K-surfaces with free boundaries Hayk Aleksanyan KTH Royal Institute - - PowerPoint PPT Presentation

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K-surfaces with free boundaries Hayk Aleksanyan KTH Royal Institute - - PowerPoint PPT Presentation

K-surfaces with free boundaries Hayk Aleksanyan KTH Royal Institute of Technology May 31, 2017 joint work with Aram Karakhanyan (University of Edinburgh) 1/25 Hayk Aleksanyan K-surfaces with free boundaries What is a K-surface? 2/25 Hayk


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K-surfaces with free boundaries

Hayk Aleksanyan

KTH Royal Institute of Technology

May 31, 2017 joint work with Aram Karakhanyan (University of Edinburgh)

Hayk Aleksanyan K-surfaces with free boundaries

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What is a K-surface?

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What is a K-surface?

Definition A smooth compact hypersurface in Rd+1 (d ≥ 2) having constant Gauss curvature K.

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What is a K-surface?

Definition A smooth compact hypersurface in Rd+1 (d ≥ 2) having constant Gauss curvature K. If NO boundary, then a K-surface (K > 0) bounds a convex body.

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What is a K-surface?

Definition A smooth compact hypersurface in Rd+1 (d ≥ 2) having constant Gauss curvature K. If NO boundary, then a K-surface (K > 0) bounds a convex body. The central question How does the boundary of a K-surface look like?

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What is a K-surface?

Definition A smooth compact hypersurface in Rd+1 (d ≥ 2) having constant Gauss curvature K. If NO boundary, then a K-surface (K > 0) bounds a convex body. The central question How does the boundary of a K-surface look like? Precisely, given a disjoint collection Γ = {Γ1, ..., Γm} of codimension 2 submanifolds of Rd+1, decide if there exists a K-surface of Rd+1 (in general immersed) having Γ as its boundary.

Hayk Aleksanyan K-surfaces with free boundaries

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What is a K-surface?

Definition A smooth compact hypersurface in Rd+1 (d ≥ 2) having constant Gauss curvature K. If NO boundary, then a K-surface (K > 0) bounds a convex body. The central question How does the boundary of a K-surface look like? Precisely, given a disjoint collection Γ = {Γ1, ..., Γm} of codimension 2 submanifolds of Rd+1, decide if there exists a K-surface of Rd+1 (in general immersed) having Γ as its boundary. S.-T. Yau, Problem N26, of his list of open problems ’90 What conditions should be imposed on a Jordan curve in R3 so that it can be a boundary of a disk with a given metric of positive curvature?

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Boundary of a K-surface: necessary conditions

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points.

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points. In higher dimensions, the analogue is that the second fundamental form does not degenerate.

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points. In higher dimensions, the analogue is that the second fundamental form does not degenerate. (H. Rosenberg, ’93) there are topological obstructions: the self-linking number of Γ must be 0.

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points. In higher dimensions, the analogue is that the second fundamental form does not degenerate. (H. Rosenberg, ’93) there are topological obstructions: the self-linking number of Γ must be 0. NOT a sufficient condition, [H. Gluck and L. Pan, ’98]

Hayk Aleksanyan K-surfaces with free boundaries

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points. In higher dimensions, the analogue is that the second fundamental form does not degenerate. (H. Rosenberg, ’93) there are topological obstructions: the self-linking number of Γ must be 0. NOT a sufficient condition, [H. Gluck and L. Pan, ’98] (M. Ghomi; JDG ’17) the torsion of any closed curve in R3 bounding a simply connected locally convex surface vanishes at least 4 times

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Boundary of a K-surface: necessary conditions

In R3 if the curve Γ bounds a K-surface, with K > 0, then Γ is free of inflection points. In higher dimensions, the analogue is that the second fundamental form does not degenerate. (H. Rosenberg, ’93) there are topological obstructions: the self-linking number of Γ must be 0. NOT a sufficient condition, [H. Gluck and L. Pan, ’98] (M. Ghomi; JDG ’17) the torsion of any closed curve in R3 bounding a simply connected locally convex surface vanishes at least 4 times

answers a question of H. Rosenberg from 1993 is a far reaching extension of the classical 4-vertex theorem, in particular extends the 4-vertex theorem of V.D. Sedykh from 1994

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Some existence results

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Some existence results

(L. Caffarelli, L. Nirenberg, J. Spruck; CPAM 1984) If Γ ⊂ R3 is a smooth curve that projects one-to-one onto ∂Ω, for some Ω smooth, strictly convex planar domain, then Γ bounds a K-surface that is a graph over Ω provided K > 0 is small enough.

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Some existence results

(L. Caffarelli, L. Nirenberg, J. Spruck; CPAM 1984) If Γ ⊂ R3 is a smooth curve that projects one-to-one onto ∂Ω, for some Ω smooth, strictly convex planar domain, then Γ bounds a K-surface that is a graph over Ω provided K > 0 is small enough. (D. Hoffman, H. Rosenberg, J. Spruck; CPAM 1992) If C1, C2 are two closed strictly convex curves in parallel planes, such that the projection of one is strictly inside the

  • ther. Then, for K > 0 small enough, there is a K-surface

with boundary {C1, C2}.

