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| author | Thibaut Horel <thibaut.horel@gmail.com> | 2015-01-24 19:26:37 -0500 |
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| committer | Thibaut Horel <thibaut.horel@gmail.com> | 2015-01-24 19:26:37 -0500 |
| commit | 38435205bff612b501f863b78cb91e7322e35594 (patch) | |
| tree | 270ee93fd383c1fa249eaa3c3d33c0f0e9a20a1a | |
| parent | 05f79327171003500015da2cc4974c6568d56061 (diff) | |
| download | cascades-38435205bff612b501f863b78cb91e7322e35594.tar.gz | |
Beginning of the model section
| -rw-r--r-- | paper/paper.tex | 11 | ||||
| -rw-r--r-- | paper/sections/model.tex | 52 |
2 files changed, 61 insertions, 2 deletions
diff --git a/paper/paper.tex b/paper/paper.tex index b677e6c..86ef9d8 100644 --- a/paper/paper.tex +++ b/paper/paper.tex @@ -46,6 +46,17 @@ % Therefore, a short form for the running title is supplied here: \icmltitlerunning{Cracking Cascades: Sparse Recovery for Graph Inference} +\usepackage{amsmath, amsfonts, amssymb} +\newcommand{\reals}{\mathbb{R}} +\newcommand{\ints}{\mathbb{N}} +\DeclareMathOperator{\E}{\mathbb{E}} +\let\P\relax +\DeclareMathOperator{\P}{\mathbb{P}} +\newcommand{\ex}[1]{\E\left[#1\right]} +\newcommand{\prob}[1]{\P\left[#1\right]} +\newcommand{\inprod}[2]{#1 \cdot #2} +\newcommand{\defeq}{\equiv} + \begin{document} \twocolumn[ diff --git a/paper/sections/model.tex b/paper/sections/model.tex index 601ddeb..3c0a354 100644 --- a/paper/sections/model.tex +++ b/paper/sections/model.tex @@ -1,4 +1,52 @@ -\subsection{Independent Cascade Model} +\subsection{Influence Cascades} + +We consider a weighted graph $G$ over the set of vertices $V$. The edge weights +are given by an (unknown) weight matrix $\Theta:V^2\to\reals^+$. $\Theta_{i,j} += 0$ simply expresses that there is no edge from $i$ to $j$. We define $m=|V|$, +and for $j\in V$, we write $\theta_j$ the $j$-th column of $\Theta$: this is +the indicator vector of the parents of $j$ in $G$. + +An \emph{influence cascade} is a homogeneous discrete-time Markov process over +$\{0,1\}^m$. More precisely, we represent the set of nodes infected at time +step $t-1\in\ints^+$ by a vector $x^{t}\in\{0,1\}^{m}$ where $x^{t}_k = 1$ can +be interpreted as \emph{node $k$ was infected at time step $t-1$}. + +We will restrict ourselves to influence processes such that for $j\in V$, +$x_j^{t+1}$ is a Bernouilli variable whose parameter can be expressed as +a function $f$ of $\inprod{\theta_j}{x^t}$, where $\inprod{a}{b}$ is the inner +product of $a$ and $b$ in $\reals^m$: +$\theta_j$ and $x^t$: +\begin{equation}\label{eq:markov} + \P\big[x_j^{t+1} = 1\,|\, x^t\big] \defeq f(\inprod{\theta_j}{x^t}). +\end{equation} +As we will later see, this type of influence processes encompasses the most +widely used influence processes: the Voter model (V), the Independent Cascade +model (IC), and the Linear Threshold model (T). + +\subsection{Problem} + +Our goal is to infer the weight matrix $\Theta$ by observing influence +cascades. Given the form of \eqref{eq:markov}, we will focus on a single row +$\theta_j$ of $\Theta$ and we will write $y^t_j \defeq x_j^{t+1}$. When there +is no ambiguity, we will simply write $y^t = y^t_j$ and $\theta= \theta_j$. -\subsection{The Voter Model} +The input of our problem is a set of observations $(x^1, y^1),\ldots,(x^n, +y^n)$. If we observe more than one cascade, we simply concatenate the +observations from each cascade to form a single longer cascade. +Equation~\eqref{eq:markov} still holds for each observation. + +With these notations, the set of observations follows a Generalized Linear +Model with Bernoulli distribution and link function $g$ such that $g^{-1} += f$. The log-likelihood of $\theta$ can be written: +\begin{displaymath} + \mathcal{L}(\theta\,|\, x, y) = \sum_{t=1}^ny^t \log f(\inprod{\theta}{x^t}) + + (1-y^t)\log \big(1-f(\inprod{\theta}{x^t})\big) +\end{displaymath} + +\paragraph{Sparsity} + + +\subsection{Voter Model} + +\subsection{Independent Cascade Model} |
