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Welcome to grad school.
F: We will not be meeting today. Recommended alternative activities: discover where the botanical garden is, find the shelves in Orbach library that carry books in your subdiscipline of physics, watch the freshmen scramble to find their first lectures of college.
See Week 1-2 assignments.
See our collection of dimensional analysis articles on our references page
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.
Simon Collison's "Maturity and the Weight of Learning" is a brilliant article in The Manual, a craft journal for web designers. It was published in the early 2010s. If you replace 'web design' with physics and references to tools with gestures to artificial intelligence, then the piece is directly applicable to our profession.
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How (and why) do physicists use index notation for everything? How do we solve the ever-present eigenvalue problem in linear algebra?
Mon 9/28: Logistics. How is math ifferent from physics? The Green's functoin problem.
Mon,9/28, discussion section: Dimensional analysis review.
Wed 9/30: Index notation. Tensors. Funny vector spaces.
Fri 10/2: Inner products and metric spaces, hermiticity. How tensors transform under a transformation matrix T: one factor of T for each upper index, one factor of T-inverse for each lower index. Two special classes of matrices: rotations (isometries) and Hermitian matrices.
See Week 1-2 Assignments on the HW page for homework and submission links.
This week you have to submit a brief survey, a video introduction, and your first short homework (all due Wed)
See the linear algebra / tensor analysis / moment of inertia sections of our references page.
Some background on the UCR Burros, "The Wild History of UCR’s Infamous Burros," by David Danelski for UCR Magazine.
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What is the infinite-dimensional limit of ordinary linear algebra? And why should we think about the "vector space" of functions as such a space?
"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 10/5: Histogram space, inner products, boundary conditions, differential operators. Lecture notes: from histograms to function space.
Mon 10/5 (Dis): Fourier Basis
Wed 10/7: The continuum limit: function space. Lecture notes.
Fri 10/9: The ubiquitous harmonic oscillator. What could go wrong? Topics: reminder of Fourier transform conventions, what is a Green's function, the Green's function equation, solving for the harmonic oscillator Green's function ... and getting stuck when we have a singular integral. Lecture notes.
See assignments page. Due this Friday: the first long homework.
For more on the continuum limit of "histogram space," see the continuum limit section of our references.
More formalism
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.
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How is ℂ different from ℝ2? In what ways is our description of nature "intrinsically" complex? How is calculus on the complex plane different from multivariable calculus on two-dimensional real space?
Mon 10/12: The complex plane, complex functions as maps. Notes.
Mon 10/12: student presentation of long homework problems, any discussion points. See assignments page for presenters.
Wed 10/16: Branch cuts and Riemann sheets.
Fri 10/17: Integration of analytic and meromorphic functions: the residue theorem. Notes.
Most of the material this week is a review of topics you may have seen as an undergrad, but framed with an eye on how we intend to use them. Please refer to your favorite mathematical physics textbook for additional resources.
We mentioned conformal mapping and its applications to the early aerospace industry. A simple example of a conformal map that takes the circle to an approximate airplane wing cross section is the Joukowski transform. You can find a bit about it on this old NASA page.
He's an example of someone working through a conformal mapping problem. I find the act of working through it to be especially insightful.
Lectures and Problems : A Gift to Young Mathematicians by V. I. Arnold, Dmitry Fuchs, Mark Saul. A collection of essays; see specifically the chapter "Geometry of Complex Numbers, Quaternions, and Spins"
"Physics of the Analytic S-Matrix" by Sebastian Mizera (arxiv:2306.05395) is an excellent set of lecture notes on the analytic properties of scattering. The first section covers some of the key ideas of our course.
"A brief Introduction to Dispersion Relations and Analyticity" by Zwicky (arxiv:1610.06090) is an older set of lecture notes on the analytic properties of quantum field theory.
If you want to see why I have been spending time thinking about the analytic properties of quantum mechanics, see "Undecay" by Megias, Perez-Victoria, and Quiros (arxiv:2310.16593). It is a study of the propagator (Green's function) of a certain class of theories called unparticles (alternatively, non-compact extra dimensional theories or near-conformal strongly coupled theories).
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How may we use the power of complex analysis (the residue theorem) to calculate real integrals that show up in physics?
Mon 10/19: Using the residue theorem for real integrals. Notes.
