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Surfaces in R 4 with constant principal angles with respect to a - - PowerPoint PPT Presentation

Surfaces in R 4 with constant principal angles with respect to a plane Gabriel Ruiz Hern andez (Joint work with P . Bayard, A. Di Scala y O. Osuna) Instituto de Matem aticas, UNAM, Mexico PADGE 2012 Leuven, Belgium August 27 2012


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“Surfaces in R4 with constant principal angles with respect to a plane”

Gabriel Ruiz Hern´ andez

(Joint work with P . Bayard, A. Di Scala y O. Osuna)

Instituto de Matem´ aticas, UNAM, Mexico

PADGE 2012 Leuven, Belgium August 27 2012

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Summary: Surfaces in R4 with constant principal angles Published in Geom. Dedicata 2012

We study surfaces in R4 whose tangent spaces have constant principal angles with respect to a plane. We classify all surfaces with one principal angle equal to 0. We also classify the complete constant angle surfaces in R4 with respect to a plane. They turn out to be extrinsic products. The existence of such surfaces turns out to be equivalent to the existence of a special local symplectomorphism of R2. Using a PDE we prove the existence of surfaces with arbitrary constant principal angles.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Linear Algebra of Principal Angles

Camille Jordan defined the concept of principal angles between two linear subspaces of the Euclidean space. The principal angles are real numbers between 0 and π

2 which gives a

description of the mutual position of two subspaces. If one subspace has dimension one, the principal angle is just the usual angle between a straight line and a subspace. When both subspaces have dimension two, its principal angles consist of two real numbers 0 ≤ θ1 ≤ θ2 ≤ π

2.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Principal Angles

Definition Let V and W be two-dimensional subspaces of R4. The principal angles between V and W, 0 ≤ θ1 ≤ θ2 ≤ π/2, are given by cos θ1 := v1, w1 := max{v, w|v ∈ V, w ∈ W, |v| = |w| = 1}, cos θ2 := v2, w2 := max{v, w|v ∈ V, w ∈ W, v ⊥ v1, w ⊥ w1, |v| = |w| = 1}.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Surface with principal angles

Definition Let Σ be an immersed surface in R4 and let Π ⊂ R4 be a two-dimensional plane. We say that Σ is a helix surface or a constant principal angles surface with respect to Π, if the principal angles between TpM and W do not depend on p ∈ Σ. We will say that Σ has constant principal angles with respect to plane Π. Example (The flat torus is a helix surface) Let us consider the flat torus in R4: T 2 = S1 × S1 ⊂ R2 × R2 = R4 with its Riemannian product metric induced from the ambient. T 2 is a helix surface with respect to the plane Π12 = {(x1, x2, x3, x4) ∈ R4|x3 = x4 = 0}.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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The work of Franki Dillen and Daniel Kowalczyk

We classify all the surfaces in M2(c1) × M2(c2) for which the tangent space TpM2 makes constant angles with Tp(M2(c1) × p2) (or equivalently with Tp(p1 × M2(c2)) for every point p = (p1, p2) of M2. Here M2(c1) and M2(c2) are 2-dimensional space forms, not both flat. As a corollary we give a classification of all the totally geodesic surfaces in M2(c1) × M2(c2).

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Principal Angles of Compact surfaces

Lema Let Σ2 ⊂ R4 be a compact immersed surface. Let Π be any two dimensional plane in R4. Then there exist p ∈ Σ, depending on Π, such that TpM and Π have a principal angle equal to zero. Proposition If Σ is an immersed compact helix surface in R4 with respect to a plane Π, then it has constant principal angles equal to zero and π/2. That means that its Gauss map image is a product of two equators in S2( √ 2/2) × S2( √ 2/2).

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Example II

Example A helix in R4 which is full and is not a Riemannian product of two curves. Let Π be a two dimensional subspace of R4 and let G the group

  • f all isometries of R4 that fixes pointwise Π. So, G is

isomorphic to the group SO(2). Let γ be a connected regular curve in R4, whose tangent lines makes a constant angle with the plane Π. We define an immersed surface Σ in R4 by taking Σ := G · γ, the orbit of γ under the action of G.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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... Example II

Example Let us observe that Σ is foliated by its geodesics g · γ, for every g ∈ G. The other curves: G · p for every p ∈ γ (these curves are planar circles in R4) are orthogonal to such family of geodesics in Σ. Let us observe that the geodesics on Σ given by g · γ have the same property as the original γ: Their tangent lines make the same constant angle with respect to plane Π, because G consist of isometries in R4 that fixes pointwise Π.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Structure Equations

Let Σ ⊂ R4 be a surface with constant principal angles with respect to the plane Π ⊂ R4. Let T1, T2 ∈ Γ(TΣ) be the unit principal vectors and let e1, e2 the corresponding frame of Π. Namely, e1 = cos(θ1)T1 + sin(θ1)ξ1 , e2 = cos(θ2)T2 + sin(θ2)ξ2 where Π = span{e1, e2} and ξ1, ξ2 are normal vector fields. Let X be a vector field of Σ. By taking derivatives in both hands: DXe1 = cos(θ1)DXT1 + sin(θ1)DXξ1 = = cos(θ1)∇XT1 − sin(θ1)Aξ1(X) + cos(θ1)α(X, T1) + sin(θ1)∇⊥

X ξ1

and DXe2 = cos(θ2)DXT2 + sin(θ2)DXξ2 = = cos(θ2)∇XT2 − sin(θ2)Aξ2(X) + cos(θ2)α(X, T2) + sin(θ2)∇⊥

