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.
yamabeQuotient: the Yamabe quotientQ_g(u).yamabeQuotient_nonneg_of_scalarCurvature_nonneg: nonnegative scalar curvature gives nonnegative quotients, without regularity assumptions onu.yamabeQuotient_smul:Q_g(c u) = Q_g(u)forc ≠ 0.yamabeQuotient_one: on a compact manifold,Q_g(1) = (∫ Scal_g dV_g) / Vol(g) ^ (2 / pₙ).hasDerivAt_yamabeQuotient_add_smul: the first variation ofQ_g.forall_hasDerivAt_yamabeQuotient_add_smul_iff_exists_conformalLaplacian_eq: the Euler–Lagrange equationL_g u = λ |u| ^ (pₙ - 2) ucharacterizes the critical points ofQ_g.forall_hasDerivAt_yamabeQuotient_add_smul_iff_exists_conformalLaplacian_eq_of_nonneg: foru ≥ 0it is the Yamabe equationL_g u = λ u ^ (pₙ - 1).yamabeQuotient_eq_of_conformalLaplacian_eq: a solution of the Euler–Lagrange equation hasQ_g(u) = λ N(u) ^ (1 - 2 / pₙ), andyamabeQuotient_eq_of_conformalLaplacian_eq_of_integral_eq_one:Q_g(u) = λat unit norm.
References #
- J. M. Lee and T. H. Parker, The Yamabe problem, Bull. Amer. Math. Soc. 17 (1987), §2 (the Yamabe functional, its Euler–Lagrange equation and the identification of the multiplier).
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
Unfolding lemma for TauCeti.Yamabe.yamabeQuotient.
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.
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.