Wed 10/21: Kramers-Kronig relations. The Green's function for the harmonic oscillator. The choice of contour depends on the sign of the exponential, which itself came from the eigenbasis of the harmonic oscillator differential equation. [Notes]
Fri 10/23: Making sense of the choice of sign for iε. The damped harmonic oscillator. [Notes]
See the Complex Analysis references on our references page.
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Let's solve the Green's function for the one system that really matters. (Why is this the one?)
Mon 10/26: Pole pushing for poor physicists.
Kramers-Kronig relations, principal value, causality, an example. Notes.
Wed 10/28: Damping.
Kramers-Kronig, the 'general solution' to the Green's function distribution (free + particular solution), seeing how causality imposes a set of 'boundary conditions' on the free solutions that are equivalent to the "pole pushing" we did earlier. Notes. (Notes contain a derivation of some of the distribution identities that we used. These mainly follow Appel's ch. 15.2 and the earlier chapters it cites.)
Fri 10/30: The heat equation and the Schrodinger equation. [Notes]
See Ch. 15.2 of Appel's Mathematics for Physics & Physicists for a discussion of using the principal value to determine the Green's function of the "ε=0" harmonic oscillator. Appel points out as a distribution, this latter case is not part of a convolution algebra.
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.
For those in particle physics, Scott Willenbrock discusses the role of the complex pole in the unstable particle propagator in "A Brief History of Mass"(arXiv:2503.07866).
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What changes when we go from time to spacetime?
Mon 11/2: Hacking together the wave equation. The continuum limit of a discrete series of harmonic oscillators. The material follows Fly By Night Physics by Zee. Notes.
Sketch of wave equation Green's function. Extended notes.
Wed 11/3: Solving the wave equation in 2 and 3 dimensions.. Notes. (We didn't end up taking about Huygen's principle.)
Fri 11/6: Dimensional reduction.
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)
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Why are all of our favorite quantities fields that obey wave-like equations?
Mon 11/9: [notes] A bird's eye view of field theory..
Wed 11/11: No class today, federal holiday: Veteran's Day.
Fri 11/14: Gaussian integrals, field theory, a hint of perturbation theory.
Your favorite probability textbook. If you do not have one, it should be Probability Theory: The Logic of Science by Jaynes.
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Your graduate coursework will make you an expert at taking a theory, say Maxwell's electromagnetism, and calculating the probability of some outcome: P( experiment | theory ). How, then, do we begin to answer the question that we actually care about: what is the probability of a given theory (model) given some experimental observations?
Mon 11/16: [notes] Basics of probability. Richard Gott's experiment. Bayes' theorem.
Wed 11/18: [notes] Likelihood.
Fri 11/21: [notes] Gaussian = free theory, Feynman diagrams, towards interacting theories.
Your favorite probability textbook. If you do not have one, it should be Probability Theory: The Logic of Science by Jaynes.
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Perturbations about the Gaussian: what do we do when the universe is not quadratic?
Mon 11/23: Interacting theories. [notes]
Wed 11/25: Introduction: mass renormalization.
Fri: 11/28: no class, Thanksgiving
"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.
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Mon 11/30: Spherical Harmonics and the CMB
Wed 12/2: Correlation functions of the CMB
Fri: 12/4: TBD. Possibilities include writing and speaking as a physicist, more on divergences in field theory
The Los Alamos Primer on Particle Physics (1984) is contains some of the most fantastic magazine-length public science writing of its era. (Not to be confused with what is known as the Los Alamos Primer.) If you have followed week 0 (dimensional analysis) and week 10 (introduction to renormalization) then I expect you will really appreciate Geoff West's contribution, "Scale & Dimension: from animals to quarks." It is an excellent thing to read when you're traveling somewhere over winter break.
There are many well written explanations of renormalization from a modern perspective. Here's one by João Melo from not too long ago. arxiv:1909.11099
For an intuitive picture of renormalization from 1969, see Charles Kaufman's "An Illustration from Classical Physics of Renormalization Mathematics" Am. J. Phys. 37, 560–561 (1969) https://doi.org/10.1119/1.1975679
Unlike other foundational ideas in theoretical physics, our understanding of renormalization is remarkably recent. Here's a brief history by Kerson Huang in memory of Ken Wilson. arxiv:1310.5533.
"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.
"Everything's a Mass on a Spring," ThatBlackChemist, Instagrasm, Dec 3, 2025. (courtesy of Chanda Prescod-Weinstein) One thing I'd like you to take away from our class: if (almost) everything is a mass on a spring, then (almost) all of the calculations we do are Green's functions.
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