Potential Theory and Dynamics on the Berkovich Projective Line
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"The Newton Polygon of a Planar Singular Curve and Its Subdivision"
THE NEWTON POLYGON OF A PLANAR SINGULAR CURVE AND ITS SUBDIVISION NIKITA KALININ Abstract. Let a planar algebraic curve C be defined over a valuation field by an equation F (x,y)= 0. Valuations of the coefficients of F define a subdivision of the Newton polygon ∆ of the curve C. If a given point p is of multiplicity m on C, then the coefficients of F are subject to certain linear constraints. These constraints can be visualized in the above subdivision of ∆. Namely, we find a 3 2 distinguished collection of faces of the above subdivision, with total area at least 8 m . The union of these faces can be considered to be the “region of influence” of the singular point p in the subdivision of ∆. We also discuss three different definitions of a tropical point of multiplicity m. 0. Introduction Fix a non-empty finite subset Z2 and any valuation field K. We consider a curve C given by an equation F (x,y) = 0, where A⊂ i j ∗ (1) F (x,y)= aijx y , aij K . ∈ (i,jX)∈A Suppose that we know only the valuations of the coefficients of the polynomial F (x,y). Is it possible to extract any meaningful information from this knowledge? Unexpectedly, many geometric properties of C are visible from such a viewpoint. The Newton polygon ∆=∆( ) of the curve C is the convex hull of in R2. The extended Newton A A2 polyhedron of the curve C is the convex hull of the set ((i, j),s) R R (i, j) ,s val(aij) . -
The Arakelov-Zhang Pairing and Julia Sets
THE ARAKELOV-ZHANG PAIRING AND JULIA SETS ANDREW BRIDY AND MATT LARSON Abstract. The Arakelov-Zhang pairing h ; φi is a measure of the \dynamical distance" between two rational maps and φ defined over a number field K. It is defined in terms of local integrals on Berkovich space at each completion of K. We obtain a simple expression for the important case of the pairing with a power map, written in terms of integrals over Julia sets. Under certain disjointness conditions on Julia sets, our expression simplifies to a single canonical height term; in general, this term is a lower bound. As applications of our method, we give bounds on the difference between the canonical height hφ and the standard Weil height h, and we prove a rigidity statement about polynomials that satisfy a strong form of good reduction. 1. Introduction Let K be a number field with fixed algebraic closure K. For z 2 P1(K), we use h(z) to denote the standard logarithmic Weil height of z and hφ(z) to denote the Call-Silverman canonical height of z with respect to φ 2 K(x). We recall background on these heights in Section 2. Let ; φ : P1 ! P1 be rational maps defined over K (equivalently, rational functions in K(x)) each of degree ≥ 2. In [21] (see also [23]), Petsche, Szpiro, and Tucker introduced the Arakelov-Zhang pairing h ; φi, a symmetric, non-negative, real-valued pairing on the space of rational maps. In Section 2, we present their definition of the pairing as a sum of integrals over Berkovich space at each place of K. -
Riemann Surfaces, Conformal Fields and Strings I. FIELD THEORY and RIEMANN SURFACES the Space-Time on Which the Particl Physicis
Riemann Surfaces, Conformal Fields and Strings I he ru k uf Rtc m:rnn s url acc~ in modern pa rticle r h y~ i cs I\ discussed. M<i thc111at- 1r :1!1 \. q11 :1111urn ri cld th eories c:1 11 he tlclinccl 011 the" : mani fo lds if the <1rc co11 - lmm11lll' in ari 11 n1. I hysic•tll y. Ri 1:t11 nnn surl:i tcs provide n 111 od1: I for th • wqrlJ , h~ c l ~ 'vc p t out IJ n prop:1gating rcla1i vistk stri ng. Thuh Ricmu nn surl uccs nrc th e natural se ll ing for confom1al fiel d theory. and. both these co n cc pl ~ together pruvidc .1 1i1r11tul .1 t1 011 of smng theory. I\~\ Words: string theory, conformal symmetry , 11•orld sh eets, Riemann surfaces I. FIELD THEORY AND RIEMANN SURFACES The space- tim e on whi ch th e particl ph ysici st writes a Lagrnngian field theory and deduces equations ol moiion, c b ss i c~ d solutions anJ quantum scaucring amplitud s is usually taken to be a Ri e nian111a11 manifold . 1 T he. ii.l ea is cent rn l l ' ge neral relati vi ty and grav1tat1 n.2 and has becom · mor imporlanl in pnrticlc phys ics w11h increasi ng cmphasi on unified th eo ries o f all for es including grav itation . R1cmannian gcomotr is usually incorpo.ratctl as a se ri es of pre Knpti ons. starting with the introduction of a i..:c ond -r:rnk ~y m mctril: tcn·or fi ' ld, the metri c g1.,,(x). -
Conformal Field Theories of Stochastic Loewner Evolutions
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by CERN Document Server Conformal Field Theories of Stochastic Loewner Evolutions. [ CFTs of SLEs ] Michel Bauer1 and Denis Bernard2 Service de Physique Th´eorique de Saclay CEA/DSM/SPhT, Unit´e de recherche associ´ee au CNRS CEA-Saclay, 91191 Gif-sur-Yvette, France Abstract Stochastic Loewner evolutions (SLEκ) are random growth pro- cesses of sets, called hulls, embedded in the two dimensional upper half plane. We elaborate and develop a relation between SLEκ evo- lutions and conformal field theories (CFT) which is based on a group theoretical formulation of SLEκ processes and on the identification of the proper hull boundary states. This allows us to define an in- finite set of SLEκ zero modes, or martingales, whose existence is a consequence of the existence of a null vector in the appropriate Vira- soro modules. This identification leads, for instance, to linear systems for generalized crossing probabilities whose coefficients are multipoint CFT correlation functions. It provides a direct link between confor- mal correlation functions and probabilities of stopping time events in SLEκ evolutions. We point out a relation between SLEκ processes and two dimensional gravity and conjecture a reconstruction proce- dure of conformal field theories from SLEκ data. 1Email: [email protected] 2Member of the CNRS; email: [email protected] 1 1 Introduction. Two dimensional conformal field theories [2] have produced an enormous amount of exact results for multifractal properties of conformally invariant critical clusters. See eg. refs.[15, 5, 9] and references therein. -
