Linear Subspaces of Hypersurfaces
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NOTES on FIBER DIMENSION Let Φ : X → Y Be a Morphism of Affine
NOTES ON FIBER DIMENSION SAM EVENS Let φ : X → Y be a morphism of affine algebraic sets, defined over an algebraically closed field k. For y ∈ Y , the set φ−1(y) is called the fiber over y. In these notes, I explain some basic results about the dimension of the fiber over y. These notes are largely taken from Chapters 3 and 4 of Humphreys, “Linear Algebraic Groups”, chapter 6 of Bump, “Algebraic Geometry”, and Tauvel and Yu, “Lie algebras and algebraic groups”. The book by Bump has an incomplete proof of the main fact we are proving (which repeats an incomplete proof from Mumford’s notes “The Red Book on varieties and Schemes”). Tauvel and Yu use a step I was not able to verify. The important thing is that you understand the statements and are able to use the Theorems 0.22 and 0.24. Let A be a ring. If p0 ⊂ p1 ⊂···⊂ pk is a chain of distinct prime ideals of A, we say the chain has length k and ends at p. Definition 0.1. Let p be a prime ideal of A. We say ht(p) = k if there is a chain of distinct prime ideals p0 ⊂···⊂ pk = p in A of length k, and there is no chain of prime ideals in A of length k +1 ending at p. If B is a finitely generated integral k-algebra, we set dim(B) = dim(F ), where F is the fraction field of B. Theorem 0.2. (Serre, “Local Algebra”, Proposition 15, p. 45) Let A be a finitely gener- ated integral k-algebra and let p ⊂ A be a prime ideal. -
Complete Hypersurfaces in Euclidean Spaces with Finite Strong Total
Complete hypersurfaces in Euclidean spaces with finite strong total curvature Manfredo do Carmo and Maria Fernanda Elbert Abstract We prove that finite strong total curvature (see definition in Section 2) complete hypersurfaces of (n + 1)-euclidean space are proper and diffeomorphic to a com- pact manifold minus finitely many points. With an additional condition, we also prove that the Gauss map of such hypersurfaces extends continuously to the punc- tures. This is related to results of White [22] and and M¨uller-Sver´ak[18].ˇ Further properties of these hypersurfaces are presented, including a gap theorem for the total curvature. 1 Introduction Let φ: M n ! Rn+1 be a hypersurface of the euclidean space Rn+1. We assume that n n n+1 M = M is orientable and we fix an orientation for M. Let g : M ! S1 ⊂ R be the n Gauss map in the given orientation, where S1 is the unit n-sphere. Recall that the linear operator A: TpM ! TpM, p 2 M, associated to the second fundamental form, is given by hA(X);Y i = −hrX N; Y i; X; Y 2 TpM; where r is the covariant derivative of the ambient space and N is the unit normal vector in the given orientation. The map A = −dg is self-adjoint and its eigenvalues are the principal curvatures k1; k2; : : : ; kn. Key words and sentences: Complete hypersurface, total curvature, topological properties, Gauss- Kronecker curvature 2000 Mathematics Subject Classification. 57R42, 53C42 Both authors are partially supported by CNPq and Faperj. 1 R n We say that the total curvature of the immersion is finite if M jAj dM < 1, where P 21=2 n n n+1 jAj = i ki , i.e., if jAj belongs to the space L (M). -
Vanishing Cycles, Plane Curve Singularities, and Framed Mapping Class Groups
VANISHING CYCLES, PLANE CURVE SINGULARITIES, AND FRAMED MAPPING CLASS GROUPS PABLO PORTILLA CUADRADO AND NICK SALTER Abstract. Let f be an isolated plane curve singularity with Milnor fiber of genus at least 5. For all such f, we give (a) an intrinsic description of the geometric monodromy group that does not invoke the notion of the versal deformation space, and (b) an easy criterion to decide if a given simple closed curve in the Milnor fiber is a vanishing cycle or not. With the lone exception of singularities of type An and Dn, we find that both are determined completely by a canonical framing of the Milnor fiber induced by the Hamiltonian vector field associated to f. As a corollary we answer a question of Sullivan concerning the injectivity of monodromy groups for all singularities having Milnor fiber of genus at least 7. 