Access the full text.
Sign up today, get DeepDyve free for 14 days.
[In this Chapter we analyze correlation functions of the type: 8.1\documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$\begin{aligned} {\mathcal T}( \partial ^{\alpha _1} G_1(h) \, \partial ^{\alpha _2} G_2(h) \ldots ) \; , \quad h \in {\mathcal A}_d \; , \end{aligned}$$\end{document}where \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$$G_i$$\end{document}’s are only piecewise continuous and the discontinuities occur inside the essential spectrum of h. We establish that, if the discontinuities occur inside the mobility gaps of h, then the canonical finite-volume algorithm presented in Chap. 5 continues to display a rapid convergence to the thermodynamic limit. Key to the error estimates is the Aizenman–Molchanov bound (Aizenman and Molchanov, Commun Math Phys 157:245–278, 1993, [2], Aizenman and Warzel, Random operators: disorder effects on quantum spectra and dynamics, 2015, [3]), which is discussed and adapted to the present context.]
Published: Mar 18, 2017
Read and print from thousands of top scholarly journals.
Already have an account? Log in
Bookmark this article. You can see your Bookmarks on your DeepDyve Library.
To save an article, log in first, or sign up for a DeepDyve account if you don’t already have one.
Copy and paste the desired citation format or use the link below to download a file formatted for EndNote
Access the full text.
Sign up today, get DeepDyve free for 14 days.
All DeepDyve websites use cookies to improve your online experience. They were placed on your computer when you launched this website. You can change your cookie settings through your browser.