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lanczos_demmel
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09b382098c |
@@ -7,6 +7,7 @@ dependencies = [
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"matplotlib>=3.10.8",
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"numpy>=2.0.0",
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"pygsp>=0.6.1",
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"scienceplots>=2.2.1",
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"scipy>=1.10.0",
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]
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requires-python = ">=3.10"
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+85
-28
@@ -1,45 +1,102 @@
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% !TeX program = pdflatex
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\documentclass{mathreport} % Uses our custom mathreport.cls
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\documentclass[11pt]{article}
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\usepackage[margin=1.2in]{geometry}
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\usepackage[utf8]{inputenc}
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\usepackage[T1]{fontenc}
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\usepackage[english]{babel}
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\usepackage{fourier}
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\usepackage{amsthm}
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\usepackage{amssymb}
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\usepackage{amsmath}
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\usepackage{amsfonts}
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\usepackage{latexsym}
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\usepackage{graphicx}
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\usepackage{float}
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\usepackage{etoolbox}
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\usepackage{hyperref}
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\usepackage{tikz}
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\usepackage{lipsum}
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\usepackage{algorithm}
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\usepackage{algpseudocode}
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\usepackage{mathtools}
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\usepackage{nccmath}
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\usepackage[most]{tcolorbox}
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\newtcolorbox[auto counter]{problem}[1][]{%
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enhanced,
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breakable,
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colback=white,
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colbacktitle=white,
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coltitle=black,
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fonttitle=\bfseries,
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boxrule=.6pt,
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titlerule=.2pt,
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toptitle=3pt,
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bottomtitle=3pt,
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title=GitHub repository of this project}
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% Load bibliography
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\addbibresource{references.bib}
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\usepackage{lipsum} % Just for the demo text
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\RequirePackage[activate={true,nocompatibility},final,tracking=true,kerning=true,spacing=true]{microtype}
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\SetTracking{encoding={*}, shape=sc}{40} % Spacing for Small Caps
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% --- Document Metadata ---
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\title{\normalfont\scshape\Large The Geometry of Complex Systems}
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\author{\normalfont\itshape A. N. Other}
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\date{\small\today}
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\newcommand{\R}{\mathbb{R}}
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\newcommand{\N}{\mathbb{N}}
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\newcommand{\Z}{\mathbb{Z}}
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\newcommand{\Q}{\mathbb{Q}}
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\newcommand{\C}{\mathbb{C}}
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\newtheorem{theorem}{Theorem}[section]
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\newtheorem{lemma}[theorem]{Lemma}
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\newtheorem{proposition}[theorem]{Proposition}
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\newtheorem{corollary}[theorem]{Corollary}
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\theoremstyle{definition}
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\newtheorem{definition}[theorem]{Definition}
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\newtheorem{example}[theorem]{Example}
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\theoremstyle{remark}
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\newtheorem{remark}[theorem]{Remark}
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\title{%
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Accelerated filtering on graphs using Lanczos method
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\\ \large Relazione del progetto di Calcolo Scientifico}
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\author{Alberto Defendi}
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\date{}
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\setlength{\parskip}{1em}
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\setlength{\parindent}{0em}
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\begin{document}
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\maketitle
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\begin{abstract}
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\noindent \small \textbf{\textit{Abstract.}} \lipsum[1][1-4]
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\noindent The Lanczos algorithm \ldots
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\end{abstract}
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\section{Introduction}
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This document uses a custom class file (\texttt{mathreport.cls}). This keeps the main file clean. The typography is set to Bringhurst's standards: wide margins, Palatino font, and old-style figures (e.g., 12345).
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{\setlength{\parskip}{0em}
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\tableofcontents}
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\section{Mathematical Theory}
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We define our primary operator in the Hilbert space $\mathcal{H}$.
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\section{Introduzione}
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\begin{definition}[Compact Operator]
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An operator $T: X \to Y$ is compact if $\overline{T(B_X)}$ is compact in $Y$.
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\end{definition}
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Introduciamo alcuni concetti di teoria dei grafi e alcuni risultati del corso che verranno usati nel corso della sperimentazione.
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Scopo del progetto è verificare numericamente i risultati
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\begin{theorem}[Spectral Theorem]
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There exists an orthonormal basis of eigenvectors.
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\end{theorem}
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Nell'analisi consideriamo i grafi di Erdo''s-Reiny (Figura)
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Consider the harmonic series shown in \cref{eq:harmonic}. The styling is handled entirely by the external class file.