1. Introduction Let f : C2 ! C denote an isolated plane curve singularity and Σ(f) the Milnor fiber over some point. A basic principle in singularity theory is to study f by way of its versal deformation space ∼ µ Vf = C , the parameter space of all deformations of f up to topological equivalence (see Section 2.2). From this point of view, two of the most basic invariants of f are the set of vanishing cycles and the geometric monodromy group. A simple closed curve c ⊂ Σ(f) is a vanishing cycle if there is some deformation fe of f with fe−1(0) a nodal curve such that c is contracted to a point when transported to −1 fe (0). -
Solutions to the Maximal Spacelike Hypersurface Equation in Generalized Robertson-Walker Spacetimes
Electronic Journal of Differential Equations, Vol. 2018 (2018), No. 80, pp. 1{14. ISSN: 1072-6691. URL: http://ejde.math.txstate.edu or http://ejde.math.unt.edu SOLUTIONS TO THE MAXIMAL SPACELIKE HYPERSURFACE EQUATION IN GENERALIZED ROBERTSON-WALKER SPACETIMES HENRIQUE F. DE LIMA, FABIO´ R. DOS SANTOS, JOGLI G. ARAUJO´ Communicated by Giovanni Molica Bisci Abstract. We apply some generalized maximum principles for establishing uniqueness and nonexistence results concerning maximal spacelike hypersur- faces immersed in a generalized Robertson-Walker (GRW) spacetime, which is supposed to obey the so-called timelike convergence condition (TCC). As application, we study the uniqueness and nonexistence of entire solutions of a suitable maximal spacelike hypersurface equation in GRW spacetimes obeying the TCC. 1. Introduction In the previous decades, the study of spacelike hypersurfaces immersed in a Lorentz manifold has been of substantial interest from both physical and mathe- matical points of view. For instance, it was pointed out by Marsden and Tipler [24] and Stumbles [37] that spacelike hypersurfaces with constant mean curvature in a spacetime play an important role in General Relativity, since they can be used as initial hypersurfaces where the constraint equations can be split into a linear system and a nonlinear elliptic equation. From a mathematical point of view, spacelike hypersurfaces are also interesting because of their Bernstein-type properties. One can truly say that the first remark- able results in this branch were the rigidity theorems of Calabi [13] and Cheng and Yau [15], who showed (the former for n ≤ 4, and the latter for general n) that the only maximal (that is, with zero mean curvature) complete spacelike hypersurfaces of the Lorentz-Minkowski space Ln+1 are the spacelike hyperplanes. -
Fiber Bundles and Intersectional Feminism 1
FIBER BUNDLES AND INTERSECTIONAL FEMINISM DAGAN KARP Abstract. This note provides an introduction to, and call for ac- tion for, intersectional feminism for mathematicians. It also serves as an example of mathematical models of social structures, provid- ing an application of geometry to social theory. 1. Gender Inequity in Mathematics Gender inequity is historically severe and remains extant in math- ematics. Although nearly half of all bachelor's1 degrees2 in the U.S. in mathematics are awarded to women according to the Conference Board of the Mathematical Sciences (CBMS) [4], only about 30% of the PhD's in mathematics in the U.S. are awarded to women, and fur- ther only 14% of tenured mathematics faculty are women, according to the American Mathematical Society (AMS) Annual Survey [19]. See Section 2 for a discussion of gender and gendered terms. The underrepresentation of women in mathematics is persistent and pervasive. Comparing previous CMBS and AMS Annual Survey Data3, we see that these critical transition points are persistent. For example, the percentage of women PhD recipients in mathematics has remained at roughly 30% for at least two decades. Hence, there is persistent gender inequity at the level of participation and representation. It is worth noting that such underrepresentation extends throughout the profession. For example, \women are underrepresented as authors of mathematics papers on the arχiv, even in comparison to the proportion of women who hold full-time positions in mathematics departments"[7]. Such patters continue to appear in peer-reviewed publications [32]. Women are also underrepresented in journal editorial boards in the mathematical sciences [39]. -
