Welcome to grad school.
Fri: Course logistics. Review of dimensional analysis, basics of linear algebra.
We talked about how math and physics are different. Some of the ideas that came up were formalism, notion of truth, a multiplicity of descriptions (and when two physical theories are equivalent versus effectively equivalent), whether one is a tool to the other.
See the references below that discuss whether dx and Δx are mathematically equivalent.
Video Introduction: please record a short video to introduce yourself to the class. Due next Wednesday, Oct. 1. Guidelines: approximately 5 minutes, share your name, research interests, where you are from (both university and hometown), and anything else you would like to share (hobbies, recommendations, aspirations, etc.).
Submission link: Introductory Video
You may use any recording device (laptop, phone), please show your face to help us get to know each other. You must upload in a way that is accessible to the other members of the class (e.g. share on UCR's Google Drive and whitelist @ucr accounts).
Link to Flip Tanedo's video introduction
Pre-Class Survey, please complete by Wednesday, Sept. 1
Submission link: Pre-Class Survey
Short Homework 1: due Wednesday, Oct. 1.
Submission link: Short HW 1
Please note that while you may edit your responses in the form, the pdf you upload cannot be replaced. Please double check your file before you upload for this and all of your uploaded pdfs.
Long Homework 1: due Friday, Oct. 10
Submission link: Long HW 1
Current lecture notes draft: Sept 24; over the first two weeks of this course we are quickly reviewing the first part of the notes (linear algebra). Most of the material will be familiar to you, but I would like us to get used to the notation.
The lecture notes contain the main narrative of the course. Each week we provide suggested reading for complementary perspectives and deeper dives into the material. You are strongly encouraged to explore the topics as they relate to your interests and needs.
See our collection of dimensional analysis articles on our references page
Every year we start this class by asking how physics is different from mathematics. One of the topics that regularly comes up is that physicists treat the infinitesimal dx as a very-small-but-finite difference Δx. I do this often. The following references dig into when this is valid:
Ely, R. "Teaching calculus with infinitesimals and differentials." ZDM Mathematics Education 53, 591–604 (2021). https://doi.org/10.1007/s11858-020-01194-2
"Extending the Algebraic Manipulability of Differentials," Jonathan Bartlett, Asatur Zh. Khurshudyan. arXiv:1801.09553
Further discussion on physics and mathematics:
"Why Physics Is Unreasonably Good at Creating New Math," Ananyo Bhattacharya in Nautilus
"The importance of stupidity in scientific research" by Marting Schwartz in Journal of the Cell and an informal follow up, "The centrality of stupidity in mathematics" on the Math for Love blog.
[ ^ top of the page ]
Finite dimensional linear algebra.
Mon 9/30:
Wed 10/1:
Fri 10/3:
Video Introduction: please record a short (~5min) video to introduce yourself to the class. Due Wednesday 10/4.
Submission link
Recording tips.
Link to Flip Tanedo's video introduction
Pre-Class Survey, due Wednesday 10/1
Short Homework 1: due Wednesday 10/1
Please note that while you may edit your responses in the form, the pdf you upload cannot be replaced. Please double check your file before you upload for this and all of your uploaded pdfs.
Upcoming Assignments: Please look over the long homework and ask questions in class this week.
Long Homework 1: due Friday 10/10. [Submission link]
Explainer Video 1: due Friday 10/17. More instructions below.
The lecture notes contain the main narrative of the course. Each week we provide suggested reading for complementary perspectives and deeper dives into the material. You are strongly encouraged to explore the topics as they relate to your interests and needs.
"Introduction to Tensor Calculus," Kees Dullemond & Kasper Peeters (booklet) 2010. This is a reasonable introduction to the "indexology" that we use in physics. The booklet is much more rigorous than we will be. It may help motivate the types of rules that we will build into our index notation. If you enjoy this reference, you can find more in the first few chapters of most general relativity textbooks, for example Sean Carrol's Spacetime and Geometry.
"Tensors: A guide for undergraduate students," Franco Battaglia, American Journal of Physics 81, 498 (2013); (accessible through UCR VPN)This is an excellent and readable introduction to to tensors. In the last half of the article (beyond our scope) one starts to get a taste of how linear algebra is a local approximation to calculus on curved spaces.
