4,275 research outputs found

    On harmonic quasiconformal immersions of surfaces in R3\mathbb{R}^3

    Full text link
    This paper is devoted to the study of the global properties of harmonically immersed Riemann surfaces in R3.\mathbb{R}^3. We focus on the geometry of complete harmonic immersions with quasiconformal Gauss map, and in particular, of those with finite total curvature. We pay special attention to the construction of new examples with significant geometry.Comment: 27 pages, 7 figures. Minor changues. To appear in Trans. Amer. Math. So

    Minimal surfaces in R3\mathbb{R}^3 properly projecting into R2\mathbb{R}^2

    Full text link
    For all open Riemann surface M and real number θ∈(0,Ο€/4),\theta \in (0,\pi/4), we construct a conformal minimal immersion X=(X1,X2,X3):Mβ†’R3X=(X_1,X_2,X_3):M \to \mathbb{R}^3 such that X3+tan⁑(ΞΈ)∣X1∣:Mβ†’RX_3+\tan(\theta) |X_1|:M \to \mathbb{R} is positive and proper. Furthermore, XX can be chosen with arbitrarily prescribed flux map. Moreover, we produce properly immersed hyperbolic minimal surfaces with non empty boundary in R3\mathbb{R}^3 lying above a negative sublinear graph.Comment: 24 pages, 7 figures, to appear in Journal of Differential Geometr

    Complete bounded embedded complex curves in C^2

    Full text link
    We prove that any convex domain of C^2 carries properly embedded complete complex curves. In particular, we exhibit the first examples of complete bounded embedded complex curves in C^2Comment: To appear in J. Eur. Math. Soc. (JEMS

    Approximation theory for non-orientable minimal surfaces and applications

    Full text link
    We prove a version of the classical Runge and Mergelyan uniform approximation theorems for non-orientable minimal surfaces in Euclidean 3-space R3. Then, we obtain some geometric applications. Among them, we emphasize the following ones: 1. A Gunning-Narasimhan type theorem for non-orientable conformal surfaces. 2. An existence theorem for non-orientable minimal surfaces in R3, with arbitrary conformal structure, properly projecting into a plane. 3. An existence result for non-orientable minimal surfaces in R3 with arbitrary conformal structure and Gauss map omitting one projective direction.Comment: 34 pages, 4 figure

    Properness of associated minimal surfaces

    Full text link
    We prove that for any open Riemann surface NN and finite subset ZβŠ‚S1={z∈Cβ€‰βˆ£β€…β€Šβˆ£z∣=1},Z\subset \mathbb{S}^1=\{z\in\mathbb{C}\,|\;|z|=1\}, there exist an infinite closed set ZNβŠ‚S1Z_N \subset \mathbb{S}^1 containing ZZ and a null holomorphic curve F=(Fj)j=1,2,3:Nβ†’C3F=(F_j)_{j=1,2,3}:N\to\mathbb{C}^3 such that the map Y:ZNΓ—Nβ†’R2,Y:Z_N\times N\to \mathbb{R}^2, Y(v,P)=Re(v(F1,F2)(P)),Y(v,P)=Re(v(F_1,F_2)(P)), is proper. In particular, Re(vF):Nβ†’R3Re(vF):N \to\mathbb{R}^3 is a proper conformal minimal immersion properly projecting into R2=R2Γ—{0}βŠ‚R3,\mathbb{R}^2=\mathbb{R}^2\times\{0\}\subset\mathbb{R}^3, for all v∈ZN.v \in Z_N.Comment: 17 pages, 5 figure

    Null Curves in C3\mathbb{C}^3 and Calabi-Yau Conjectures

    Full text link
    For any open orientable surface MM and convex domain Ξ©βŠ‚C3,\Omega\subset \mathbb{C}^3, there exists a Riemann surface NN homeomorphic to MM and a complete proper null curve F:Nβ†’Ξ©.F:N\to\Omega. This result follows from a general existence theorem with many applications. Among them, the followings: For any convex domain Ξ©\Omega in C2\mathbb{C}^2 there exist a Riemann surface NN homeomorphic to MM and a complete proper holomorphic immersion F:Nβ†’Ξ©.F:N\to\Omega. Furthermore, if DβŠ‚R2D \subset \mathbb{R}^2 is a convex domain and Ξ©\Omega is the solid right cylinder {x∈C2∣Re(x)∈D},\{x \in \mathbb{C}^2 | {Re}(x) \in D\}, then FF can be chosen so that Re(F):Nβ†’D{\rm Re}(F):N\to D is proper. There exists a Riemann surface NN homeomorphic to MM and a complete bounded holomorphic null immersion F:Nβ†’SL(2,C).F:N \to {\rm SL}(2,\mathbb{C}). There exists a complete bounded CMC-1 immersion X:Mβ†’H3.X:M \to \mathbb{H}^3. For any convex domain Ξ©βŠ‚R3\Omega \subset \mathbb{R}^3 there exists a complete proper minimal immersion (Xj)j=1,2,3:Mβ†’Ξ©(X_j)_{j=1,2,3}:M \to \Omega with vanishing flux. Furthermore, if DβŠ‚R2D \subset \mathbb{R}^2 is a convex domain and Ξ©={(xj)j=1,2,3∈R3∣(x1,x2)∈D},\Omega=\{(x_j)_{j=1,2,3} \in \mathbb{R}^3 | (x_1,x_2) \in D\}, then XX can be chosen so that (X1,X2):Mβ†’D(X_1,X_2):M\to D is proper. Any of the above surfaces can be chosen with hyperbolic conformal structure.Comment: 20 pages, 4 figures. To appear in Mathematische Annale

