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TauCeti.Analysis.PDE.Yamabe.Quotient

The Yamabe quotient and its Euler–Lagrange equation #

On a Riemannian manifold (M, g) of dimension n, the Yamabe quotient of a function u is

Q_g(u) = (∫ (aₙ |grad u|² + Scal_g u²) dV_g) / (∫ |u| ^ pₙ dV_g) ^ (2 / pₙ),

with aₙ = 4 (n - 1) / (n - 2) and pₙ = 2 n / (n - 2) (TauCeti.Yamabe.yamabeQuotient). It is invariant under multiplication of u by a nonzero constant. For a positive function u on a closed manifold, Q_g(u) is the volume-normalized total scalar curvature of the conformal metric u ^ (4 / (n - 2)) g, by TauCeti.Yamabe.integral_scalarCurvature_rescale_div_riemannianTotalVolume_rpow together with the energy identity TauCeti.Yamabe.integral_mul_conformalLaplacian_self, and the Yamabe problem asks for a minimizer.

This file computes the first variation of Q_g on a compact manifold. Write N(u) = ∫ |u| ^ pₙ dV. For C¹ functions u ≠ 0 and v,

d/dt Q_g(u + t v) |_(t = 0) = 2 ((∫ (aₙ ⟪grad v, grad u⟫ + Scal_g v u) dV) / N(u) ^ (2 / pₙ) - Q_g(u) (∫ |u| ^ (pₙ - 2) u v dV) / N(u)).

The energy is quadratic in t, and |·| ^ pₙ is differentiable with derivative pₙ |s| ^ (pₙ - 2) s because pₙ > 1, so N(u + t v) is differentiated under the integral sign. On a closed manifold, integration by parts turns the first term into ∫ v L_g u dV, where L_g is the conformal Laplacian. Since smooth functions separate continuous functions under integration, this gives the Euler–Lagrange equation: a nonzero C² function u is a critical point of Q_g in every smooth direction exactly when it solves

L_g u = λ |u| ^ (pₙ - 2) u

for some constant λ. Integrating the equation against u identifies the constant: Q_g(u) = λ N(u) ^ (1 - 2 / pₙ), so λ = Q_g(u) when u has unit L^pₙ norm. For a nonnegative u the equation is the Yamabe equation L_g u = λ u ^ (pₙ - 1); for a positive smooth u it says that u ^ (4 / (n - 2)) g has constant scalar curvature λ (TauCeti.Yamabe.scalarCurvature_rescale_eq_iff_conformalLaplacian_eq).

The quotient is defined for every function, through the Riemannian gradient and Bochner integrals; its classical meaning and variational results concern differentiable functions, while scale invariance (yamabeQuotient_smul) and nonnegativity under nonnegative scalar curvature hold for every function. The metric is the RiemannianBundle instance of the tangent bundle and the volume is TauCeti.riemannianVolume, as for TauCeti.Yamabe.conformalLaplacian.

Main declarations #

All in the namespace TauCeti.Yamabe.

References #

The Yamabe quotient Q_g(u) = (∫ (aₙ |grad u|² + Scal_g u²) dV_g) / (∫ |u| ^ pₙ dV_g) ^ (2 / pₙ) of a function u on a Riemannian manifold of dimension n, where aₙ = 4 (n - 1) / (n - 2) and pₙ = 2 n / (n - 2). Its classical meaning is for differentiable u.

Instances For

    Nonnegative scalar curvature makes the total Yamabe quotient nonnegative in dimension n > 2, even without regularity or integrability assumptions on the function.

    Scale invariance of the Yamabe quotient. In dimension n > 2, multiplying a function by a nonzero constant does not change its Yamabe quotient.

    @[simp]

    On a compact manifold of dimension n, the Yamabe quotient of the constant function 1 is the volume-normalized total scalar curvature (∫ Scal_g dV_g) / Vol(g) ^ (2 / pₙ).

    The first variation #

    The first variation of the Yamabe quotient. On a compact manifold of dimension n > 2, let u ≠ 0 and v be C¹ functions, and write N(u) = ∫ |u| ^ pₙ dV. Then t ↦ Q_g(u + t v) has derivative 2 ((∫ (aₙ ⟪grad v, grad u⟫ + Scal_g v u) dV) / N(u) ^ (2 / pₙ) - Q_g(u) (∫ |u| ^ (pₙ - 2) u v dV) / N(u)) at t = 0.

    The multiplier of the Euler–Lagrange equation. On a closed manifold of dimension n > 2, if a C² function u solves L_g u = λ |u| ^ (pₙ - 2) u, then Q_g(u) = λ (∫ |u| ^ pₙ dV) ^ (1 - 2 / pₙ).

    The multiplier at unit norm. On a closed manifold of dimension n > 2, if a C² function u with ∫ |u| ^ pₙ dV = 1 solves L_g u = λ |u| ^ (pₙ - 2) u, then λ = Q_g(u).

    The Euler–Lagrange equation of the Yamabe quotient. On a closed manifold of dimension n > 2, a nonzero C² function u is a critical point of the Yamabe quotient, in the sense that t ↦ Q_g(u + t v) has derivative 0 at t = 0 for every smooth v, exactly when it solves L_g u = λ |u| ^ (pₙ - 2) u for some constant λ.

    The Euler–Lagrange equation for nonnegative functions. On a closed manifold of dimension n > 2, a nonzero nonnegative C² function u is a critical point of the Yamabe quotient exactly when it solves the Yamabe equation L_g u = λ u ^ (pₙ - 1) for some constant λ.