Rotational Hypersurfaces Satisfying ∆ = in the Four-Dimensional
POLİTEKNİK DERGİSİ JOURNAL of POLYTECHNIC ISSN: 1302-0900 (PRINT), ISSN: 2147-9429 (ONLINE) URL: http://dergipark.org.tr/politeknik Rotational hypersurfaces satisfying ∆푰퐑 = 퐀퐑 in the four-dimensional Euclidean space Dört-boyutlu Öklid uzayında ∆퐼푹 = 푨푹 koşulunu sağlayan dönel hiperyüzeyler Yazar(lar) (Author(s)): Erhan GÜLER ORCID : 0000-0003-3264-6239 Bu makaleye şu şekilde atıfta bulunabilirsiniz (To cite to this article): Güler E., “Rotational hypersurfaces satisfying ∆퐼퐑 = 퐀퐑 in the four-dimensional Euclidean space”, Politeknik Dergisi, 24(2): 517-520, (2021). Erişim linki (To link to this article): http://dergipark.org.tr/politeknik/archive DOI: 10.2339/politeknik.670333 Rotational Hypersurfaces Satisfying 횫퐈퐑 = 퐀퐑 in the Four-Dimensional Euclidean Space Highlights ❖ Rotational hypersurface has zero mean curvature iff its Laplace-Beltrami operator vanishing ❖ Each element of the 4×4 order matrix A, which satisfies the condition 훥퐼푅 = 퐴푅, is zero ❖ Laplace-Beltrami operator of the rotational hypersurface depends on its mean curvature and the Gauss map Graphical Abstract Rotational hypersurfaces in the 4-dimensional Euclidean space are discussed. Some relations of curvatures of hypersurfaces are given, such as the mean, Gaussian, and their minimality and flatness. The Laplace-Beltrami operator has been defined for 4-dimensional hypersurfaces depending on the first fundamental form. In addition, it is indicated that each element of the 4×4 order matrix A, which satisfies the condition 훥퐼푅 = 퐴푅, is zero, that is, the rotational hypersurface R is minimal. Aim We consider the rotational hypersurfaces in 피4 to find its Laplace-Beltrami operator. Design & Methodology We indicate fundamental notions of 피4. Considering differential geometry formulas in 3-space, we transform them in 4-space. -
Rotation Hypersurfaces in Sn × R and Hn × R
Note di Matematica Note Mat. 29 (2009), n. 1, 41-54 ISSN 1123-2536, e-ISSN 1590-0932 DOI 10.1285/i15900932v29n1p41 Notehttp://siba-ese.unisalento.it, di Matematica 29, ©n. 2009 1, 2009, Università 41–54. del Salento __________________________________________________________________ Rotation hypersurfaces in Sn × R and Hn × R Franki Dillen i [email protected] Johan Fastenakels ii [email protected] Joeri Van der Veken iii Katholieke Universiteit Leuven, Department of Mathematics, Celestijnenlaan 200B Box 2400, BE-3001 Leuven, Belgium. [email protected] Received: 14/11/2007; accepted: 07/04/2008. Abstract. We introduce the notion of rotation hypersurfaces of Sn × R and Hn × R and we prove a criterium for a hypersurface of one of these spaces to be a rotation hypersurface. Moreover, we classify minimal rotation hypersurfaces, flat rotation hypersurfaces and rotation hypersurfaces which are normally flat in the Euclidean resp. Lorentzian space containing Sn ×R resp. Hn × R. Keywords: rotation hypersurface, flat, minimal MSC 2000 classification: 53B25 1 Introduction In[3]theclassicalnotionofarotationsurfaceinE3 was extended to rota- tion hypersurfaces of real space forms of arbitrary dimension. Motivated by the recent study of hypersurfaces of the Riemannian products Sn × R and Hn × R, see for example [2], [4], [5] and [6], we will extend the notion of rotation hyper- surfaces to these spaces. Starting with a curve α on a totally geodesic cylinder S1 × R resp. H1 × R and a plane containing the axis of the cylinder, we will construct such a hypersurface and we will compute its principal curvatures. Moreover, we will prove a criterium for a hypersurface of Sn × R resp. -
