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Atlas.IntroductionToPartialDifferentialEquations.code.CM17.FlowSymmetry

@[reducible, inline]
abbrev ODEFlow.Spacetime (n : ) :

A spacetime point in $\mathbb{R}^{1+n}$.

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    @[reducible, inline]

    A real-valued scalar field on $\mathbb{R}^{1+n}$.

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      @[reducible, inline]

      A vector field on $\mathbb{R}^{1+n}$, i.e. a map from spacetime points to vectors.

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        @[reducible, inline]
        abbrev ODEFlow.Metric (n : ) :

        A spacetime metric: at each point of $\mathbb{R}^{1+n}$, a function $m_{\mu\nu}$ on pairs of indices.

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          noncomputable def ODEFlow.spacetimeGradient {n : } (φ : ScalarField n) (x : Spacetime n) :
          Fin (n + 1)

          The spacetime gradient of a scalar field $\varphi$: the index-$\mu$ component is the partial derivative $\partial_\mu \varphi$.

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            noncomputable def ODEFlow.jacobian {n : } (F : Spacetime nSpacetime n) (x : Spacetime n) :
            Fin (n + 1)Fin (n + 1)

            The Jacobian of a map $F : \mathbb{R}^{1+n} \to \mathbb{R}^{1+n}$ at $x$: $(\partial F^\mu / \partial x^\nu)(x)$.

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              def ODEFlow.kroneckerDelta (n : ) (μ ν : Fin (n + 1)) :

              The Kronecker delta $\delta_{\mu\nu}$, equal to $1$ if $\mu = \nu$ and $0$ otherwise.

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                noncomputable def ODEFlow.divergence {n : } (Y : VectorField n) (x : Spacetime n) :

                The (spacetime) divergence of a vector field $Y$: $\nabla \cdot Y = \sum_\alpha \partial_\alpha Y^\alpha$.

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                  noncomputable def ODEFlow.jacobianMatrix {n : } (G : Spacetime nSpacetime n) (x : Spacetime n) :
                  Matrix (Fin (n + 1)) (Fin (n + 1))

                  The Jacobian of a spacetime map packaged as a matrix.

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                    A vector field $Y$ has all partial derivatives uniformly bounded by $C > 0$: $|\partial_\mu Y^\nu(x)| \leq C$ for all $x, \mu, \nu$.

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                      structure ODEFlow.FlowMapData (n : ) :

                      Data packaging the ODE flow generated by a vector field $Y$ on spacetime $\mathbb{R}^{1+n}$ (Proposition 2.0.1): the flow map $F_\epsilon$ on $[-\epsilon_0, \epsilon_0]$, its smoothness, the one-parameter group properties, the Taylor expansion, and the corresponding expansion of the Jacobian.

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                        def ODEFlow.transformScalar {n : } (φ : ScalarField n) (Finv : Spacetime nSpacetime n) :

                        Transformation of a scalar field under a change of coordinates: $\widetilde{\varphi}(\widetilde{x}) = \varphi(F^{-1}(\widetilde{x}))$ (cf. Definition 2.0.6).

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                          noncomputable def ODEFlow.transformGradient {n : } (φ : ScalarField n) (Finv : Spacetime nSpacetime n) (xt : Spacetime n) :
                          Fin (n + 1)

                          Transformation of the spacetime gradient of a scalar field under a change of coordinates (Definition 2.0.6): $\widetilde{\nabla}_\mu \widetilde{\varphi} = (M^{-1})_\mu{}^\alpha \nabla_\alpha \varphi$, expressed using the Jacobian of $F^{-1}$.

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                            noncomputable def ODEFlow.transformMetric {n : } (m : Metric n) (Finv : Spacetime nSpacetime n) :

                            Transformation of a metric under a change of coordinates (Definition 2.0.6): $\widetilde{m}_{\mu\nu} = (M^{-1})_\mu{}^\alpha (M^{-1})_\nu{}^\beta m_{\alpha\beta}$, expressed using the Jacobian of $F^{-1}$.

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                              A Lagrangian as a function of $(\varphi, \nabla \varphi, m)$: the scalar field value, its gradient, and the metric components.

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                                A Lagrangian $\mathcal{L}(\varphi, \nabla \varphi, m)$ is coordinate invariant (Definition 2.0.7) if for every smooth diffeomorphism $\Psi$ and every scalar field $\varphi$ and metric $m$, the value $\mathcal{L}$ evaluated on the original fields at $x$ equals $\mathcal{L}$ evaluated on the transformed fields at $\widetilde{x} = \Psi(x)$.

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