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Some existence results

(L. Caffarelli, L. Nirenberg, J. Spruck; CPAM 1984) If Γ ⊂ R3 is a smooth curve that projects one-to-one onto ∂Ω, for some Ω smooth, strictly convex planar domain, then Γ bounds a K-surface that is a graph over Ω provided K > 0 is small enough. (D. Hoffman, H. Rosenberg, J. Spruck; CPAM 1992) If C1, C2 are two closed strictly convex curves in parallel planes, such that the projection of one is strictly inside the

  • ther. Then, for K > 0 small enough, there is a K-surface

with boundary {C1, C2}. (B. Guan, J. Spruck; Annals 1993) For each integer n > 0, there exists an embedded K-surface of genus n.

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Some existence results

(L. Caffarelli, L. Nirenberg, J. Spruck; CPAM 1984) If Γ ⊂ R3 is a smooth curve that projects one-to-one onto ∂Ω, for some Ω smooth, strictly convex planar domain, then Γ bounds a K-surface that is a graph over Ω provided K > 0 is small enough. (D. Hoffman, H. Rosenberg, J. Spruck; CPAM 1992) If C1, C2 are two closed strictly convex curves in parallel planes, such that the projection of one is strictly inside the

  • ther. Then, for K > 0 small enough, there is a K-surface

with boundary {C1, C2}. (B. Guan, J. Spruck; Annals 1993) For each integer n > 0, there exists an embedded K-surface of genus n. Further remarkable results by [B. Guan, J. Spruck; JDG 2002, 2004, M. Ghomi; JDG 2001, and other authors...]

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Can we leave part of the boundary free?

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0.

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0. K-surfaces with (Bernoulli) free boundary What conditions should be imposed on Γ, T0, and θ in order to get a K-surface spanning Γ and hitting T0 at an angle θ ?

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0. K-surfaces with (Bernoulli) free boundary What conditions should be imposed on Γ, T0, and θ in order to get a K-surface spanning Γ and hitting T0 at an angle θ ? A model case:

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0. K-surfaces with (Bernoulli) free boundary What conditions should be imposed on Γ, T0, and θ in order to get a K-surface spanning Γ and hitting T0 at an angle θ ? A model case: (The boundary) Take Γ = ∂Ω where Ω ⊂ Rd × {h0} is strictly convex, and h0 > 0.

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0. K-surfaces with (Bernoulli) free boundary What conditions should be imposed on Γ, T0, and θ in order to get a K-surface spanning Γ and hitting T0 at an angle θ ? A model case: (The boundary) Take Γ = ∂Ω where Ω ⊂ Rd × {h0} is strictly convex, and h0 > 0. (The target manifold) T0 = Rd × {0}.

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Can we leave part of the boundary free?

Fix Γ = {Γ1, ..., Γm} a collection of disjoint (d − 1)-dimensional closed smooth embedded submanifolds of Rd+1, and let T0 be a smooth embedded submanifold in Rd+1 of codimension 1. Fix also an angle θ > 0. K-surfaces with (Bernoulli) free boundary What conditions should be imposed on Γ, T0, and θ in order to get a K-surface spanning Γ and hitting T0 at an angle θ ? A model case: (The boundary) Take Γ = ∂Ω where Ω ⊂ Rd × {h0} is strictly convex, and h0 > 0. (The target manifold) T0 = Rd × {0}. (The hitting angle) θ = arccos(1 + λ0)−1/2, for some λ0 > 0.

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Our setting: formal statement

For a convex domain Ω ⊂ Rd × {0} and parameters h0, λ0 > 0, K0 ≥ 0, find a concave function u : Rd × {0} → R+ such that      detD2(−u) = K0ψ(|∇u|), in {u > 0} \ Ω, u = h0,

  • n ∂Ω,

|∇u| = λ0,

  • n Γu

where ψ > 0 is a prescribed real-valued C ∞ function, Γu = ∂{u > 0} \ Ω.

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Our setting: formal statement

For a convex domain Ω ⊂ Rd × {0} and parameters h0, λ0 > 0, K0 ≥ 0, find a concave function u : Rd × {0} → R+ such that      detD2(−u) = K0ψ(|∇u|), in {u > 0} \ Ω, u = h0,

  • n ∂Ω,

|∇u| = λ0,

  • n Γu

where ψ > 0 is a prescribed real-valued C ∞ function, Γu = ∂{u > 0} \ Ω. Geometry relevant choices: (the homogeneous equation) K0 = 0,

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Our setting: formal statement

For a convex domain Ω ⊂ Rd × {0} and parameters h0, λ0 > 0, K0 ≥ 0, find a concave function u : Rd × {0} → R+ such that      detD2(−u) = K0ψ(|∇u|), in {u > 0} \ Ω, u = h0,

