{ "id": "1101.5041", "version": "v1", "published": "2011-01-26T12:23:46.000Z", "updated": "2011-01-26T12:23:46.000Z", "title": "The Symmetry Group of Gaussian States in $L^2 (\\mathbb{R}^n)$", "authors": [ "K. R. Parthasarathy" ], "categories": [ "math.PR" ], "abstract": "This is a continuation of the expository article \\cite{krp} with some new remarks. Let $S_n$ denote the set of all Gaussian states in the complex Hilbert space $L^2 (\\mathbb{R}^n),$ $K_n$ the convex set of all momentum and position covariance matrices of order $2n$ in Gaussian states and let $\\mathcal{G}_n$ be the group of all unitary operators in $L^2 (\\mathbb{R}^n)$ conjugations by which leave $S_n$ invariant. Here we prove the following results. $K_n$ is a closed convex set for which a matrix $S$ is an extreme point if and only if $S=\\frac{1}{2} L^{T} L$ for some $L$ in the symplectic group $Sp (2n, \\mathbb{R}).$ Every element in $K_n$ is of the form $\\frac{1}{2} (L^{T} L + M^{T} M)$ for some $L,M$ in $Sp (2n, \\mathbb{R}).$ Every Gaussian state in $L^2 (\\mathbb{R}^n)$ can be purified to a Gaussian state in $L^2 (\\mathbb{R}^{2n}).$ Any element $U$ in the group $\\mathcal{G}_n$ is of the form $U = \\lambda W ({\\bm {\\alpha}}) \\Gamma (L)$ where $\\lambda$ is a complex scalar of modulus unity, ${\\bm {\\alpha}} \\in \\mathbb{C}^n,$ $L \\in Sp (2n, \\mathbb{R}),$ $W({\\bm {\\alpha}})$ is the Weyl operator corresponding to ${\\bm {\\alpha}} $ and $\\Gamma (L)$ is a unitary operator which implements the Bogolioubov automorphism of the Lie algebra generated by the canonical momentum and position observables induced by the symplectic linear transformation $L.$", "revisions": [ { "version": "v1", "updated": "2011-01-26T12:23:46.000Z" } ], "analyses": { "subjects": [ "81S25", "60B15", "42A82", "81R30" ], "keywords": [ "gaussian state", "symmetry group", "unitary operator", "complex hilbert space", "position covariance matrices" ], "note": { "typesetting": "TeX", "pages": 0, "language": "en", "license": "arXiv", "status": "editable" } } }