Constructing Entire Functions (a summary)
Kirill Lazebnik
SUNY Stony Brook Kirill.Lazebnik@stonybrook.edu
November 26, 2015
Kirill Lazebnik
Constructing Entire Functions (a summary) Kirill Lazebnik SUNY - - PowerPoint PPT Presentation
Constructing Entire Functions (a summary) Kirill Lazebnik SUNY Stony Brook Kirill.Lazebnik@stonybrook.edu November 26, 2015 Kirill Lazebnik Constructing Entire Functions By Quasiconformal Folding (a summary) Kirill Lazebnik SUNY Stony
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
T - unbounded, locally finite tree, with a bipartite labeling of vertices. Ωj - components of C − T. τ : ∪Ωj → C - the map conformal on each Ωj to Hr . V - the vertices of T. Vj - the image of V under τ restricted to Ωj . For r > 0, define T(r) = ∪e∈T {z : dist(z, e) < rdiam(e)} The τ-size of edge e is the minimum length of the two images τ(e) T has uniformly bounded geometry if: (1) The edges of T are C2 with uniform bounds. (2) The angles between adjacent edges are bounded uniformly from zero (3) Adjacent edges have uniformly comparable lengths (4) For non-adjacent edges e, f , we have diam(e)/dist(e, f ) uniformly bounded.
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
S+ = {x + iy : x > 0, |y| < π/2} is mapped conformally to Hr by λ · sinh. Then holomorphically to C − [−1, 1] by cosh. an = cosh−1
π λ
π cosh(nπ)
by a quasiconformal map ρn of the disc so that: (1) ρn(z) = z for z ∈ ∂D (2) ρn(0) = wn where wn is a point near 1/2. (3) ρn is conformal on 3
4 D
(4) ρn is quasiconformal on D.
Kirill Lazebnik
Kirill Lazebnik