  • n ∂Ω,

|∇u| = λ0,

  • n Γu

where ψ > 0 is a prescribed real-valued C ∞ function, Γu = ∂{u > 0} \ Ω. Geometry relevant choices: (the homogeneous equation) K0 = 0, (constant curvature measure) ψ ≡ 1,

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Our setting: formal statement

For a convex domain Ω ⊂ Rd × {0} and parameters h0, λ0 > 0, K0 ≥ 0, find a concave function u : Rd × {0} → R+ such that      detD2(−u) = K0ψ(|∇u|), in {u > 0} \ Ω, u = h0,

  • n ∂Ω,

|∇u| = λ0,

  • n Γu

where ψ > 0 is a prescribed real-valued C ∞ function, Γu = ∂{u > 0} \ Ω. Geometry relevant choices: (the homogeneous equation) K0 = 0, (constant curvature measure) ψ ≡ 1, (constant Gauss curvature) ψ(t) = (1 + t2)(d+2)/2

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Our setting: formal statement

For a convex domain Ω ⊂ Rd × {0} and parameters h0, λ0 > 0, K0 ≥ 0, find a concave function u : Rd × {0} → R+ such that      detD2(−u) = K0ψ(|∇u|), in {u > 0} \ Ω, u = h0,

  • n ∂Ω,

|∇u| = λ0,

  • n Γu

where ψ > 0 is a prescribed real-valued C ∞ function, Γu = ∂{u > 0} \ Ω. Geometry relevant choices: (the homogeneous equation) K0 = 0, (constant curvature measure) ψ ≡ 1, (constant Gauss curvature) ψ(t) = (1 + t2)(d+2)/2 For p-Laplace equation, see [A. Henrot and H. Shahgholian; J. Reine und Angew. Math 2000], although methods and motivation are entirely different here.

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Weak solutions (` a la A.D. Aleksandrov)

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω.

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω. The set of slopes ωx0(u) = {p ∈ Rd : u(x) ≥ u(x0) + p · (x − x0), ∀x ∈ Ω} is called the gradient mapping of u at x0.

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω. The set of slopes ωx0(u) = {p ∈ Rd : u(x) ≥ u(x0) + p · (x − x0), ∀x ∈ Ω} is called the gradient mapping of u at x0. For a set E ⊂ Ω set ωE(u) =

x∈E

ωx(u).

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω. The set of slopes ωx0(u) = {p ∈ Rd : u(x) ≥ u(x0) + p · (x − x0), ∀x ∈ Ω} is called the gradient mapping of u at x0. For a set E ⊂ Ω set ωE(u) =

x∈E

ωx(u). The Monge-Amp` ere measure We call a convex u : E → R a solution to detD2u = K0ψ(|∇u|) on E, if for any Borel set B ⊂ E one has

  • ωB(u)

dξ ψ(|ξ|) = K0|B|.

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω. The set of slopes ωx0(u) = {p ∈ Rd : u(x) ≥ u(x0) + p · (x − x0), ∀x ∈ Ω} is called the gradient mapping of u at x0. For a set E ⊂ Ω set ωE(u) =

x∈E

ωx(u). The Monge-Amp` ere measure We call a convex u : E → R a solution to detD2u = K0ψ(|∇u|) on E, if for any Borel set B ⊂ E one has

  • ωB(u)

dξ ψ(|ξ|) = K0|B|.

The l.h.s. is called the Monge-Amp` ere measure.

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Weak solutions (` a la A.D. Aleksandrov)

The gradient mapping Let u : Ω → R be convex, x0 ∈ Ω. The set of slopes ωx0(u) = {p ∈ Rd : u(x) ≥ u(x0) + p · (x − x0), ∀x ∈ Ω} is called the gradient mapping of u at x0. For a set E ⊂ Ω set ωE(u) =

x∈E

ωx(u). The Monge-Amp` ere measure We call a convex u : E → R a solution to detD2u = K0ψ(|∇u|) on E, if for any Borel set B ⊂ E one has

  • ωB(u)

dξ ψ(|ξ|) = K0|B|.

The l.h.s. is called the Monge-Amp` ere measure. The MA measure is weakly* continuous.

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The free boundary condition

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν).

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists:

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists: by concavity of u, for any t2 > t1 > 0 we get u(x0+t1ν) = u

  • 1 − t1

t2

  • x0 + t1

t2 (x0 + t2ν)

  • ≥ t1

t2 u(x0+t2ν).

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists: by concavity of u, for any t2 > t1 > 0 we get u(x0+t1ν) = u

  • 1 − t1

t2

  • x0 + t1

t2 (x0 + t2ν)

  • ≥ t1

t2 u(x0+t2ν). (Geometric reformulation) There is a unique support plane G in Rd × {0} for Γu at x0.

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists: by concavity of u, for any t2 > t1 > 0 we get u(x0+t1ν) = u

  • 1 − t1

t2

  • x0 + t1

t2 (x0 + t2ν)

  • ≥ t1

t2 u(x0+t2ν). (Geometric reformulation) There is a unique support plane G in Rd × {0} for Γu at x0. Any support hyperplane H to the graph(u) at (x0, 0) ∈ Rd × R, must pass through G.

