- Experiment, demonstration (string)
- Problems (from Mastering Physics and Hecht)
- Fourier Transforms (2 h) (mostly lecture) (Kim, it was Johan in 2019)
- Integrals of trigonometric functions
- Finite system, Periodic function, Fourier Series as a postulate, Finite FT
- Infinite system, generalization, infinite FT as a postulate, FT of a lattice and a particle
- MATLAB demo online (did not work last time)
- Scattering Physics (1 h) (Kim)
- Neutrons and X-rays as waves
- 1-atom scattering, the complex scattered wave
- 2-atom scattering, complex description of interference, motivation to define q = ki – kf
- N-atom scattering, diffraction cross section as postulate, Fourier transform
- Examples: lattice, particle
- Experiment: laser on optical lattice
1. Motivation
Overview: Teaching plan for course
Overview: Teaching plan for math-phys intro
Reminder on neutrons, light, and X-rays, materials, experimental setup
Discussion: What is similar between these types of radiation? (wave nature, wavelength size)
Discussion: How do we measure the radiation? (particle detectors)
Discussion: How do we determine scattering angle? (collimators, slits)
Neutrons and X-rays
- Particle-wave duality; energy quanta of the two
- Same duality, same scattering Picture: 1 + atoms
Motivation: We will understand the scattering on an atomic level; therefore we need to know about waves and the corresponding math.
Material:
Slide: intro
Slide: Teaching plan
Slide: Teaching plan for M-P intro
Presentation: Kim
2. Mathematical background
Trigonometry
- Unit circle, define sine and cosine
- Rectangular and polar coordinates
- Addition formulae
- Problems about the unit circle, the Pythagorean identity, trigonometric functions:
Exponential functions
- Distinction between powers and exponentials
- 2x + 2y = 2x + y; 20 = 1
- e = 2.718...; e–x = 1/ex; shape of function
- Problems about powers and exponential growth:
Complex numbers
- i ; i2 = –1
- Complex plane; c = a + i b
- Complex conjugate; c* ; |c|2 = c c* = a2 + b2
- Complex number as polar coordinate; c = r (cos φ + i sin φ)
- Definition of complex exponential; c = r exp(i φ)
- Show that exp(i φ) exp(i χ) = exp(i (φ + χ)) - the “usual” behaviour of exponentials
- Problems about complex numbers:
Integrals
- Definition drawing, finding area, (inverse derivative)
- Example, integrate y = x
- Integrate complex functions = Integrate real part + i integrate imaginary part
- Problems about integration:
Material:
Link document to Khan Academy problems
Math 307 (The Complex Exponential Function) lecture notes
Presentation: Kim
3. Wave physics
Definition: wave = media + disturbance
- Discussion: examples (water-height, string-displacement, light-EM field, sound-pressure)
- Harmonic waves
Wave descriptors
- Drawing: y(t), y(x), y(x,t)
- Discussion: find λ, k, ω, ν, c
- Demonstration with a string/spring
Wave field sine/cosine
- Harmonic approximation
- Description of wave as cos(kx), cos(ωt)
- Drawing of A(x,t)
- Description as A = A0 cos(kx – ωt), A0 cos(kx – ωt)
- Plane waves
Superposition, interference
- Scattering from two sources, Huygens, add waves
- Standing wave
Complex wave description
- Construction to ease calculations, real part is the classical wave
- In QM, the imaginary part is “real”
- One spherical wave from scattering
- Complex description of interference
Experiment, demonstration (string or spring)
Problems: There are some suggested problems from the two books below, focus on the ones from University Physics first
Material:
Spring experiment
Scanned textbooks: Hecht (chapter 2), University Physics/Mastering Physics (chapter 15)
Selected problems from University Physics (note: not the discussion questions, but the exercises starting on page 501): 15.4, 15.8, 15.11, 15.35, 15.39, 15.76
Selected problems from Hecht: 2.1, 2.2, 2.13
Extra: Describe standing waves with complex description
still needed: solutions to problems in Hecht
Presentation: Kim
4. Fourier transformations
Integrals of trigonometric functions
- ∫02π sin(x), sin(2x), sin(x)sin(2x) etc. all = 0; graphical solution
- ∫02π sin^2(x) = π; graphical solution
Finite system, Periodic function
- Example: f(x) = A1 sin(x) + A2 sin(2x); tabulated values; find A1, A2 by integration
- Fourier Series on (0,2π); on (0, L)
- Postulate. Describe any periodic function
- Finite FT
Infinite system
- Generalization, let L → ∞
- Infinite FT equation
- Example: FT of a lattice and a particle
- MATLAB demo online (not ready)
- FFT webcam demonstration (draw some patterns and play around with it!):
- Demonstrations online / in browser:
- Problem suggestions from Arfken-Weber-Harris:
- 19.1.3, 19.2.7, 19.2.9, 20.2.1, 20.3.2, 20.3.3
Material:
Lecture notes (hand written by Johan Hellsvik)
Scanned textbook chapter: Arfken, Weber, et al, Fourier Series and Integral Transforms (chapter 19+20, plus a document with exercise solutions for those two chapters)
Handout of slides: Reciprocal Lattice
PDF of Fourier Transform problems from e-neutrons/pan-learning wiki, with hints and solutions
Presentation: Kim (was Jacob)
5. Scattering physics
1-atom scattering, the complex scattered wave
- A = b/|r – rj| exp(i k |r – rj|) exp(–i ωt)
- Example: find scattering intensity
2-atom scattering
- Derive A = b/r ∑j exp(i q·rj ) exp(–i ωt); motivation to define q = ki – kf
- Example: find scattering intensity
N-atom scattering
- Diffraction cross section as generalisation; | ∑j bj exp(i q·rj) |2
- Compare to Fourier transform of atomic positions
Examples:
- Periodic lattice; sharp features
- Spherical particle; broad features
Experiments:
- Laser on optical lattice
- Laser on hair
Material:
Slides, same as day 1
Neutron notes chap. 2
Exp: Laser, lattice, hair
Presentation: Kim