There's a fantastic history of vectors in mathematics and physics, Vector: a surprising story of space, time, and mathematical transformation by Robyn Arianrhod. It's the kind of history that a physicist would love, connecting some familiar names with a story of the development of an idea that we tend to ignore in our education.
One of my favorite examples of a vector space is color space. The three types of cone cells in our eyes are sensitive to different pieces of the visual spectrum. They define a basis for a three-dimensional vector space corresponding to neurological responses to the electromagnetic spectrum. Other animals can have more types of cone cells, in which case their color spaces are higher dimensional. Here are a couple of nice videos discussing the concept. There are references to more academic papers in our course notes.
"RGB to XYZ: The Science and History of Color" by John Austin" at the Strange Loop Conference, 2019
"Color Spaces: Explained from the Ground Up" via- Video Tech Explained
We posed the question of why the moment of inertia tensor is a tensor and not a matrix. Many textbooks get this wrong. One way to see this is that the moment of inertia tensor properly has two lower indices. It may help to write the cross prodcut with respect to the Levi-Civita tensor in 3D. Some references:
This answer on physics.stackexchange. The presentation is a little technical. It is similar to what one finds in V.I. Arnold's Mathematical Methods of Classical Mechanics in the section on rigid body motion.
A really great reference is this article on bivectors: "Teaching Rotational Physics with Bivectors," Steuard Jensen, Jack Poling. (arXiv: 2207.03560) The bivector construction may seem a little unfamiliar, but they do a good job of introducing it. In 3D, the bivector is a nicer way to represent the cross product. However, bivectors (and their cousins, k-forms) generalize to higher dimensions. The appendix describes the moment of inertia tensor in higher dimensions.
Along the lines of the above, here's a more systematic introduction to geometric algebra, including a nice discussion of the moment of inertia tensor: "Unifying the inertia and Riemann curvature tensors through geometric algebra" by M.. Berrondo, J. Greenwald, and C. Verhaaren (Am. J. Phys. 80, 905–912).
If you want to really dive deeper into this field, check out "Spacetime algebra as a powerful tool for electromagnetism" (arXiv:1411.5002) by Dressel, Bliokh, and Nori.
A nice introduction to the ideas of geometric algebra on YouTube: "A Swift Introduction to Geometric Algebra."
A slightly more sophisticated set of videos: "QED Prerequisites Geometric Algebra: Introduction and Motivation"
A YouTube explainer on rigid body dynamics using geometric algebra.
[ ^ top of the page ]
"Infinite dimensional linear algebra" as the linear vector space of functions. Differential operators as linear operators. Complex spaces. And finally, the Green's function.
Mon 10/6:
Wed 10/8:
Fri 10/10:
Long Homework 1: due Friday 10/10 [Submission link]
Upcoming: Starting week 3 we begin our full cadence of assignments. Something is due every Wed and Fri.
Short Homework 2: due Wednesday 10/15. [Submission link]
Explainer Video 1: due Friday 10/17
More instructions below.
Assignments are on our internal sheet
Peer Review 1: due Wednesday 10/22 [submission link]
Assignments are on our internal sheet
Long Homework 2: due Friday 10/24. [Submission link]
Please refer to Part I of our course notes.
Section 4.1 of Stone & Goldbart distinguishes between formal and concrete differential operators. For our purposes, a formal differential operator is what one would typically call "a differential operator," examples include the d'Alembertian or the Laplacian. A concrete differential operator comes with a specification of the domain and the boundary conditions.
Chapter 4.1-4.8 of Byron & Fuller is a nice summary of finite dimensional vector spaces. Chapter 5 introduces function spaces.
Section 4.1 of the Manchester notes.
In our lectures we discuss why there there are really only a few differential operators that always keep showing up in physics. Part of this has to do with the symmetries that our physical models satisfy, and part of it has to do with the idea that terms with more derivatives are typically small in the limit where our model is valid. This falls under the idea of an "effective theory." This year there's a virtual seminar series about effective field theories (all talks are recorded) that I recommend for those who are curious.