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\begin{equation} \label{eq:harmonic}
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H_n = \sum_{k=1}^n \frac{1}{k} \approx \ln n + \gamma
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\end{equation}
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Consideriamo un grafo non diretto e pesato $ G = (V, E, W)$.
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\section{Esperimento 1}
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Studiamo i grafi di Erdos-Reiny e di tipo Sensors. Dal plot possiamo
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Figura (dida: Grafi di ER e sensor colorati in base al segnale (non filtrato, sopra) e filtrato
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attraverso la valutazione $g(\mathcal{L})s$.
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test
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\clearpage
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\bibliographystyle{unsrt}
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\bibliography{ref}
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\nocite{*}
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\section{Results and Discussion}
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\lipsum[2-4]
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\printbibliography
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\end{document}
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@@ -0,0 +1,9 @@
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@article{susnjara2015,
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title={Accelerated filtering on graphs using Lanczos method},
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author={Ana Susnjara and Nathanael Perraudin and Daniel Kressner and Pierre Vandergheynst},
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year={2015},
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eprint={1509.04537},
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archivePrefix={arXiv},
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primaryClass={math.NA},
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url={https://arxiv.org/abs/1509.04537},
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}
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@@ -1,7 +0,0 @@
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@book{bringhurst2004,
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author = {Robert Bringhurst},
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title = {The Elements of Typographic Style},
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year = {2004},
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publisher = {Hartley \& Marks},
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address = {Vancouver}
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}
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@@ -1,40 +0,0 @@
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import numpy as np
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import numpy.linalg as LA
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"""
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Arguments
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L Real valued NxN symmetric matrix
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s vector of size N
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M natural number indicating basis size
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Returns
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-------
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V : ndarray
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M-dimensional vector with orthonormal columns.
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alp : ndarray
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M-dimensional array of scalars.
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beta : ndarray
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M-dimensional array of scalars.
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"""
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def lanczos(L, s, M):
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N = len(s)
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alp = np.zeros(M)
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beta = np.zeros(M - 1)
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V = np.zeros((N, M))
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V[:, 0] = s / LA.norm(s)
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for j in range(M):
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w = L @ V[:, j]
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alp[j] = np.dot(V[:, j], w)
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v_tilde = w - V[:, j] * alp[j]
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if j > 0:
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v_tilde = v_tilde - V[:, j - 1] * beta[j - 1]
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if j < M - 1:
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beta[j] = LA.norm(v_tilde)
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V[:, j + 1] = v_tilde / beta[j]
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return [V, alp, beta]
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+7
-4
@@ -1,10 +1,13 @@
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# src/afgl/main.py
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import sys
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import afgl.test_2 as t_2
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from afgl.util.plot import plot_setup
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def run():
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"""Main execution function."""
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print("Starting the Accelerated Filtering Graphs Lanczos (AFGL) process...")
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def run() -> None:
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plot_setup()
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# t_1.run()
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t_2.run()
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if __name__ == "__main__":
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@@ -0,0 +1,177 @@
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import matplotlib.pyplot as plt
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import matplotlib.ticker as ticker
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import numpy as np
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import numpy.linalg as LA
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# Requires latex installed
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import scienceplots # noqa: F401
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import scipy
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from pygsp import graphs
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from afgl.util.build_T_matrix import build_T_matrix
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from afgl.util.lanczos import lanczos
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from afgl.util.plot import latex_log_formatter
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def plot_graphs(G_ER, G_Sensor, s: np.ndarray, N: int, p: float) -> None:
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fig, axs = plt.subplots(2, 2, figsize=(6.6, 5))
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# Set coordinates
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G_ER.set_coordinates()
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G_Sensor.set_coordinates()
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signal_ER = filter_signal_with_fourier(G_ER, s)
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signal_S = filter_signal_with_fourier(G_Sensor, s)
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# TOP LEFT
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G_ER.plot(s, ax=axs[0, 0], vertex_size=15, edge_width=0.5, edge_color="gray")
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axs[0, 0].set_title(rf"Erdős-Rényi Graph $(N = {N}, p = {p})$", pad=20)
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axs[0, 0].set_axis_off()
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# BOTTOM LEFT
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G_ER.plot(
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signal_ER, ax=axs[1, 0], vertex_size=15, edge_width=0.5, edge_color="gray"
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)
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axs[1, 0].set_title("", pad=20)
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axs[1, 0].set_axis_off()
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# TOP RIGHT
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G_Sensor.plot(s, ax=axs[0, 1], vertex_size=15, edge_width=0.5, edge_color="gray")
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axs[0, 1].set_title(rf"Sensor Network $(N = {N})$", pad=20)
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axs[0, 1].set_axis_off()
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# BOTTOM RIGHT
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G_Sensor.plot(
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signal_S, ax=axs[1, 1], vertex_size=15, edge_width=0.5, edge_color="gray"
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)
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axs[1, 1].set_title("", pad=20)
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axs[1, 1].set_axis_off()
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# Prevent label/title overlap
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plt.savefig("./out/printed_graphs.pdf", bbox_inches="tight")
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def g_extended(t: np.ndarray) -> np.ndarray:
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return np.sin(0.5 * np.pi * np.cos(np.pi * t) ** 2)
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"""
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Evaluates the function sin(0.5*pi*cos(pi*t)^2)chi_[-1/2,1/2] where chi_I is the
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characteristic function of I, as defined in example 1 (see [1]).
