{ "cells" : [ { "cell_origin" : "client", "cell_type" : "latex", "cells" : [ { "cell_origin" : "client", "cell_type" : "latex_view", "source" : "\\section*{A higher-derivative Bianchi identity}\n\nThe identity which we will prove here comes from appendix A of hep-th/0111128. It shows that a particular\ncubic polynomial of Weyl tensors vanishes by virtue of the Weyl tensor multi-term symmetries. The declaration\nof the indices, Weyl tensor and covariant derivative is done with:" } ], "hidden" : true, "source" : "\\section*{A higher-derivative Bianchi identity}\n\nThe identity which we will prove here comes from appendix A of hep-th/0111128. It shows that a particular\ncubic polynomial of Weyl tensors vanishes by virtue of the Weyl tensor multi-term symmetries. The declaration\nof the indices, Weyl tensor and covariant derivative is done with:" }, { "cell_origin" : "client", "cell_type" : "input", "cells" : [ { "cell_origin" : "server", "cell_type" : "latex_view", "source" : "\\begin{dmath*}{}-C_{i m k l} C_{j p k q} C_{l p m q}%\n+\\frac{1}{4}C_{i m k l} C_{j m p q} C_{k l p q}%\n - \\frac{1}{2}C_{i k j l} C_{k m p q} C_{l m p q}\\end{dmath*}" }, { "cell_origin" : "server", "cell_type" : "latex_view", "source" : "\\begin{dmath*}{}\\nabla_{i}\\left(\\nabla_{j}\\left(-C_{i m k l} C_{j p k q} C_{l p m q}%\n+\\frac{1}{4}C_{i m k l} C_{j m p q} C_{k l p q}%\n - \\frac{1}{2}C_{i k j l} C_{k m p q} C_{l m p q}\\right)\\right)%\n - \\frac{1}{6}\\nabla_{i}\\left(\\nabla_{i}\\left(C_{j m n k} C_{m p q n} C_{p j k q}%\n+\\frac{1}{2}C_{j k m n} C_{p q m n} C_{j k p q}\\right)\\right)\\end{dmath*}" } ], "source" : "{i,j,m,n,k,p,q,l,r,r#}::Indices(vector).\nC_{m n p q}::WeylTensor.\n\\nabla{#}::Derivative.\n\\nabla_{r}{ C_{m n p q} }::SatisfiesBianchi.\n\\delta_{i j}::KroneckerDelta.\n\nEij:=- C_{i m k l} C_{j p k q} C_{l p m q} + 1/4 C_{i m k l} C_{j m p q} C_{k l p q}\n - 1/2 C_{i k j l} C_{k m p q} C_{l m p q}:\n\nE:= C_{j m n k} C_{m p q n} C_{p j k q} + 1/2 C_{j k m n} C_{p q m n} C_{j k p q}:\n\nexp:= \\nabla_{i}{\\nabla_{j}{ @(Eij) }} - 1/6 \\nabla_{i}{\\nabla_{i}{ @(E) }};" }, { "cell_origin" : "client", "cell_type" : "latex", "cells" : [ { "cell_origin" : "client", "cell_type" : "latex_view", "source" : "First apply the product rule twice to write out derivatives:" } ], "hidden" : true, "source" : "First apply the product rule twice to write out derivatives:" }, { "cell_origin" : "client", "cell_type" : "input", "cells" : [ { "cell_origin" : "server", "cell_type" : "latex_view", "source" : "\\begin{dmath*}{}C_{i j m n} C_{i k m p} \\nabla_{q}\\left(\\nabla_{j}{C_{n k p q}}\\right)%\n-C_{i j m n} \\nabla_{k}{C_{i p m q}} \\nabla_{p}{C_{j q n k}}%\n-2C_{i j m n} \\nabla_{i}{C_{m k p q}} \\nabla_{p}{C_{j k n q}}%\n-C_{i j m n} \\nabla_{k}{C_{i k m p}} \\nabla_{q}{C_{j p n q}}%\n+C_{i j m n} C_{i k m p} \\nabla_{j}\\left(\\nabla_{q}{C_{n k p q}}\\right)%\n-2C_{i j m n} \\nabla_{i}{C_{j k m p}} \\nabla_{q}{C_{n k p q}}%\n-C_{i j m n} C_{i k p q} \\nabla_{m}\\left(\\nabla_{p}{C_{j q n k}}\\right)%\n - \\frac{1}{4}C_{i j m n} C_{i j k p} \\nabla_{q}\\left(\\nabla_{m}{C_{n q k p}}\\right)%\n+\\frac{1}{4}C_{i j m n} \\nabla_{k}{C_{i j p q}} \\nabla_{p}{C_{m n k q}}%\n - \\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{j k p q}} \\nabla_{k}{C_{m n p q}}%\n - \\frac{1}{4}C_{i j m n} \\nabla_{k}{C_{i j k p}} \\nabla_{q}{C_{m n p q}}%\n - \\frac{1}{4}C_{i j m n} C_{i j k p} \\nabla_{m}\\left(\\nabla_{q}{C_{n q k p}}\\right)%\n - \\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{m n k p}} \\nabla_{q}{C_{j q k p}}%\n+\\frac{1}{4}C_{i j m n} C_{i k p q} \\nabla_{j}\\left(\\nabla_{k}{C_{m n p q}}\\right)%\n - \\frac{1}{2}C_{i j m n} C_{i j m k} \\nabla_{p}\\left(\\nabla_{q}{C_{n p k q}}\\right)%\n+C_{i j m n} \\nabla_{k}{C_{i j m p}} \\nabla_{q}{C_{n q k p}}%\n-C_{i j m n} \\nabla_{k}{C_{i j m p}} \\nabla_{q}{C_{n k p q}}%\n+\\frac{1}{2}C_{i j m n} C_{i k p