Extra: "Dimensional Analysis in Field Theory," Stevenson, Annals of Physics 132, 383 (1981). A non-trivial example of dimensional analysis.
Extra: for more of a discussion about tangent spaces versus base spaces, Arnold's Mathematical Methods of Classical Mechanics is a classic. You can also see Collinucci and Wijn's lectures at the Modave Summer School in 2006 for a brief introduction to the mathematics of fiber bundles.
[ ^ top of the page ]
"Infinite dimensional linear algebra" as the linear vector space of functions. Differential operators as linear operators. Complex spaces. And finally, the Green's function.
Mon 10/13:
Wed 10/15:
Fri 10/17:
Please go over the long homework this week, even though it is due next week. Let us use class time to discuss the homework.
Short Homework 2: due Wednesday 10/15. [Submission link]
Explainer Video 1: due Friday 10/17
You have been assigned one problem from Long Homework 1 to present a 5 minute explainer video.
Please find your problem on the internal sheet
Due next week
Peer Review 1: due Wednesday 10/22 [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
Long Homework 2: due Friday 10/24. [Submission link]
Please refer to Part I of our course notes.
Section 4.1 of Stone & Goldbart distinguishes between formal and concrete differential operators. For our purposes, a formal differential operator is what one would typically call "a differential operator," examples include the d'Alembertian or the Laplacian. A concrete differential operator comes with a specification of the domain and the boundary conditions.
Chapter 4.1-4.8 of Byron & Fuller is a nice summary of finite dimensional vector spaces. Chapter 5 introduces function spaces.
Section 4.1 of the Manchester notes.
In our lectures we discuss why there there are really only a few differential operators that always keep showing up in physics. Part of this has to do with the symmetries that our physical models satisfy, and part of it has to do with the idea that terms with more derivatives are typically small in the limit where our model is valid. This falls under the idea of an "effective theory." This year there's a virtual seminar series about effective field theories (all talks are recorded) that I recommend for those who are curious.
Extra: "Dimensional Analysis in Field Theory," Stevenson, Annals of Physics 132, 383 (1981). A non-trivial example of dimensional analysis.
Extra: for more of a discussion about tangent spaces versus base spaces, Arnold's Mathematical Methods of Classical Mechanics is a classic. You can also see Collinucci and Wijn's lectures at the Modave Summer School in 2006 for a brief introduction to the mathematics of fiber bundles.
[ ^ top of the page ]
"Infinite dimensional linear algebra" as the linear vector space of functions. Differential operators as linear operators. Complex spaces. And finally, the Green's function.
Mon 10/20:
Wed 10/22,
Fri 10/24:
Long Homework 2: due Friday 10/24. [Submission link]
Peer Review 1: due Wednesday 10/22. [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
Upcoming
Short Homework 3: due Wednesday 10/29. [submission link]
Explainer Video 2: due Friday 10/31. [submission link]
Assignments are on our internal sheet
"Guide to Cultivating Complex Analysis" by Jiří Lebl seems to be a nice formal discussion of complex analysis.
Visual Complex Analysis by Needham is nice textbook that does not skimp on images. The approach is a little idiosyncratic.
Your favorite undergraduate math methods course is a good starting point. I am partial to the textbook by Boas.
What are Riemann sheets good for?
"Resonances and poles in the second Riemann sheet," by Thomas Wolkanowski. A MSc thesis on the significance of the second Riemann sheet in quantum field theory.
"Scattering amplitudes and contour deformations," by Gernot Eichmann, Pedro Duarte, M. T. Peña, Alfred Stadler
[ ^ top of the page ]
Let's solve the Green's function for the one system that really matters. (Why is this the one?)
Mon 10/27:
Wed 10/29:
Fri 10/31:
Short Homework 3: due Wednesday 10/29. [submission link]
Explainer Video 2: due Friday 10/31 [submission link]
Assignments are on our internal sheet
Upcoming: please review the long homework this week so we may discuss it in class.
