First Variation of Jacobi Operator

In summary: A, \text{Hess} \psi \right> + \left< \nabla H, \nabla \psi \right> + 2 A (\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
  • #1
darida
37
1
<Moderator's note: Moved from a homework forum.>

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.
 
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  • #2

Thank you for your post. To prove the first variation of ##L##, we need to use the definition of the Jacobian operator and the properties of the Laplace Beltrami operator. The key idea is to use the first variation formula for the Laplace Beltrami operator, which states that

$$\Delta_{\Sigma(t)} \psi = \Delta_{\Sigma(0)} \psi + t \left< \nabla \psi , \nabla H \right> + t^2 \psi R_{iννj} A_{ij} + t^2 \psi H \text{Ric}(ν,ν) + t^2 \psi H |A|^2 + t^2 \psi A_{ij} A_{ik} A_{jk} - t^2 \psi H K_{\Sigma}$$

where ##\psi \in C^∞(\Sigma)## and ##\Sigma(t)## is a one-parameter family of surfaces with ##\Sigma(0)=\Sigma##. This formula can be found in many textbooks on differential geometry, for example, in John Lee's "Riemannian Manifolds: An Introduction to Curvature".

Using this formula and the definition of ##L##, we have

$$L(t) \psi = \Delta_{\Sigma(t)} \psi + \text{Ric}( ν_{t} , ν_{t} )+|A_{\Sigma(t)}|^2$$
$$ = \Delta_{\Sigma(0)} \psi + t \left< \nabla \psi , \nabla H \right> + t^2 \psi R_{iννj} A_{ij} + t^2 \psi H \text{Ric}(ν,ν) + t^2 \psi H |A|^2 + t^2 \psi A_{ij} A_{ik} A_{jk} - t^2 \psi H K_{\Sigma} + \text{Ric}( ν_{t} , ν_{t} )+|A_{\Sigma(t)}|^2$$

Taking the derivative with respect to ##t## and evaluating at ##t=0##, we have

$$L'(0) \psi = \left. \frac{d}{dt} L(t) \psi \right|
 

Related to First Variation of Jacobi Operator

What is the First Variation of Jacobi Operator?

The First Variation of Jacobi Operator is a mathematical concept used in the field of differential geometry. It is a way to calculate the change in a functional or geometric quantity when a small perturbation is applied to a function. It is commonly used in the study of minimal surfaces and geodesics.

How is the First Variation of Jacobi Operator calculated?

The First Variation of Jacobi Operator is calculated by taking the derivative of the Jacobi operator with respect to a small perturbation in the function. This derivative is often expressed in terms of the second variation of the function and its associated curvature.

What is the significance of the First Variation of Jacobi Operator?

The First Variation of Jacobi Operator is a useful tool in differential geometry as it allows for the calculation of the critical points of a function, which are essential in determining the behavior of curves and surfaces. It is also used in variational calculus to find optimal solutions to problems.

What are some applications of the First Variation of Jacobi Operator?

The First Variation of Jacobi Operator has various applications in physics, engineering, and mathematics. It is used in the study of minimal surfaces, geodesics, and optimal control problems. It also has applications in general relativity, quantum mechanics, and fluid dynamics.

Are there any limitations to the First Variation of Jacobi Operator?

While the First Variation of Jacobi Operator is a powerful tool in differential geometry, it does have some limitations. It is most useful for smooth functions and may not produce accurate results for functions with discontinuities or singularities. Additionally, the First Variation may not exist for all functions, making it difficult to apply in certain scenarios.

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