q} \\nabla_{m}\\left(\\nabla_{j}{C_{n k p q}}\\right)%\n+\\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{m k p q}} \\nabla_{n}{C_{j k p q}}%\n - \\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{j k p q}} \\nabla_{m}{C_{n k p q}}%\n+\\frac{1}{2}C_{i j m n} C_{i k p q} \\nabla_{j}\\left(\\nabla_{m}{C_{n k p q}}\\right)%\n+\\frac{1}{2}C_{i j m n} C_{i k m p} \\nabla_{q}\\left(\\nabla_{q}{C_{j k n p}}\\right)%\n+C_{i j m n} \\nabla_{k}{C_{i p m q}} \\nabla_{k}{C_{j p n q}}%\n - \\frac{1}{4}C_{i j m n} C_{i j k p} \\nabla_{q}\\left(\\nabla_{q}{C_{m n k p}}\\right)%\n - \\frac{1}{2}C_{i j m n} \\nabla_{k}{C_{i j p q}} \\nabla_{k}{C_{m n p q}}\\end{dmath*}" } ], "source" : "distribute(_); product_rule(_); distribute(_); product_rule(_)\nsort_product(_); canonicalise(_)\nrename_dummies(_);" }, { "cell_origin" : "client", "cell_type" : "latex", "cells" : [ { "cell_origin" : "client", "cell_type" : "latex_view", "source" : "Because the identity which we intend to prove is only supposed to hold on Einstein spaces, we\nset the divergence of the Weyl tensor to zero," } ], "hidden" : true, "source" : "Because the identity which we intend to prove is only supposed to hold on Einstein spaces, we\nset the divergence of the Weyl tensor to zero," }, { "cell_origin" : "client", "cell_type" : "input", "cells" : [ { "cell_origin" : "server", "cell_type" : "latex_view", "source" : "\\begin{dmath*}{}C_{i j m n} C_{i k m p} \\nabla_{q}\\left(\\nabla_{j}{C_{n k p q}}\\right)%\n-C_{i j m n} \\nabla_{k}{C_{i p m q}} \\nabla_{p}{C_{j q n k}}%\n-2C_{i j m n} \\nabla_{i}{C_{m k p q}} \\nabla_{p}{C_{j k n q}}%\n-C_{i j m n} C_{i k p q} \\nabla_{m}\\left(\\nabla_{p}{C_{j q n k}}\\right)%\n - \\frac{1}{4}C_{i j m n} C_{i j k p} \\nabla_{q}\\left(\\nabla_{m}{C_{n q k p}}\\right)%\n+\\frac{1}{4}C_{i j m n} \\nabla_{k}{C_{i j p q}} \\nabla_{p}{C_{m n k q}}%\n - \\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{j k p q}} \\nabla_{k}{C_{m n p q}}%\n+\\frac{1}{4}C_{i j m n} C_{i k p q} \\nabla_{j}\\left(\\nabla_{k}{C_{m n p q}}\\right)%\n+\\frac{1}{2}C_{i j m n} C_{i k p q} \\nabla_{m}\\left(\\nabla_{j}{C_{n k p q}}\\right)%\n+\\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{m k p q}} \\nabla_{n}{C_{j k p q}}%\n - \\frac{1}{2}C_{i j m n} \\nabla_{i}{C_{j k p q}} \\nabla_{m}{C_{n k p q}}%\n+\\frac{1}{2}C_{i j m n} C_{i k p q} \\nabla_{j}\\left(\\nabla_{m}{C_{n k p q}}\\right)%\n+\\frac{1}{2}C_{i j m n} C_{i k m p} \\nabla_{q}\\left(\\nabla_{q}{C_{j k n p}}\\right)%\n+C_{i j m n} \\nabla_{k}{C_{i p m q}} \\nabla_{k}{C_{j p n q}}%\n - \\frac{1}{4}C_{i j m n} C_{i j k p} \\nabla_{q}\\left(\\nabla_{q}{C_{m n k p}}\\right)%\n - \\frac{1}{2}C_{i j m n} \\nabla_{k}{C_{i j p q}} \\nabla_{k}{C_{m n p q}}\\end{dmath*}" } ], "source" : "substitute(_, $\\nabla_{i}{ C_{k i l m} } -> 0, \\nabla_{i}{ C_{k m l i} } -> 0$);" }, { "cell_origin" : "client", "cell_type" : "latex", "cells" : [ { "cell_origin" : "client", "cell_type" : "latex_view", "source" : "This expression should vanish upon use of the Bianchi identity. By expanding all tensors using\ntheir Young projectors, this becomes manifest; a few seconds of computation produces:" } ], "hidden" : true, "source" : "This expression should vanish upon use of the Bianchi identity. By expanding all tensors using\ntheir Young projectors, this becomes manifest; a few seconds of computation produces:" }, { "cell_origin" : "client", "cell_type" : "input", "cells" : [ { "cell_origin" : "server", "cell_type" : "latex_view", "source" : "\\begin{dmath*}{}0\\end{dmath*}" } ], "source" : "young_project_product(_);" }, { "cell_origin" : "client", "cell_type" : "latex", "cells" : [ { "cell_origin" : "client", "cell_type" : "latex_view", "source" : "This proves the identity." } ], "hidden" : true, "source" : "This proves the identity." }, { "cell_origin" : "client", "cell_type" : "input", "source" : "" } ], "description" : "Cadabra JSON notebook format", "version" : 1 }