{"title":"Cyclicity Analysis of the Ornstein-Uhlenbeck Process","authors":"Vivek Kaushik","doi":"arxiv-2409.12102","DOIUrl":null,"url":null,"abstract":"In this thesis, we consider an $N$-dimensional Ornstein-Uhlenbeck (OU)\nprocess satisfying the linear stochastic differential equation $d\\mathbf x(t) =\n- \\mathbf B\\mathbf x(t) dt + \\boldsymbol \\Sigma d \\mathbf w(t).$ Here, $\\mathbf\nB$ is a fixed $N \\times N$ circulant friction matrix whose eigenvalues have\npositive real parts, $\\boldsymbol \\Sigma$ is a fixed $N \\times M$ matrix. We\nconsider a signal propagation model governed by this OU process. In this model,\nan underlying signal propagates throughout a network consisting of $N$ linked\nsensors located in space. We interpret the $n$-th component of the OU process\nas the measurement of the propagating effect made by the $n$-th sensor. The\nmatrix $\\mathbf B$ represents the sensor network structure: if $\\mathbf B$ has\nfirst row $(b_1 \\ , \\ \\dots \\ , \\ b_N),$ where $b_1>0$ and $b_2 \\ , \\ \\dots \\\n,\\ b_N \\le 0,$ then the magnitude of $b_p$ quantifies how receptive the $n$-th\nsensor is to activity within the $(n+p-1)$-th sensor. Finally, the $(m,n)$-th\nentry of the matrix $\\mathbf D = \\frac{\\boldsymbol \\Sigma \\boldsymbol\n\\Sigma^\\text T}{2}$ is the covariance of the component noises injected into the\n$m$-th and $n$-th sensors. For different choices of $\\mathbf B$ and\n$\\boldsymbol \\Sigma,$ we investigate whether Cyclicity Analysis enables us to\nrecover the structure of network. Roughly speaking, Cyclicity Analysis studies\nthe lead-lag dynamics pertaining to the components of a multivariate signal. We\nspecifically consider an $N \\times N$ skew-symmetric matrix $\\mathbf Q,$ known\nas the lead matrix, in which the sign of its $(m,n)$-th entry captures the\nlead-lag relationship between the $m$-th and $n$-th component OU processes. We\ninvestigate whether the structure of the leading eigenvector of $\\mathbf Q,$\nthe eigenvector corresponding to the largest eigenvalue of $\\mathbf Q$ in\nmodulus, reflects the network structure induced by $\\mathbf B.$","PeriodicalId":501379,"journal":{"name":"arXiv - STAT - Statistics Theory","volume":"20 1","pages":""},"PeriodicalIF":0.0000,"publicationDate":"2024-09-18","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"","citationCount":"0","resultStr":null,"platform":"Semanticscholar","paperid":null,"PeriodicalName":"arXiv - STAT - Statistics Theory","FirstCategoryId":"1085","ListUrlMain":"https://doi.org/arxiv-2409.12102","RegionNum":0,"RegionCategory":null,"ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":null,"EPubDate":"","PubModel":"","JCR":"","JCRName":"","Score":null,"Total":0}
引用次数: 0
Abstract
In this thesis, we consider an $N$-dimensional Ornstein-Uhlenbeck (OU)
process satisfying the linear stochastic differential equation $d\mathbf x(t) =
- \mathbf B\mathbf x(t) dt + \boldsymbol \Sigma d \mathbf w(t).$ Here, $\mathbf
B$ is a fixed $N \times N$ circulant friction matrix whose eigenvalues have
positive real parts, $\boldsymbol \Sigma$ is a fixed $N \times M$ matrix. We
consider a signal propagation model governed by this OU process. In this model,
an underlying signal propagates throughout a network consisting of $N$ linked
sensors located in space. We interpret the $n$-th component of the OU process
as the measurement of the propagating effect made by the $n$-th sensor. The
matrix $\mathbf B$ represents the sensor network structure: if $\mathbf B$ has
first row $(b_1 \ , \ \dots \ , \ b_N),$ where $b_1>0$ and $b_2 \ , \ \dots \
,\ b_N \le 0,$ then the magnitude of $b_p$ quantifies how receptive the $n$-th
sensor is to activity within the $(n+p-1)$-th sensor. Finally, the $(m,n)$-th
entry of the matrix $\mathbf D = \frac{\boldsymbol \Sigma \boldsymbol
\Sigma^\text T}{2}$ is the covariance of the component noises injected into the
$m$-th and $n$-th sensors. For different choices of $\mathbf B$ and
$\boldsymbol \Sigma,$ we investigate whether Cyclicity Analysis enables us to
recover the structure of network. Roughly speaking, Cyclicity Analysis studies
the lead-lag dynamics pertaining to the components of a multivariate signal. We
specifically consider an $N \times N$ skew-symmetric matrix $\mathbf Q,$ known
as the lead matrix, in which the sign of its $(m,n)$-th entry captures the
lead-lag relationship between the $m$-th and $n$-th component OU processes. We
investigate whether the structure of the leading eigenvector of $\mathbf Q,$
the eigenvector corresponding to the largest eigenvalue of $\mathbf Q$ in
modulus, reflects the network structure induced by $\mathbf B.$