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists: by concavity of u, for any t2 > t1 > 0 we get u(x0+t1ν) = u

  • 1 − t1

t2

  • x0 + t1

t2 (x0 + t2ν)

  • ≥ t1

t2 u(x0+t2ν). (Geometric reformulation) There is a unique support plane G in Rd × {0} for Γu at x0. Any support hyperplane H to the graph(u) at (x0, 0) ∈ Rd × R, must pass through G. Hence, there is one free parameter, the slope of H.

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The free boundary condition

Fix any regular point x0 ∈ Γu, i.e. Γu has a well-defined inner normal (call it ν). The condition |∇u(x0)| = λ0 means ∂u

∂ν (x0) = λ0, which

always exists: by concavity of u, for any t2 > t1 > 0 we get u(x0+t1ν) = u

  • 1 − t1

t2

  • x0 + t1

t2 (x0 + t2ν)

  • ≥ t1

t2 u(x0+t2ν). (Geometric reformulation) There is a unique support plane G in Rd × {0} for Γu at x0. Any support hyperplane H to the graph(u) at (x0, 0) ∈ Rd × R, must pass through G. Hence, there is one free parameter, the slope of H. The extreme H (i.e. the “most inclined on the graph”) must have slope λ0.

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The main results: homogeneous case

Theorem A (K0 = 0, the homogeneous case) Let K0 = 0, and Ω ⊂ Rd be bounded convex C 1,1-regular domain. Then, there exists a unique weak solution u.

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The main results: homogeneous case

Theorem A (K0 = 0, the homogeneous case) Let K0 = 0, and Ω ⊂ Rd be bounded convex C 1,1-regular domain. Then, there exists a unique weak solution u. Moreover the graph of u is a ruled surface, u is C 1,1 on {u > 0} \ Ω, the free boundary Γu is C 1,1, if in addition, Ω is strictly convex, then so is the free boundary.

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The main results: homogeneous case

Theorem A (K0 = 0, the homogeneous case) Let K0 = 0, and Ω ⊂ Rd be bounded convex C 1,1-regular domain. Then, there exists a unique weak solution u. Moreover the graph of u is a ruled surface, u is C 1,1 on {u > 0} \ Ω, the free boundary Γu is C 1,1, if in addition, Ω is strictly convex, then so is the free boundary. Example (truncated cone) Take Ω = B(x0, r) in Rd (d ≥ 2). Fix λ0 > 0 and h0 = 1. Then u(x) = 1 + λ0 − λ0 r |x − x0|, r ≤ |x − x0| ≤ r

  • 1 + 1

λ0

  • is the solution, with free boundary |x − x0| = r(1 + 1/λ0).

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The main results: elliptic case

Theorem B (K0 > 0, the strictly convex (elliptic) case) Let K0 > 0, and Ω ⊂ Rd be bounded strictly convex smooth

  • domain. Let also ψ : R+ → (0, ∞) be non-decreasing and smooth.

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The main results: elliptic case

Theorem B (K0 > 0, the strictly convex (elliptic) case) Let K0 > 0, and Ω ⊂ Rd be bounded strictly convex smooth

  • domain. Let also ψ : R+ → (0, ∞) be non-decreasing and smooth.

Then, there exists a small constant K = K(Ω, ψ, λ0) > 0, such that for any K0 ∈ (0, K) there exists a weak solution u, which is C ∞ on {u > 0} \ Ω and the free boundary Γu is C ∞ as well.

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The main results: elliptic case

Theorem B (K0 > 0, the strictly convex (elliptic) case) Let K0 > 0, and Ω ⊂ Rd be bounded strictly convex smooth

  • domain. Let also ψ : R+ → (0, ∞) be non-decreasing and smooth.

Then, there exists a small constant K = K(Ω, ψ, λ0) > 0, such that for any K0 ∈ (0, K) there exists a weak solution u, which is C ∞ on {u > 0} \ Ω and the free boundary Γu is C ∞ as well. On NON-existence The smallness of K0 cannot be eliminated entirely!

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 53

10/25

The main results: elliptic case

Theorem B (K0 > 0, the strictly convex (elliptic) case) Let K0 > 0, and Ω ⊂ Rd be bounded strictly convex smooth

  • domain. Let also ψ : R+ → (0, ∞) be non-decreasing and smooth.

