\documentclass{ximera} \usepackage{tikz} \usepackage{color} \usepackage{amsmath,amssymb,amsfonts} \usepackage{graphicx} %\usepackage{helvet} %\renewcommand{\familydefault}{\sfdefault} \author{Jeffrey Kuan} \input{../preamble} %% Loads the graphics path \title{Matrix Product Ansatz} \license{CC: 0} \begin{document} \begin{abstract} I like Taylor Swift. \end{abstract} \maketitle %\part{Introduction} %\chapterstyle % \activity{basics/basicWorksheet} % \sectionstyle % \activity{basics/exercises/someExercises} % \chapterstyle % \activity{basics/graphicsInteractives} Accessibility statement: I will eventually create a WCAG2.1AA compliant version of this webpage. You can also \href{https://ximera.osu.edu/firststeps24html/aFirstStepInXimera/basics/Matrix_Product_Ansatz.tex}{download the TeX source file.} \section{About this webpage} This webpage was created with \href{https://ximera.osu.edu/}{Ximera}, an interactive textbook platform hosted by Ohio State University. The Ximera Project is funded 2024-2026 (with no other external funding) by a \$2,125,000 \href{https://www.ed.gov/grants-and-programs/grants-higher-education/improvement-postsecondary-education/open-textbooks-pilot-program}{Open Textbooks Pilot Program} grant from the federal Department of Education. \section{Introduction} The \underline{Matrix Product Ansatz} is a method for finding stationary measures in an interacting particle system with open boundary conditions. Let the generator be written in the form \[ B_1 + \sum_{l=1}^l w_{l,l+1} + \bar{B}_L \] where we use the subscript notation. In other words, \(w\) is a local two--site generator, while \(B\) acts on the left--most lattice site, and \(\bar{B}\) acts on the right--most lattice site. Denote a particle configuration on \(L\) sites by \[ \mathcal{C} = (\tau_1,\ldots,\tau_L), \] where each \(tau_i\) are particle variables equally either 0 or 1, indicating the number of particles. The Ansatz takes the form \[ \mathcal{S}(\mathcal{C}) = \frac{1}{Z_L} \langle W | \prod_{i=1}^L ((1-\tau_i)E + \tau_i D) | V \rangle \] where \(E\) and \(D\) are elements of a non--commutative algebra, and the product is ordered from the index \(i=1\) on the left to \(i=L\) on the right. In \cite{KS97}, it was proven that there is a solution of the form \[ w\left[ \binom{E}{D} \otimes \binom{E}{D} \right] \] \begin{thebibliography}{10} \bibitem[CRV14]{CRV14} N Crampe, E Ragoucy and M Vanicat, ``Integrable approach to simple exclusion processes with boundaries. Review and progress.'' Journal of Statistical Mechanics: Theory and Experiment, Volume 2014, November 2014 \bibitem[DEHP93]{DEHP93} B Derrida, M R Evans, V Hakim and V Pasquier Exact solution of a 1D asymmetric exclusion model using a matrix formulation Journal of Physics A: Mathematical and General, Volume 26, Number 7, 1993. \bibitem[KS97]{KS97} K. Krebs and S. Sandow, Matrix Product Eigenstates for One-Dimensional Stochastic Models and Quantum Spin Chains, J. Phys. A30 (1997) 3165 and arXiv:cond-mat/9610029. \end{thebibliography} \end{document}