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"""
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def g(T: np.ndarray) -> np.ndarray:
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if scipy.sparse.issparse(T):
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# Operator & not supporting sparse matrix
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T = T.toarray()
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Chi = ((T >= -1 / 2) & (T <= 1 / 2)).astype(int)
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# Apply g_extended where Chi is True, else output 0
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return np.where(Chi, g_extended(T), 0)
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"""
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Computes the approximation g_M (see [1]) using Lanczos
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"""
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def compute_g_M(
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V: np.ndarray, alp: np.ndarray, beta: np.ndarray, s: np.ndarray
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) -> np.ndarray:
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M = len(alp)
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e_1 = np.zeros(M)
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e_1[0] = 1
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T = build_T_matrix(alp, beta)
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y = LA.norm(s) * (g(T) @ e_1)
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return V @ y
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def filter_signal_with_fourier(G, s: np.ndarray) -> np.ndarray:
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G.compute_fourier_basis()
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U = G.U
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return (U @ np.diag(g(G.e)) @ U.T) @ s
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def plot_error_comparison(
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l_err_ER: np.ndarray, t_err_ER: np.ndarray, l_err_S: np.ndarray, t_err_S: np.ndarray
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) -> None:
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fig, (ax1, ax2) = plt.subplots(1, 2, figsize=(6.6, 2.5))
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# Left plot (Erdos-Renyi)
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ax1.plot(l_err_ER, label=r"$\left\lVert g_{M+3} - g_M \right\rVert_2$")
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ax1.plot(t_err_ER, label=r"$\left\lVert e_M \right\rVert_2$")
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ax1.set_title("Erdős-Rényi graph")
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# Right plot (Sensor)
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ax2.plot(l_err_S, label=r"$\left\lVert g_{M+3} - g_M \right\rVert_2$")
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ax2.plot(t_err_S, label=r"$\left\lVert e_M \right\rVert_2$")
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ax2.set_title("Sensor graph")
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# Apply identical formatting to both subplots
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for ax in (ax1, ax2):
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ax.xaxis.set_major_locator(ticker.MultipleLocator(50))
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ax.set_yscale("log")
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ax.yaxis.set_major_formatter(ticker.FuncFormatter(latex_log_formatter))
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ax.legend()
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# Prevents overlapping of labels between the subplots
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plt.tight_layout()
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plt.savefig("./out/ex1_estimate.pdf", bbox_inches="tight")
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def run_comparison_1_for_graph(
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G, s: np.ndarray, M_MAX: int
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) -> tuple[np.ndarray, np.ndarray]:
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"""Compares the error with error generated by Lanczos.
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Args:
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G: Graph
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s: Signal vector
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Returns:
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[lanczos_err, true_err]: Vectors of errors norm(g_{M+3} - g_M) and norm(e_M)
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as defined in [1]
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"""
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G.compute_laplacian("combinatorial")
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L = G.L
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j = 3
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V, alp, beta = lanczos(L, s, M_MAX + j)
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lanczos_err = np.zeros(M_MAX + j)
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true_err = np.zeros(M_MAX + j)
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GLs = filter_signal_with_fourier(G, s)
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for M in range(2, M_MAX + j):
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g_M = compute_g_M(V[:, 0:M], alp[0:M], beta[0 : M - 1], s)
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g_Mj = compute_g_M(V[:, 0 : M + j], alp[0 : M + j], beta[0 : M + j - 1], s)
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lanczos_err[M - 1] = LA.norm(g_Mj - g_M)
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true_err[M - 1] = LA.norm(GLs - g_M)
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return lanczos_err, true_err
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def run() -> None:
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"""Ripete il test corrispondente ad Example 1 dell'articolo limitandosi al
|
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metodo di Lanczos (no Chebyshev) e utilizzando come funzione g(t) = sin(0.5π
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cos(πt)2) * \chi_{[-0.5, 0.5]}.