Then, there exists a small constant K = K(Ω, ψ, λ0) > 0, such that for any K0 ∈ (0, K) there exists a weak solution u, which is C ∞ on {u > 0} \ Ω and the free boundary Γu is C ∞ as well. On NON-existence The smallness of K0 cannot be eliminated entirely! Work out the case of radial solutions (when Ω is a ball) by hand.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 54

11/25

Some ideas of the proofs: the homogeneous case

Ω Rd × {0}

X0 HX0 Y0 A scematic view for the homogeneous case.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 55

12/25

Convex polygonal domains

Let Ω ⊂ Rd × {0} be a convex polygon, and let F1, ..., Fn be the facets of Ω := Ω × {h0}.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 56

12/25

Convex polygonal domains

Let Ω ⊂ Rd × {0} be a convex polygon, and let F1, ..., Fn be the facets of Ω := Ω × {h0}. For each 1 ≤ i ≤ n let Hi be the hyperplane in Rd+1 passing through Fi and having slope λ0. Identify each Hi with the linear function.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 57

12/25

Convex polygonal domains

Let Ω ⊂ Rd × {0} be a convex polygon, and let F1, ..., Fn be the facets of Ω := Ω × {h0}. For each 1 ≤ i ≤ n let Hi be the hyperplane in Rd+1 passing through Fi and having slope λ0. Identify each Hi with the linear function. Then u(x) = inf1≤i≤n Hi(x), x ∈ Rd, solves the homogeneous problem.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 58

12/25

Convex polygonal domains

Let Ω ⊂ Rd × {0} be a convex polygon, and let F1, ..., Fn be the facets of Ω := Ω × {h0}. For each 1 ≤ i ≤ n let Hi be the hyperplane in Rd+1 passing through Fi and having slope λ0. Identify each Hi with the linear function. Then u(x) = inf1≤i≤n Hi(x), x ∈ Rd, solves the homogeneous problem. The most delicate part is to show that there is no X ∈ Rd+1 in the strip 0 < xd+1 < h0 where more than d planes meet, i.e. the graph of u has NO vertex (a geometric proof).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 59

13/25

Approximation by polygons: existence

Let Ω be bounded, convex and C 1. For each X0 ∈ Ω there is a support hyperplane HX0 in Rd+1 through X0 and having slope λ0.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 60

13/25

Approximation by polygons: existence

Let Ω be bounded, convex and C 1. For each X0 ∈ Ω there is a support hyperplane HX0 in Rd+1 through X0 and having slope λ0. Define h∗(x) = inf

X0∈∂ Ω

HX0(x), x ∈ Rd. The infimum does not collapse due to the uniform bound on the slopes.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 61

13/25

Approximation by polygons: existence

Let Ω be bounded, convex and C 1. For each X0 ∈ Ω there is a support hyperplane HX0 in Rd+1 through X0 and having slope λ0. Define h∗(x) = inf

X0∈∂ Ω

HX0(x), x ∈ Rd. The infimum does not collapse due to the uniform bound on the slopes. Approximate Ω by polygonal domains, and for each polygon take the solution constructed above. Then, the limit will converge to h∗ and will give a weak solution for the homogeneous problem (uses the weak* continuity of MA measure).

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SLIDE 62

14/25

Every weak solution is a ruled surface

Proposition (Line segments on the graph) Let u be any weak solution, and assume X0 is on the graph of u. Then, there is a line segment though X0 joining the free boundary with Rd × {h0} and lying entirely on the graph of u.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 63

14/25

Every weak solution is a ruled surface

Proposition (Line segments on the graph) Let u be any weak solution, and assume X0 is on the graph of u. Then, there is a line segment though X0 joining the free boundary with Rd × {h0} and lying entirely on the graph of u. Proof. For a weak solution u fix X0 in the interior of M := graph(u).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 64

14/25

Every weak solution is a ruled surface

Proposition (Line segments on the graph) Let u be any weak solution, and assume X0 is on the graph of u. Then, there is a line segment though X0 joining the free boundary with Rd × {h0} and lying entirely on the graph of u. Proof. For a weak solution u fix X0 in the interior of M := graph(u). Fix a support hyperplane Π to M through X0, and define X := Hull(Π ∩ M); we need to see that X intersects the h0- and 0-level surfaces of u.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 65

14/25

Every weak solution is a ruled surface

Proposition (Line segments on the graph) Let u be any weak solution, and assume X0 is on the graph of u. Then, there is a line segment though X0 joining the free boundary with Rd × {h0} and lying entirely on the graph of u. Proof. For a weak solution u fix X0 in the interior of M := graph(u). Fix a support hyperplane Π to M through X0, and define X := Hull(Π ∩ M); we need to see that X intersects the h0- and 0-level surfaces of u. Assume NOT, then we can squeeze a strictly convex surface “between” Π and M (using “smoothing of polytopes” after

  • M. Ghomi), violating the condition detD2u = 0.

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SLIDE 66

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Every weak solution is a ruled surface

Proposition (Line segments on the graph) Let u be any weak solution, and assume X0 is on the graph of u. Then, there is a line segment though X0 joining the free boundary with Rd × {h0} and lying entirely on the graph of u. Proof. For a weak solution u fix X0 in the interior of M := graph(u). Fix a support hyperplane Π to M through X0, and define X := Hull(Π ∩ M); we need to see that X intersects the h0- and 0-level surfaces of u. Assume NOT, then we can squeeze a strictly convex surface “between” Π and M (using “smoothing of polytopes” after

  • M. Ghomi), violating the condition detD2u = 0.

The case when X0 ∈ ∂ Ω ∪ Γu follows by approximation.