X ξ2

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Structure Equations II

DXe1 = df(X)e2 , DXe2 = −df(X)e1 . By taking the normal and tangent components we get cos(θ2)df(X)T2 = cos(θ1)∇XT1 − sin(θ1)Aξ1(X) , − cos(θ1)df(X)T1 = cos(θ2)∇XT2 − sin(θ2)Aξ2(X) (1) sin(θ2)df(X)ξ2 = cos(θ1)α(X, T1) + sin(θ1)∇⊥

X ξ1 ,

− sin(θ1)df(X)ξ1 = cos(θ2)α(X, T2) + sin(θ2)∇⊥

X ξ2

(2)

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Helix are flat and normal flat

Lema The Levi-Civita connection and the normal connection are flat. Proof. Indeed, from above equations it follows α(T1, T2) = 0 and α(T1, T1) ⊥ α(T2, T2) . Now the first claim follows from Gauss equation and the second from the Ricci equation.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Principal Direction

Then with respect to the frame T1, T2 we have Aξ1 = m1

  • Aξ2 =

m2

  • α(T1, T1) = m2ξ2,

α(T2, T2) = m1ξ1

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Caracterizations of complete helix surfaces

Theorem Assume Σ ⊂ R4 with constant principal angles and 0 < θ1 < θ2 < π

2 to be complete. Then Σ is totally geodesic.

Theorem Assume Σ ⊂ R4 with constant principal angles θ1 = 0 to be complete and not totally geodesic. Then T1, T2 are parallel vector fields and Σ is an extrinsic product.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Existence

Existence of surfaces Σ2 ⊂ R4 with constant principal angles θ1, θ2 ∈ (0, π

2). Locally Σ2 can be regarded as a graph of a

function F : Π → Π. F(x, y) = (f(x, y), g(x, y)). That is to say, Σ2 ⊂ R4 is locally given parametrically by (x, y) → (x, y, f(x, y), g(x, y)). The metric tensor , restricted to Σ2 in coordinates (x, y). E := ∂x, ∂x = 1 + f 2

x + g2 x

F := ∂x, ∂y = fxfy + gxgy G := ∂y, ∂y = 1 + f 2

y + g2 y.

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The Metric of a helix has constant eigenvalues

Proposition Let PF(x, y) = (x, y, f(x, y), g(x, y)) be the parametrization of surface Σ2 ⊂ R4. Then Σ2 has constant principal angles with respect to the plane Π = span(e1, e2) if and only if the matrix tensor E F F G

  • has constant eigenvalues.

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Metric Vs Principal Angles

Proposition Let PF(x, y) = (x, y, f(x, y), g(x, y)) be the parametrization of a surface Σ2 ⊂ R4. Then Σ2 has constant principal angles θ1, θ2 with respect to the plane Π = span(e1, e2) if and only if E + G = sec2(θ1) + sec2(θ2) EG − F2 = sec2(θ1) sec2(θ2) Since EG − F2 = 1 + f 2

x + g2 x + f 2 y + g2 y + (fxgy − fygx)2.

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The PDE system

In order to show the existence of surfaces with principal curvatures we have to solve the following PDE system:        2 + f 2

x + g2 x + f 2 y + g2 y

= sec2(θ1) + sec2(θ2) (fxgy − fygx)2 = sec2(θ1) sec2(θ2) + 1 − sec2(θ1) − sec2(θ2) = tan2(θ1) tan2(θ2) By taking square root we get the equivalent system with the next two equations: f 2

x + g2 x + f 2 y + g2 y

= c1 := sec2(θ1) + sec2(θ2) − 2, fxgy − fygx = c2 := tan(θ1) tan(θ2)

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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Finding the PDE

Then from the second equation there exists a function λ such that gx =

−fy+λfx f 2

x +f 2 y ,

gy =

fx+λfy f 2

x +f 2 y .

By using the first equation it follows that λ satisfies: 1 + (f 2

x + f 2 y )2 + λ2

f 2

x + f 2 y

= c1 . Set ∆ := f 2

x + f 2 y . Then λ satisfies

λ2 = c1∆ − 1 − ∆2 .

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles

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f is a solution of the following second order quasi-linear PDE: (−fy +

  • c1∆ − 1 − ∆2fx

∆ )y = (fx +

  • c1∆ − 1 − ∆2fy

∆ )x, (3) where ∆ := f 2

x + f 2 y .

Reciprocally, if f is a non lineal solution of the above equation then it is possible to construct g such that F(x, y) = (f(x, y), g(x, y)) is a (non linear) symplectomorphism whose Jacobian matrix has constant length.

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Proposition A non totally geodesic surface with constant principal angles do exists if and only if there exists a non linear local symplectomorphism of R2 whose Jacobian matrix has constant length. Proof. Assume that such surface do exists and set ψ(x, y) := (

f √c2 , g √c2 ). Then the above system imply that ψ is a

non linear local symplectomorphism of R2 whose Jacobian matrix has constant length. The converse follows from the above equivalences.

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Theorem Let Lf = 0 be a second order quasi-linear equation with analytic coefficients. Namely, Lf = A(fx, fy)fxx + B(fx, fy)fxy + C(fx, fy)fyy + E(fx, fy) = 0 , where A, B, C, E are real analytic functions defined in some

  • pen subset Ω ⊂ R2.

Then there exists a non linear solution f : D ⊂ R2 → R, i.e. there exists a function f with non constant gradient such that Lf = 0.

Gabriel Ruiz Hern´ andez Surfaces in R4 with constant principal angles