The model (also known as the clock model) is a simplified statistical mechanical spin model. It is a generalization of the Ising model. Although it can be defined on an arbitrary graph, it is integrable only on one and two-dimensional lattices, in several special cases. (Wikipedia).
Model Theory - part 01 - The Setup in Classical Set Valued Model Theory
Here we give the basic setup for Model Theory. I learned this from a talk Tom Scanlon gave in 2010 at CUNY.
From playlist Model Theory
The Atom A5 The Bohr Model of the Hydrogen Atom
The Bohr model of the atom.
From playlist Physics - The Atom
The Atom A3 The Bohr Model of the Hydrogen Atom
The Bohr model of the atom.
From playlist Physics - The Atom
What are the W and Z particles?
Subscribe to our YouTube Channel for all the latest from World Science U. Visit our Website: http://www.worldscienceu.com/ Like us on Facebook: https://www.facebook.com/worldscienceu Follow us on Twitter: https://twitter.com/worldscienceu
From playlist Science Unplugged: Particle Physics
The Atom A4 The Bohr Model of the Hydrogen Atom
The Bohr model of the atom.
From playlist Physics - The Atom
I Hope the Standard Model Isn't Wrong
It seems like a good time to dig this one up and load it in light of the muon g-2 experiment. I think I made it for an online class the last time the Standard Model was in question..
From playlist Off Topic
Set Theory (Part 2): ZFC Axioms
Please feel free to leave comments/questions on the video and practice problems below! In this video, I introduce some common axioms in set theory using the Zermelo-Fraenkel w/ choice (ZFC) system. Five out of nine ZFC axioms are covered and the remaining four will be introduced in their
From playlist Set Theory by Mathoma
B28 An example problem of a linear model
Here is our first real-world linear problem.
From playlist Differential Equations
Graph of x^2 + 6xb + 5b^2 as b varies
From playlist 3d graphs
Hao Shen (Wisconsin) -- Stochastic quantization, large N, and mean field limit
We study "large N problems” in quantum field theory using SPDE methods via stochastic quantization. In the SPDE setting this is formulated as mean field problems. We will consider the vector Phi^4 model (i.e. linear sigma model), whose stochastic quantization is a system of N coupled dynam
From playlist Columbia Probability Seminar
Stanford CS229: Machine Learning | Summer 2019 | Lecture 17 - Factor Analysis & ELBO
For more information about Stanford’s Artificial Intelligence professional and graduate programs, visit: https://stanford.io/3E4MouM Anand Avati Computer Science, PhD To follow along with the course schedule and syllabus, visit: http://cs229.stanford.edu/syllabus-summer2019.html
From playlist Stanford CS229: Machine Learning Course | Summer 2019 (Anand Avati)
Sophie Morel - 2/3 Shimura Varieties
Depending on your point of view, Shimura varieties are a special kind of locally symmetric spaces, a generalization of moduli spaces of abelian schemes with extra structures, or the imperfect characteristic 0 version of moduli spaces of shtuka. They play an important role in the Langlands
From playlist 2022 Summer School on the Langlands program
Lecture 15 - EM Algorithm & Factor Analysis | Stanford CS229: Machine Learning Andrew Ng -Autumn2018
For more information about Stanford’s Artificial Intelligence professional and graduate programs, visit: https://stanford.io/3jsY9n7 Andrew Ng Adjunct Professor of Computer Science https://www.andrewng.org/ To follow along with the course schedule and syllabus, visit: http://cs229.sta
From playlist Stanford CS229: Machine Learning Full Course taught by Andrew Ng | Autumn 2018
Hugo Duminil-Copin - Introduction to parafermionic observables
In the early eighties, the physicists Belavin, Polyakov and Zamolodchikov postulated the conformal invariance of critical planar statistical models. This prediction enabled physicists to use Conformal Field Theory in order to formulate many conjectures on these models. From a mathematical
From playlist 8ème Séminaire Itzykson : "Les observables parafermioniques et la physique statistique en 2D"
Phase transitions in hard-core systems by Deepak Dhar ( Lecture - 4 )
PROGRAM BANGALORE SCHOOL ON STATISTICAL PHYSICS - X ORGANIZERS : Abhishek Dhar and Sanjib Sabhapandit DATE : 17 June 2019 to 28 June 2019 VENUE : Ramanujan Lecture Hall, ICTS Bangalore This advanced level school is the tenth in the series. This is a pedagogical school, aimed at bridgin
From playlist Bangalore School on Statistical Physics - X (2019)
Sepideh Mirrahimi : Integro-differential models of evolutionary adaptation in changing...- lecture 1
What would be the impact of an environment change on the persistence and the genetic/phenotypic distribution of a population? We present some integro-differential models describing the evolutionary adaptation of asexual phenotypically structured populations subject to mutation and selectio
From playlist CEMRACS 2022
Said Hamoun (2/23/23): On the rational topological complexity of coformal elliptic spaces
We establish some upper and lower bounds of the rational topological complexity for certain classes of elliptic spaces. Our techniques permit us in particular to show that the rational topological complexity coincides with the dimension of the rational homotopy for some special families of
From playlist Topological Complexity Seminar
Regression Analysis by Dr. Soumen Maity,Department of Mathematics,IIT Kharagpur.For more details on NPTEL visit http://nptel.ac.in
From playlist IIT Kharagpur: Regression Analysis | CosmoLearning.org Mathematics
The model of the atom - Bounded by the light
Reworking of the Weekend's blinded by the light
From playlist Level 2 NCEA Physics
Nick Barton & Alison Etheridge: Establishment in a new habitat under the infinitesimal model
Abstract: Maladapted individuals can only colonise a new habitat if they can evolve a positive growth rate fast enough to avoid extinction - evolutionary rescue. We use the infinitesimal model to follow the evolution of the growth rate, and find that the probability that a single migrant c
From playlist Probability and Statistics