Systems of Lines Amd Planes on the Quadric
Systems of lines and planes on the quadric hypersurface in spaces of four and five dimensions Item Type text; Thesis-Reproduction (electronic) Authors Fish, Anne, 1924- Publisher The University of Arizona. Rights Copyright © is held by the author. Digital access to this material is made possible by the University Libraries, University of Arizona. Further transmission, reproduction or presentation (such as public display or performance) of protected items is prohibited except with permission of the author. Download date 01/10/2021 14:55:47 Link to Item http://hdl.handle.net/10150/319188 SYSTEMS OF LINES■AMD PLANES ON THE QUADRIC HYPERSURFACE SPACES OF FOUR AND- FIVE DIMENSIONS - by Anne Fish A TLes is submitted to the faculty of the Department of Mathematics in partial fullfilment of the requirements for the degree of Master of Science in the Graduate College University of Arizona 1948 Approved: Direeto^ of Thesis t Date & R A& TABLE OF CONTENTS I? O (TU. O "fc X OH a a © © a © o © © © © o © o © © ©ooo oool Chapter I Geometry of M-Dirnensiona 1 Projective Space © » 2 II Ruled Surfaces in Three-Dimensional Projective Space © © © © © © © © © © © © 10 III Systems of Lines on a Quadric Surface in Three-Dimensional Projective Space © © « © 13 IV Systems of Lines on a Quadric Hypersurface in Four-Dimensional Projective Space « © © © 23 V Systems of Planes on a Quadric Hypersurface in a Projective Space of Five Dimensions © © 34 Bibliography © © © © © © © © © © © © © © © © © © © s © © © 4V 194189 INTRODUCTION It has long been common knowledge -
Set Theory in Computer Science a Gentle Introduction to Mathematical Modeling I
Set Theory in Computer Science A Gentle Introduction to Mathematical Modeling I Jose´ Meseguer University of Illinois at Urbana-Champaign Urbana, IL 61801, USA c Jose´ Meseguer, 2008–2010; all rights reserved. February 28, 2011 2 Contents 1 Motivation 7 2 Set Theory as an Axiomatic Theory 11 3 The Empty Set, Extensionality, and Separation 15 3.1 The Empty Set . 15 3.2 Extensionality . 15 3.3 The Failed Attempt of Comprehension . 16 3.4 Separation . 17 4 Pairing, Unions, Powersets, and Infinity 19 4.1 Pairing . 19 4.2 Unions . 21 4.3 Powersets . 24 4.4 Infinity . 26 5 Case Study: A Computable Model of Hereditarily Finite Sets 29 5.1 HF-Sets in Maude . 30 5.2 Terms, Equations, and Term Rewriting . 33 5.3 Confluence, Termination, and Sufficient Completeness . 36 5.4 A Computable Model of HF-Sets . 39 5.5 HF-Sets as a Universe for Finitary Mathematics . 43 5.6 HF-Sets with Atoms . 47 6 Relations, Functions, and Function Sets 51 6.1 Relations and Functions . 51 6.2 Formula, Assignment, and Lambda Notations . 52 6.3 Images . 54 6.4 Composing Relations and Functions . 56 6.5 Abstract Products and Disjoint Unions . 59 6.6 Relating Function Sets . 62 7 Simple and Primitive Recursion, and the Peano Axioms 65 7.1 Simple Recursion . 65 7.2 Primitive Recursion . 67 7.3 The Peano Axioms . 69 8 Case Study: The Peano Language 71 9 Binary Relations on a Set 73 9.1 Directed and Undirected Graphs . 73 9.2 Transition Systems and Automata . -
Arxiv:2008.11018V1 [Math.DG]
UNIQUENESS OF HYPERSURFACES OF CONSTANT HIGHER ORDER MEAN CURVATURE IN HYPERBOLIC SPACE BARBARA NELLI, JINGYONG ZHU Abstract. We study the uniqueness of horospheres and equidistant spheres in hyperbolic space under different conditions. First we generalize the Bernstein theorem by Do Carmo and Lawson [12] to the embedded hypersurfaces with constant higher order mean curva- ture. Then we prove two Bernstein type results for immersed hypersurfaces under different assumptions. Last, we show the rigidity of horospheres and equidistant spheres in terms of their higher order mean curvatures. 