Hayk Aleksanyan K-surfaces with free boundaries

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15/25

Comparison principle

Proposition Let Ω1 ⊂ Ω2 be convex domains, and let a concave function ui be a weak solutions for Ωi, i = 1, 2. Define ωi := Hull(Γi). Then

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 68

15/25

Comparison principle

Proposition Let Ω1 ⊂ Ω2 be convex domains, and let a concave function ui be a weak solutions for Ωi, i = 1, 2. Define ωi := Hull(Γi). Then if either of Γi is C 1, then ω1 ⊂ ω2,

Hayk Aleksanyan K-surfaces with free boundaries

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15/25

Comparison principle

Proposition Let Ω1 ⊂ Ω2 be convex domains, and let a concave function ui be a weak solutions for Ωi, i = 1, 2. Define ωi := Hull(Γi). Then if either of Γi is C 1, then ω1 ⊂ ω2, if either of ui is C 1 in {ui > 0} \ Ω, then U1 ≤ U2, where Ui is the extension of ui into Ωi as identically h0.

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SLIDE 70

15/25

Comparison principle

Proposition Let Ω1 ⊂ Ω2 be convex domains, and let a concave function ui be a weak solutions for Ωi, i = 1, 2. Define ωi := Hull(Γi). Then if either of Γi is C 1, then ω1 ⊂ ω2, if either of ui is C 1 in {ui > 0} \ Ω, then U1 ≤ U2, where Ui is the extension of ui into Ωi as identically h0.

  • Proof. Argue by contradiction, and use the existence of line

segments on the graphs. .

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SLIDE 71

16/25

Regularity of a weak solution and free boundary

Proposition Let Ω be bounded convex C 1,1-regular domain, and let h∗(x) = infX0∈∂

Ω HX0(x), x ∈ Rd. Then, Γh∗ is C 1,1 and h∗ is C 1,1

in Rd \ Ω.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 72

16/25

Regularity of a weak solution and free boundary

Proposition Let Ω be bounded convex C 1,1-regular domain, and let h∗(x) = infX0∈∂

Ω HX0(x), x ∈ Rd. Then, Γh∗ is C 1,1 and h∗ is C 1,1

in Rd \ Ω. The proof: follow the shared line segment. Ω Rd × {0}

X0 HX0 Y0

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 73

17/25

Uniqueness and strict convexity

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 74

17/25

Uniqueness and strict convexity

If Ω is C 1,1, then h∗ is C 1,1, and has C 1,1 free boundary.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 75

17/25

Uniqueness and strict convexity

If Ω is C 1,1, then h∗ is C 1,1, and has C 1,1 free boundary. Then, any weak solution can be compared with h∗, hence the uniqueness.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 76

17/25

Uniqueness and strict convexity

If Ω is C 1,1, then h∗ is C 1,1, and has C 1,1 free boundary. Then, any weak solution can be compared with h∗, hence the uniqueness. Strict convexity of h∗ follows by comparison with conical solutions. A quantitative version of strict convexity follows from Blaschke inclusion principle and comparison of the solution with conical barriers (from above).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 77

18/25

Elliptic case, K0 > 0, the strategy

(The class of super-solutions ) concave functions u ∈ W+(K0, λ0, Ω) s.t. u = h0 on ∂Ω and detD2(−u) ≥ K0ψ(|∇u|) on {u > 0}\Ω and |∇u| ≤ λ0 on Γu.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 78

18/25

Elliptic case, K0 > 0, the strategy

(The class of super-solutions ) concave functions u ∈ W+(K0, λ0, Ω) s.t. u = h0 on ∂Ω and detD2(−u) ≥ K0ψ(|∇u|) on {u > 0}\Ω and |∇u| ≤ λ0 on Γu. Show that W+ = ∅ (by construction, an envelope of certain paraboloids).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 79

18/25

Elliptic case, K0 > 0, the strategy

(The class of super-solutions ) concave functions u ∈ W+(K0, λ0, Ω) s.t. u = h0 on ∂Ω and detD2(−u) ≥ K0ψ(|∇u|) on {u > 0}\Ω and |∇u| ≤ λ0 on Γu. Show that W+ = ∅ (by construction, an envelope of certain paraboloids). (Perron’s method) Show that there is a minimal element in W+, and that it solves the problem. The free boundary condition is the most delicate part (is being handled by a special type of extension, which we named Blaschke extension).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 80

18/25

Elliptic case, K0 > 0, the strategy

(The class of super-solutions ) concave functions u ∈ W+(K0, λ0, Ω) s.t. u = h0 on ∂Ω and detD2(−u) ≥ K0ψ(|∇u|) on {u > 0}\Ω and |∇u| ≤ λ0 on Γu. Show that W+ = ∅ (by construction, an envelope of certain paraboloids). (Perron’s method) Show that there is a minimal element in W+, and that it solves the problem. The free boundary condition is the most delicate part (is being handled by a special type of extension, which we named Blaschke extension). (For smoothness of the free boundary) extend the solution beyond the free boundary, to reduce the matters to interior case.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 81