    Every meromorphic function is the Gauss map of a conformal minimal surface

    Full text link
    Let MM be an open Riemann surface. We prove that every meromorphic function on MM is the complex Gauss map of a conformal minimal immersion Mβ†’R3M\to\mathbb{R}^3 which may furthermore be chosen as the real part of a holomorphic null curve Mβ†’C3M\to\mathbb{C}^3. Analogous results are proved for conformal minimal immersions Mβ†’RnM\to\mathbb{R}^n for any n>3n>3. We also show that every conformal minimal immersion Mβ†’RnM\to\mathbb{R}^n is isotopic through conformal minimal immersions Mβ†’RnM\to\mathbb{R}^n to a flat one, and we identify the path connected components of the space of all conformal minimal immersions Mβ†’RnM\to\mathbb{R}^n for any nβ‰₯3n\ge 3.Comment: J. Geom. Anal., to appear. Available on SpringerLink: https://link.springer.com/article/10.1007%2Fs12220-017-9948-

    A construction of complete complex hypersurfaces in the ball with control on the topology

    Full text link
    Given a closed complex hypersurface ZβŠ‚CN+1Z\subset \mathbb{C}^{N+1} (N∈N)(N\in\mathbb{N}) and a compact subset KβŠ‚ZK\subset Z, we prove the existence of a pseudoconvex Runge domain DD in ZZ such that KβŠ‚DK\subset D and there is a complete proper holomorphic embedding from DD into the unit ball of CN+1\mathbb{C}^{N+1}. For N=1N=1, we derive the existence of complete properly embedded complex curves in the unit ball of C2\mathbb{C}^2, with arbitrarily prescribed finite topology. In particular, there exist complete proper holomorphic embeddings of the unit disc DβŠ‚C\mathbb{D}\subset \mathbb{C} into the unit ball of C2\mathbb{C}^2. These are the first known examples of complete bounded embedded complex hypersurfaces in CN+1\mathbb{C}^{N+1} with any control on the topology.Comment: 20 pages, 3 figures. Main Theorem improved and proof simplified. To appear in J. Reine Angew. Math. (Crelle's J.

    Embedded minimal surfaces in Rn\mathbb{R}^n

    Full text link
    In this paper, we prove that every confomal minimal immersion of an open Riemann surface into Rn\mathbb{R}^n for nβ‰₯5n\ge 5 can be approximated uniformly on compacts by conformal minimal embeddings. Furthermore, we show that every open Riemann surface carries a proper conformal minimal embedding into R5\mathbb{R}^5. One of our main tools is a Mergelyan approximation theorem for conformal minimal immersions to Rn\mathbb{R}^n for any nβ‰₯3n\ge 3 which is also proved in the paper.Comment: Math. Z., in press. The official version is available on Springerlink at http://link.springer.com/article/10.1007%2Fs00209-015-1586-

    The phi(1020) a0(980) S-wave scattering and hints for a new vector-isovector resonance

    Full text link
    We have studied the phi(1020)a0(980) S-wave scattering at threshold energies employing chiral Lagrangians coupled to vector mesons by minimal coupling. The interaction is described without new free parameters by considering the scalar isovector a0(980) resonance as dynamically generated in coupled channels, and demanding that the recently measured e+ e- -> phi(1020) f0(980) cross section is reproduced. For some realistic choices of the parameters, the presence of a dynamically generated isovector companion of the Y(2175) is revealed. We have also investigated the corrections to the e+ e- -> phi(1020) pi0 eta reaction cross section that arise from phi(1020)a0(980) re-scattering in the final state. They are typically large and modify substantially the cross section. For a suitable choice of parameters, the presence of the resonance would manifest itself as a clear peak at sqrt{s}~2.03 GeV in e+ e- -> phi(1020) pi0 eta.Comment: 16 pages, 9 figures, 2 table
    • …
    corecore