1. Introduction In 1927, S. N. Bernstein proved that the only entire minimal graphs in R3 are planes. The analogous problem in higher dimension is known as Bernstein problem. Namely, given u : Rn → R a minimal graph, is the graph of u a flat hyperplane? It turns out that the answer is yes for n ≤ 7 and that has been settled down by a series of very significative papers [4, 11, 16, 24]. On the contrary, for n ≥ 8, one has the famous counterexamples by E. Bombieri, E. De Giorgi and E. Giusti [6]. Afterwards, many generalizations of Bernstein theorem have arised. As an example, we mention [23] where R. Schoen, L. Simon and S. T. Yau studied a Bernstein type theorem for stable minimal hypersurfaces. Later on, Bernstein type theorems for constant mean curvature hypersurfaces in Euclidean and in hyperbolic space Hn+1 have been studied. Let us give a very simple example in the Euclidean space. Does it exist an entire graph M in Rn+1 with constant mean curvature H =6 0? It is well known that the answer is no and here is the proof. -
Properties of Hypersurfaces Which Are Characteristic for Spaces of Constant
ANNALI DELLA SCUOLA NORMALE SUPERIORE DI PISA Classe di Scienze OLDRICHˇ KOWALSKI Properties of hypersurfaces which are characteristic for spaces of constant curvature Annali della Scuola Normale Superiore di Pisa, Classe di Scienze 3e série, tome 26, no 1 (1972), p. 233-245 <http://www.numdam.org/item?id=ASNSP_1972_3_26_1_233_0> © Scuola Normale Superiore, Pisa, 1972, tous droits réservés. L’accès aux archives de la revue « Annali della Scuola Normale Superiore di Pisa, Classe di Scienze » (http://www.sns.it/it/edizioni/riviste/annaliscienze/) implique l’accord avec les conditions générales d’utilisation (http://www.numdam.org/conditions). Toute utilisa- tion commerciale ou impression systématique est constitutive d’une infraction pénale. Toute copie ou impression de ce fichier doit contenir la présente mention de copyright. Article numérisé dans le cadre du programme Numérisation de documents anciens mathématiques http://www.numdam.org/ PROPERTIES OF HYPERSURFACES WHICH ARE CHARACTERISTIC FOR SPACES OF CONSTANT CURVATURE OLD0159ICH KOWALSKI, Praha If is well-known that the spaces of constant curvature are characteri- zed among all Riemannian spaces by the following property : for any (n -1)- dimensional linear elements En-l of a Riemann space N (dim N = n > 3) there is a totally geodesic hypersurface which is tangent to En-1. (Cf. [1]). The purpose of this Note is to present a number of theorems of the above type ; only the requirement that our hypersurfaces should be totally geodesic will be replaced be another geometrical or analytical postu- lates. Umbilical points of hypersurfaces and so called « normal Bianchi identity >> play the leading part here. -
LINES on SMOOTH HYPERSURFACES Let K Be an Algebraically Closed Field of Characteristic P. If X Is a Subvariety of Pn K and X
LINES ON SMOOTH HYPERSURFACES OLIVIER DEBARRE Let k be an algebraically closed field of characteristic p. If X is a n subvariety of Pk and x a point on X, we denote by TxX the projective closure of the embedded Zariski tangent space to X at x. It is known that the family of lines on a general hypersurface of degree d in Pn is smooth of dimension 2n − 3 − d. When n is very large with respect to d, any smooth hypersurface of degree d in Pn has this property ([HMP]). However, the bound in [HMP] is very large, whereas • the family of lines on a smooth cubic in Pn, with n ≥ 3, is smooth of the expected dimension 2n − 6. • the family of lines on a smooth quartic in Pn, with n ≥ 4, has the expected dimension 2n − 7 for p 6= 2; 3 (Collino). However, it may be reducible and non-reduced. Conjecture 1. Assume p = 0 or p ≥ d. The family of lines on a smooth hypersurface of degree d in Pn has the expected dimension 2n − 3 − d for n ≥ d. These bounds are the best possible: the family of lines contained in a Fermat hypersurface in Pn has dimension at least n − 3, which is larger than the expected dimension for n < d. Also, when p > 0, the family of lines contained in a Fermat hypersurface of degree p + 1 in Pn has dimension 2n − 4, which is larger than the expected dimension. Note that by taking general hyperplane sections,1 it is enough to prove Conjecture 1 in the case n = d.