Peer Review 2: due Wednesday 11/5 [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
Long Homework 3: due Friday 11/7. [submission link]
There are some classic textbooks for this: Byron and Fuller, Butkov, Felder and Felder, etc. Pick your favorite.
Chapter 9 of Penrose's Road to Reality is not directly applicable, but offers some nice connections. Some of the extra credit problems draw from this source.
"Scattering amplitudes and contour deformations," by Gernot Eichmann, Pedro Duarte, M. T. Peña, Alfred Stadler
[ ^ top of the page ]
Let's solve the Green's function for the one system that really matters. (Why is this the one?)
Mon 11/3:
Mon 11/3 (discussion hour):
Wed 11/5:
Fri 11/7: no class
Peer Review 2: due Wednesday 11/5. [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
Long Homework 3: due Friday 11/7. [submission link]
Upcoming:
Explainer Video 3: due Friday 11/14 [submission link]
Assignments are on our internal sheet
Short Homework 4: due Wednesday 11/12 [submission link]
Fly By Night Physics, Tony Zee: See Appendix G
Dimensional reduction is discussed in the textbook by Appel.
"Wakes and waves in N dimensions," Harry Soodak; Martin S. Tiersten, Am. J. Phys. 61, 395–401 (1993)
[ ^ top of the page ]
This week we treat the wave equation as the limit of a continuum of coupled harmonic oscillators.
Mon 11/10:
Wed 11/12:
Fri 11/14:
Short Homework 4: due Wed 11/12 [submission link]
Explainer Video 3: due Friday 11/14 [submission link]
Assignments are on our internal sheet
Upcoming:
Peer Review 3: due Wed, 11/19 [submission link]
Assignments are on our internal sheet
Long Homework 4: due Friday 11/21 [submission link]
Your favorite probability textbook. If you do not have one, it should be Probability Theory: The Logic of Science by Jaynes.
[ ^ top of the page ]
A brief introduction to perturbative field theory. Theories with quadratic actions have linear equations of motion for which the propagation of information is described by linear operators. In th real world, there are non-quadratic "interaction" terms. In the worst case scenario, you must rely on simulations to study these theories. However, when the theory is perturbatively close to a Gaussian fiext point, you may employ a Feynman diagram expansion.
Mon 11/17:
Wed 11/19:
Fri 11/21:
Peer Review 3: due Wed 11/19 [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
Long Homework 4: due Friday 11/21. [submission link]
Upcoming
Explainer Video 4: due Friday 11/28 [Mon Dec 1 is ok] [submission link]
Last 2 weeks' assignments are to be determined.
Your favorite probability textbook. If you do not have one, it should be Probability Theory: The Logic of Science by Jaynes.
"Feynman Diagrams," Weinzierl arXiv:2501.08354
[ ^ top of the page ]
Perturbations about the Gaussian: what to do when the universe is not quadratic.
Mon 11/24:
Mon 11/24 (discussion hour):
Wed 11/28: no class
Fri: 11/28: no class, Thanksgiving
Explainer Video 4: due Friday 11/28 [Mon Dec 1 is ok] [submission link]
Assignments are on our internal sheet
Last 2 weeks' assignments are TBD
Peer Review 4: due Wed 12/3 [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
"Feynman Diagrams," Weinzierl arXiv:2501.08354
Your favorite probability textbook. If you do not have one, it should be Probability Theory: The Logic of Science by Jaynes.
"What is Entropy?" arxiv:2409.09232 by John Baez.
"Statistical Physics," Jaynes 1962 Brandeis Lectures on Theoretical Physics, Vol 3
"Entropy, Cross-Entropy, & KL-Divergence," Aurélien Géron.
[ ^ top of the page ]
A further investigation of analyticity in physics.
Mon 10/1:
Wed 10/3:
Fri 10/5:
Last 2 weeks' assignments are TBD
Peer Review 4: due Wed 12/3 [submission link]
Please fill out the same form once for each of the three peers you are reviewing
Assignments are on our internal sheet
"Physics of the Analytic S-Matrix" (arXiv: 2306.05395) by Sebastian Mizera. This is an excellent summary of topics in this course and a peek at how it applies to quantum mechanics and quantum field theory.
[ ^ top of the page ]