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"""
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N = 500
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M_MAX = 200
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p = 0.04
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s = np.random.randint(1, 10000, N).astype(float)
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# Normalize s as in request
|
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s /= LA.norm(s)
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G_ER = graphs.ErdosRenyi(N, p)
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G_S = graphs.Sensor(N)
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l_err_ER, t_err_ER = run_comparison_1_for_graph(G_ER, s, M_MAX)
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l_err_S, t_err_S = run_comparison_1_for_graph(G_S, s, M_MAX)
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plot_error_comparison(l_err_ER, t_err_ER, l_err_S, t_err_S)
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plot_graphs(G_ER, G_S, s, N, p)
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@@ -0,0 +1,36 @@
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import numpy as np
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import numpy.linalg as LA
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from pygsp import graphs
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from afgl.util.lanczos import lanczos
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|
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|
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def run() -> None:
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"""Genera i grafi di di Erdos-Reny di grandezza crescente (ad esempio 250,
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500,1000, 2000, 4000) e parametro p = 0.04 e misura il tempo
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computazionale del metodo di Lanczos utilizzando come soglia per il criterio
|
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d'arresto epsilon = 10^-2 (o una soglia a scelta).
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Args:
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None
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||||
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Returns:
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None
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"""
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n = 6
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p = 0.04
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M = 200
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N_VALUES = 250 * (2 ** np.arange(n))
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|
||||
for N in N_VALUES:
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s = np.random.randint(1, 10000, N).astype(float)
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# Normalize s as in request
|
||||
s /= LA.norm(s)
|
||||
|
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G = graphs.ErdosRenyi(N, p)
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G.compute_laplacian("combinatorial")
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||||
L = G.L
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|
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lanczos(L, s, M)
|
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@@ -0,0 +1,5 @@
|
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import numpy as np
|
||||
|
||||
|
||||
def build_T_matrix(alp, beta):
|
||||
return np.diag(alp) + np.diag(beta, -1) + np.diag(beta, 1)
|
||||
@@ -0,0 +1,43 @@
|
||||
import numpy as np
|
||||
import numpy.linalg as LA
|
||||
|
||||
"""
|
||||
Classic Lanczos method (without re-orthogonalization)
|
||||
Using Demmel's book version.
|
||||
|
||||
Arguments
|
||||
L : Real valued NxN symmetric matrix
|
||||
s : vector of size N
|
||||
M : natural number indicating basis size
|
||||
|
||||
Returns
|
||||
-------
|
||||
V : ndarray
|
||||
M-dimensional vector with orthonormal columns.
|
||||
alp : ndarray
|
||||
M-dimensional array of scalars.
|
||||
beta : ndarray
|
||||
M-dimensional array of scalars.
|
||||
"""
|
||||
|
||||
|
||||
def lanczos(L, s, M):
|
||||
N = len(s)
|
||||
alp = np.zeros(M)
|
||||
beta = np.zeros(M)
|
||||
V = np.zeros((N, M + 1))
|
||||
V[:, 1] = s / LA.norm(s)
|
||||
|
||||
for j in range(1, M):
|
||||
w = L @ V[:, j]
|
||||
alp[j] = np.dot(V[:, j], w)
|
||||
|
||||
w = w - V[:, j] * alp[j] - V[:, j - 1] * beta[j - 1]
|
||||
|
||||
beta[j] = LA.norm(w)
|
||||
if beta[j] == 0:
|
||||
print("Breakdown")
|
||||
break
|
||||
V[:, j + 1] = w / beta[j]
|
||||
|
||||
return [V[:, 1:], alp, beta[1:]]
|
||||
@@ -0,0 +1,28 @@
|
||||
import matplotlib.pyplot as plt
|
||||
import numpy as np
|
||||
import scienceplots # noqa: F401
|
||||
from pygsp import plotting
|
||||
|
||||
|
||||
def latex_sci(val: float, decimals: int = 2) -> str:
|
||||
"""Converts a value to LaTeX scientific notation A x 10^{B}."""
|
||||
if val == 0:
|
||||
return "0"
|
||||
exponent = int(np.floor(np.log10(abs(val))))
|
||||
mantissa = val / 10**exponent
|
||||
return rf"{mantissa:.{decimals}f} \times 10^{{{exponent}}}"
|
||||
|
||||
|
||||
def latex_log_formatter(y: float, pos: int) -> str:
|
||||
"""Custom formatter to render tick labels as LaTeX 10^{n}."""
