- #1
darida
- 37
- 1
<Moderator's note: Moved from a homework forum.>
From this paper.
Let ##L## be the Jacobian operator of a two-sided compact surface embedded in a three-maniold ##(M,g)##, ##\Sigma \subset M##, and defined by
$$L(t)=\Delta_{\Sigma(t)}+ \text{Ric}( ν_{t} , ν_{t} )+|A_{\Sigma(t)}|^2$$
where
##\Delta## is the Laplace Beltrami operator on ##\Sigma##
##\text{Ric}## is the Ricci tensor of three-manifold ##M##
##|A_{\Sigma(t)}|^2## is the traceless part of the second fundamental form ##A_{ij}## of ##\Sigma## in ##M##
$$|A_{\Sigma(t)}|^2=A^{ij}A_{ij}$$
Now, for each function ##\psi \subset C^∞(\Sigma)##, the first variation of ##L## could be calculated as (Proposition 6.2 page 16):
$$L'(0)\psi = 2 \phi \left< A, \text{Hess} \psi \right> + 2\psi \left< A, \text{Hess} \phi \right> - 2 \phi \omega (\nabla \psi) - 2 \psi \omega (\nabla \phi) $$
$$ + \phi \left< \nabla H, \nabla \psi \right> - H \left< \nabla \phi , \nabla \psi \right> + 2A (\nabla \phi , \nabla \psi) - \psi \text{div}_{\Sigma} ( \text{div}_{\Sigma} \omega ) $$
$$ +\phi \psi R_{iννj} A_{ij} + \phi \psi H \text{Ric}(ν,ν) + \phi \psi H |A|^2 + \phi \psi A_{ij} A_{ik} A_{jk} - \phi \psi H K_{\Sigma}$$
where
##\omega## is the 1-form on ##\Sigma## defined by ##\omega(X)=\text{Ric}(X,ν)##
##K_{\Sigma}## the Gauss curvature of ##\Sigma##
Page 17-18.
If we consider the particular case where ##(M,g)## is the deSitter-Schwarzschild manifold ##(\mathbb R \times \mathbb S^2, g_a)## and ##\Sigma \subset M## is some slice ##{r} \times \mathbb S^2##. In this case, we have
##R## is constant equal to 2;
##\Sigma## is totally umbilic and has constant Gauss curvature, ##K_{\Sigma}=\frac{4\pi}{| \Sigma |}##;
##\omega = 0##.
Therefore, the first variation of ##L## becomes (page 18):
$$L'(0)\phi = 2 H\phi \Delta \phi + \frac{3}{2} H \left( \text{Ric}(ν,ν) + \frac{H^2}{2} \right) \phi^2 - \frac{4\pi}{| \Sigma|} H \phi^2$$
where ##|A|^2 = \frac{H^2}{2}##, since ##\Sigma## is umbilic.
How to prove this ##L'(0)\phi##?
How come the other terms vanish?
I have tried, but this is what I get
$$L'(0)\psi = 4 \phi \left< A, \text{Hess} \phi \right> + \phi \left< \nabla H, \nabla \phi \right> - H (\nabla \phi)^2 + 2A (\nabla \phi)^2 $$
$$ +\phi^2 R_{iννj} A_{ij} + \phi^2 H \left( \text{Ric}(ν,ν) + \frac{H^2}{2} \right) + \phi^2 A_{ij} A_{ik} A_{jk} - \frac{4\pi}{| \Sigma|} H \phi^2$$
Could someone please give me the detail steps to get ##L'(0)\phi## (page 18)? Thank you.
Homework Statement
From this paper.
Let ##L## be the Jacobian operator of a two-sided compact surface embedded in a three-maniold ##(M,g)##, ##\Sigma \subset M##, and defined by
$$L(t)=\Delta_{\Sigma(t)}+ \text{Ric}( ν_{t} , ν_{t} )+|A_{\Sigma(t)}|^2$$
where
##\Delta## is the Laplace Beltrami operator on ##\Sigma##
##\text{Ric}## is the Ricci tensor of three-manifold ##M##
##|A_{\Sigma(t)}|^2## is the traceless part of the second fundamental form ##A_{ij}## of ##\Sigma## in ##M##
$$|A_{\Sigma(t)}|^2=A^{ij}A_{ij}$$
Now, for each function ##\psi \subset C^∞(\Sigma)##, the first variation of ##L## could be calculated as (Proposition 6.2 page 16):
$$L'(0)\psi = 2 \phi \left< A, \text{Hess} \psi \right> + 2\psi \left< A, \text{Hess} \phi \right> - 2 \phi \omega (\nabla \psi) - 2 \psi \omega (\nabla \phi) $$
$$ + \phi \left< \nabla H, \nabla \psi \right> - H \left< \nabla \phi , \nabla \psi \right> + 2A (\nabla \phi , \nabla \psi) - \psi \text{div}_{\Sigma} ( \text{div}_{\Sigma} \omega ) $$
$$ +\phi \psi R_{iννj} A_{ij} + \phi \psi H \text{Ric}(ν,ν) + \phi \psi H |A|^2 + \phi \psi A_{ij} A_{ik} A_{jk} - \phi \psi H K_{\Sigma}$$
where
##\omega## is the 1-form on ##\Sigma## defined by ##\omega(X)=\text{Ric}(X,ν)##
##K_{\Sigma}## the Gauss curvature of ##\Sigma##
Homework Equations
Page 17-18.
If we consider the particular case where ##(M,g)## is the deSitter-Schwarzschild manifold ##(\mathbb R \times \mathbb S^2, g_a)## and ##\Sigma \subset M## is some slice ##{r} \times \mathbb S^2##. In this case, we have
##R## is constant equal to 2;
##\Sigma## is totally umbilic and has constant Gauss curvature, ##K_{\Sigma}=\frac{4\pi}{| \Sigma |}##;
##\omega = 0##.
Therefore, the first variation of ##L## becomes (page 18):
$$L'(0)\phi = 2 H\phi \Delta \phi + \frac{3}{2} H \left( \text{Ric}(ν,ν) + \frac{H^2}{2} \right) \phi^2 - \frac{4\pi}{| \Sigma|} H \phi^2$$
where ##|A|^2 = \frac{H^2}{2}##, since ##\Sigma## is umbilic.
How to prove this ##L'(0)\phi##?
How come the other terms vanish?
The Attempt at a Solution
I have tried, but this is what I get
$$L'(0)\psi = 4 \phi \left< A, \text{Hess} \phi \right> + \phi \left< \nabla H, \nabla \phi \right> - H (\nabla \phi)^2 + 2A (\nabla \phi)^2 $$
$$ +\phi^2 R_{iννj} A_{ij} + \phi^2 H \left( \text{Ric}(ν,ν) + \frac{H^2}{2} \right) + \phi^2 A_{ij} A_{ik} A_{jk} - \frac{4\pi}{| \Sigma|} H \phi^2$$
Could someone please give me the detail steps to get ##L'(0)\phi## (page 18)? Thank you.