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 82

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 83

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one). If x0 ∈ ∂Ω is fixed, and the ball B = B(z0, r0) touches Ω at x0 and Ω ⊂ B, then the paraboloid P(x) = h0 + αr2

0 − α|x − z0|2

(with a properly chosen α > 0) satisfies

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 84

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one). If x0 ∈ ∂Ω is fixed, and the ball B = B(z0, r0) touches Ω at x0 and Ω ⊂ B, then the paraboloid P(x) = h0 + αr2

0 − α|x − z0|2

(with a properly chosen α > 0) satisfies

P(x0) = h0 and P(x) ≥ h0 on Ω,

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 85

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one). If x0 ∈ ∂Ω is fixed, and the ball B = B(z0, r0) touches Ω at x0 and Ω ⊂ B, then the paraboloid P(x) = h0 + αr2

0 − α|x − z0|2

(with a properly chosen α > 0) satisfies

P(x0) = h0 and P(x) ≥ h0 on Ω, detD2(−P) ≥ K0ψ(|∇P|) on {P > 0}.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 86

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one). If x0 ∈ ∂Ω is fixed, and the ball B = B(z0, r0) touches Ω at x0 and Ω ⊂ B, then the paraboloid P(x) = h0 + αr2

0 − α|x − z0|2

(with a properly chosen α > 0) satisfies

P(x0) = h0 and P(x) ≥ h0 on Ω, detD2(−P) ≥ K0ψ(|∇P|) on {P > 0}. |∇P| ≤ λ0 on ∂{P > 0}.

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SLIDE 87

19/25

Construction of super-solution

Assumptions: Ω is bounded, strictly convex and C 2, ψ is non-decreasing (need to adjust the free boundary condition) and smooth. Let κ0 > 0 be the smallest principal curvature of ∂Ω. Then, Ω rolls freely inside a ball of radius r0 := 1/κ0 (W. Blaschke’s rolling ball theorem (2d case), and [J. Rauch, JDG, 1974] for d > 2). (Intuition: A “more curved” fits inside the “less curved” one). If x0 ∈ ∂Ω is fixed, and the ball B = B(z0, r0) touches Ω at x0 and Ω ⊂ B, then the paraboloid P(x) = h0 + αr2

0 − α|x − z0|2

(with a properly chosen α > 0) satisfies

P(x0) = h0 and P(x) ≥ h0 on Ω, detD2(−P) ≥ K0ψ(|∇P|) on {P > 0}. |∇P| ≤ λ0 on ∂{P > 0}.

Do this for a dense set of points, and take the infimum: gives an element of W+.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 88

20/25

Perron in action

Any element of W+ is larger than the solution to the homogeneous equation. Hence, u∗(x) := inf

w∈W+ w(x), x ∈ Rd,

does not collapse.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 89

20/25

Perron in action

Any element of W+ is larger than the solution to the homogeneous equation. Hence, u∗(x) := inf

w∈W+ w(x), x ∈ Rd,

does not collapse. Show an existence of a minimizing sequence, and hence u∗ ∈ W+ (plus strict concavity of u∗).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 90

20/25

Perron in action

Any element of W+ is larger than the solution to the homogeneous equation. Hence, u∗(x) := inf

w∈W+ w(x), x ∈ Rd,

does not collapse. Show an existence of a minimizing sequence, and hence u∗ ∈ W+ (plus strict concavity of u∗). Solving the Dirichlet problem for affine boundary data, and using strong comparison principle, show u∗ solves the equation in {u∗ > 0} \ Ω.

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 91

20/25

Perron in action

Any element of W+ is larger than the solution to the homogeneous equation. Hence, u∗(x) := inf

w∈W+ w(x), x ∈ Rd,

does not collapse. Show an existence of a minimizing sequence, and hence u∗ ∈ W+ (plus strict concavity of u∗). Solving the Dirichlet problem for affine boundary data, and using strong comparison principle, show u∗ solves the equation in {u∗ > 0} \ Ω. Still need to show that |∇u∗| = λ0 on the free boundary (we have only ≤ everywhere by construction).

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 92

21/25

Blaschke extension and the free boundary condition

Rd × {0} Hx0 H⊥

x0

x0 Reflection of a surface at a single point on the free boundary.

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...details

Hayk Aleksanyan K-surfaces with free boundaries

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SLIDE 94

22/25

...details

Define a convex body S+

∗ bounded by the graph(u∗) if

0 < xd+1 < h0, Ω × {h0} if xd+1 = h0, and when xd+1 < h0 take the intersection of all extreme halfspaces at Γu∗.

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...details

Define a convex body S+

∗ bounded by the graph(u∗) if

0 < xd+1 < h0, Ω × {h0} if xd+1 = h0, and when xd+1 < h0 take the intersection of all extreme halfspaces at Γu∗. For each x ∈ Γu∗, if Hx is an extreme supporting hyperplane to the graph, define H⊥

x passing through Hx ∩ (Rd × {0}) and

the normal to Hx.