|
||||
if y <= 0:
|
||||
return ""
|
||||
# Extract the exponent using log10
|
||||
n = int(np.round(np.log10(y)))
|
||||
return f"$10^{{{n}}}$"
|
||||
|
||||
|
||||
def plot_setup() -> None:
|
||||
plotting.BACKEND = "matplotlib"
|
||||
plt.style.use(["science"])
|
||||
# TODO match font with document
|
||||
+3
-2
@@ -1,6 +1,7 @@
|
||||
import numpy as np
|
||||
import numpy.linalg as LA
|
||||
from afgl.lanczos import lanczos
|
||||
from afgl.util.build_T_matrix import build_T_matrix
|
||||
from afgl.util.lanczos import lanczos
|
||||
|
||||
"""
|
||||
Todo: better test case
|
||||
@@ -18,7 +19,7 @@ def test_lanczos_return_correct_solution():
|
||||
s = np.random.randint(1, 10, N)
|
||||
[V, alp, beta] = lanczos(L, s, M)
|
||||
|
||||
T = np.diag(alp) + np.diag(beta, -1) + np.diag(beta, 1)
|
||||
T = build_T_matrix(alp, beta)
|
||||
|
||||
x = LA.solve(L, s)
|
||||
e_1 = np.zeros(M)
|
||||
|
||||
@@ -15,6 +15,7 @@ dependencies = [
|
||||
{ name = "numpy", version = "2.2.6", source = { registry = "https://pypi.org/simple" }, marker = "python_full_version < '3.11'" },
|
||||
{ name = "numpy", version = "2.4.3", source = { registry = "https://pypi.org/simple" }, marker = "python_full_version >= '3.11'" },
|
||||
{ name = "pygsp" },
|
||||
{ name = "scienceplots" },
|
||||
{ name = "scipy", version = "1.15.3", source = { registry = "https://pypi.org/simple" }, marker = "python_full_version < '3.11'" },
|
||||
{ name = "scipy", version = "1.17.1", source = { registry = "https://pypi.org/simple" }, marker = "python_full_version >= '3.11'" },
|
||||
]
|
||||
@@ -24,6 +25,7 @@ requires-dist = [
|
||||
{ name = "matplotlib", specifier = ">=3.10.8" },
|
||||
{ name = "numpy", specifier = ">=2.0.0" },
|
||||
{ name = "pygsp", specifier = ">=0.6.1" },
|
||||
{ name = "scienceplots", specifier = ">=2.2.1" },
|
||||
{ name = "scipy", specifier = ">=1.10.0" },
|
||||
]
|
||||
|
||||
@@ -737,6 +739,18 @@ wheels = [
|
||||
{ url = "https://files.pythonhosted.org/packages/ec/57/56b9bcc3c9c6a792fcbaf139543cee77261f3651ca9da0c93f5c1221264b/python_dateutil-2.9.0.post0-py2.py3-none-any.whl", hash = "sha256:a8b2bc7bffae282281c8140a97d3aa9c14da0b136dfe83f850eea9a5f7470427", size = 229892, upload-time = "2024-03-01T18:36:18.57Z" },
|
||||
]
|
||||
|
||||
[[package]]
|
||||
name = "scienceplots"
|
||||
version = "2.2.1"
|
||||
source = { registry = "https://pypi.org/simple" }
|
||||
dependencies = [
|
||||
{ name = "matplotlib" },
|
||||
]
|
||||
sdist = { url = "https://files.pythonhosted.org/packages/ae/a5/5f858668ca1a513033a7f0d55cd12b0940a12e822f9f61f317ce344e07c6/scienceplots-2.2.1.tar.gz", hash = "sha256:51ad98c420e499d3284d07b6447a4b3aedd8ec122aca39ba91c58205226c408a", size = 17966, upload-time = "2026-02-25T01:26:54.603Z" }
|
||||
wheels = [
|
||||
{ url = "https://files.pythonhosted.org/packages/cc/22/14e7b20f7d11f3e9ea9b5ae6acf9ea695c423eee785906cd5c5914a841dc/scienceplots-2.2.1-py3-none-any.whl", hash = "sha256:a1a9f670cbf5b59d92cdd3250be85b079ee4cf08bcaf2ace5ef57995be0b6c42", size = 30237, upload-time = "2026-02-25T01:26:53.298Z" },
|
||||
]
|
||||
|
||||
[[package]]
|
||||
name = "scipy"
|
||||
version = "1.15.3"
|
||||
|
||||
Reference in New Issue
Block a user