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SLIDE 96

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...details

Define a convex body S+

∗ bounded by the graph(u∗) if

0 < xd+1 < h0, Ω × {h0} if xd+1 = h0, and when xd+1 < h0 take the intersection of all extreme halfspaces at Γu∗. For each x ∈ Γu∗, if Hx is an extreme supporting hyperplane to the graph, define H⊥

x passing through Hx ∩ (Rd × {0}) and

the normal to Hx. define S−

x as the mirror reflection of S+ x with respect to H⊥ x .

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...details

Define a convex body S+

∗ bounded by the graph(u∗) if

0 < xd+1 < h0, Ω × {h0} if xd+1 = h0, and when xd+1 < h0 take the intersection of all extreme halfspaces at Γu∗. For each x ∈ Γu∗, if Hx is an extreme supporting hyperplane to the graph, define H⊥

x passing through Hx ∩ (Rd × {0}) and

the normal to Hx. define S−

x as the mirror reflection of S+ x with respect to H⊥ x .

Fix x0 ∈ Γu∗, and take a dense sequence xj ⊂ Γu∗ near x0. Define a nested sequence of convex bodies Sm = S+

∗ ∩ m

  • j=1

S−

xj ,

and take a limit as m → ∞. Call the limit convex body SB the Blaschke reflection body.

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...details

Show that the boundary of SB is a graph over Rd close to x0.

Hayk Aleksanyan K-surfaces with free boundaries

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...details

Show that the boundary of SB is a graph over Rd close to x0. Assume at x0 ∈ Γu∗ we have |∇u∗(x0)| = λ < λ0. Then a slight tilt of the extreme support plane Hx0, say H, will intersect a cap from SB.

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...details

Show that the boundary of SB is a graph over Rd close to x0. Assume at x0 ∈ Γu∗ we have |∇u∗(x0)| = λ < λ0. Then a slight tilt of the extreme support plane Hx0, say H, will intersect a cap from SB. Slightly translate H parallel towards Ω, to Hδ, and in a slab between H and Hδ replace the boundary of SB by an exact solution. For δ > 0 small enough, this will violate the minimality of u∗.

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...details

Show that the boundary of SB is a graph over Rd close to x0. Assume at x0 ∈ Γu∗ we have |∇u∗(x0)| = λ < λ0. Then a slight tilt of the extreme support plane Hx0, say H, will intersect a cap from SB. Slightly translate H parallel towards Ω, to Hδ, and in a slab between H and Hδ replace the boundary of SB by an exact solution. For δ > 0 small enough, this will violate the minimality of u∗. The conclusion is that |∇u∗| = λ0 everywhere on Γu∗ for the minimal solution, and the free boundary is C 1.

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Higher regularity of the free boundary

Strict ellipticity of u∗ and the regularity theory of MA equations imply that u∗ is C ∞ in the interior.

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Higher regularity of the free boundary

Strict ellipticity of u∗ and the regularity theory of MA equations imply that u∗ is C ∞ in the interior. Using the C 1 regularity of the free boundary, and C 1,1-boundary estimates of [J. Urbas, Calc. Var. 1998] for the

  • blique boundary value problems, one gets a bound from

below on the 2nd fundamental form of the free boundary.

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Higher regularity of the free boundary

Strict ellipticity of u∗ and the regularity theory of MA equations imply that u∗ is C ∞ in the interior. Using the C 1 regularity of the free boundary, and C 1,1-boundary estimates of [J. Urbas, Calc. Var. 1998] for the

  • blique boundary value problems, one gets a bound from

below on the 2nd fundamental form of the free boundary. Hence, Blaschke inclusion (again) implies that the free boundary rolls freely inside a ball of some large radius.

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Higher regularity of the free boundary

Strict ellipticity of u∗ and the regularity theory of MA equations imply that u∗ is C ∞ in the interior. Using the C 1 regularity of the free boundary, and C 1,1-boundary estimates of [J. Urbas, Calc. Var. 1998] for the

  • blique boundary value problems, one gets a bound from

below on the 2nd fundamental form of the free boundary. Hence, Blaschke inclusion (again) implies that the free boundary rolls freely inside a ball of some large radius. We can thus do the same construction with the free boundary as our initial domain.

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Higher regularity of the free boundary

Strict ellipticity of u∗ and the regularity theory of MA equations imply that u∗ is C ∞ in the interior. Using the C 1 regularity of the free boundary, and C 1,1-boundary estimates of [J. Urbas, Calc. Var. 1998] for the

  • blique boundary value problems, one gets a bound from

below on the 2nd fundamental form of the free boundary. Hence, Blaschke inclusion (again) implies that the free boundary rolls freely inside a ball of some large radius. We can thus do the same construction with the free boundary as our initial domain. Extending in this way, we get that the gradient of extension agrees with the gradient on u∗ on the free boundary, and we get a solution across the free boundary. This makes, Γu∗ a level surface of a smooth strictly convex solution, and hence the smoothness of free boundary.

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Thank you!

Hayk Aleksanyan K-surfaces with free boundaries