Berkovich Analytification
Berkovich analytification Wouter Zomervrucht, November 10, 2016 1. Berkovich spaces Throughout, k is a non-archimedean field. −1 −1 Let’s recall some definitions. An affinoid algebra A is a quotient of kfr1 T1,..., rn Tng for some r1,..., rn > 0. Its Berkovich spectrum is the topological space bounded multiplicative (equivalence classes of) bounded X = M(A) = = . seminorms on A maps from A to a valuation field A domain D ⊆ X is a closed subset that admits a bounded homomorphism A ! AD universal for the property that M(AD) !M(A) has image inside D. For such D one has D = M(AD). The map A ! AD is flat. Domains form systems of neighborhoods at each point of X. In other words, domains behave exactly like the standard opens D( f ) ⊆ Spec A do for schemes. A subset Z ⊆ X is special if it is a finite union of domains. If Z = D1 [ ... [ Dn is such a = presentation, then we write AZ ker ∏i ADi ⇒ ∏i,j ADi\Dj . Define OX(U) = lim AZ. Z ⊆ U special Now (X, OX) is a locally ringed space, satisfying OX(X) = A. Remark 1.1. The functor M : faffinoid algebrasg ! flocally ringed spacesg is faithful, but not full. This problem, together with the lack of localizations, warrants the somewhat involved definition below. A quasi-affinoid space is a locally ringed space U equipped with the data of an affinoid algebra A and an open immersion U ,!M(A).A morphism of quasi-affinoid spaces f : (U, A) ! (V, B) is a map of locally ringed spaces such that for all domains D ⊆ U, E ⊆ V with f (D) ⊆ E the restriction f : D ! E is affinoid, i.e. -
Second Kind Integral Equations for the Classical Potential Theory on Open Surfaces I: Analytical Apparatus
Journal of Computational Physics 191 (2003) 40–74 www.elsevier.com/locate/jcp Second kind integral equations for the classical potential theory on open surfaces I: analytical apparatus Shidong Jiang *,1, Vladimir Rokhlin Department of Computer Science, Yale University, New Haven, Connecticut 06520, USA Received 6 February 2003; accepted 21 May 2003 Abstract A stable second kind integral equation formulation has been developed for the Dirichlet problem for the Laplace equation in two dimensions, with the boundary conditions specified on a collection of open curves. The performance of the obtained apparatus is illustrated with several numerical examples. Ó 2003 Elsevier Science B.V. All rights reserved. AMS: 65R10; 77C05 Keywords: Open surface problems; Laplace equation; Finite Hilbert transform; Second kind integral equation; Dirichlet problem 1. Introduction Integral equations have been one of principal tools for the numerical solution of scattering problems for more than 30 years, both in the Helmholtz and Maxwell environments. Historically, most of the equations used have been of the first kind, since numerical instabilities associated with such equations have not been critically important for the relatively small-scale problems that could be handled at the time. The combination of improved hardware with the recent progress in the design of ‘‘fast’’ algorithms has changed the situation dramatically. Condition numbers of systems of linear algebraic equations resulting from the discretization of integral equations of potential theory have become critical, and the simplest way to limit such condition numbers is by starting with second kind integral equations. Hence, interest has increased in reducing scattering problems to systems of second kind integral equations on the boundaries of the scatterers. -
Renormalization and Effective Field Theory
Mathematical Surveys and Monographs Volume 170 Renormalization and Effective Field Theory Kevin Costello American Mathematical Society surv-170-costello-cov.indd 1 1/28/11 8:15 AM http://dx.doi.org/10.1090/surv/170 Renormalization and Effective Field Theory Mathematical Surveys and Monographs Volume 170 Renormalization and Effective Field Theory Kevin Costello American Mathematical Society Providence, Rhode Island EDITORIAL COMMITTEE Ralph L. Cohen, Chair MichaelA.Singer Eric M. Friedlander Benjamin Sudakov MichaelI.Weinstein 2010 Mathematics Subject Classification. Primary 81T13, 81T15, 81T17, 81T18, 81T20, 81T70. The author was partially supported by NSF grant 0706954 and an Alfred P. Sloan Fellowship. For additional information and updates on this book, visit www.ams.org/bookpages/surv-170 Library of Congress Cataloging-in-Publication Data Costello, Kevin. Renormalization and effective fieldtheory/KevinCostello. p. cm. — (Mathematical surveys and monographs ; v. 170) Includes bibliographical references. ISBN 978-0-8218-5288-0 (alk. paper) 1. Renormalization (Physics) 2. Quantum field theory. I. Title. QC174.17.R46C67 2011 530.143—dc22 2010047463 Copying and reprinting. Individual readers of this publication, and nonprofit libraries acting for them, are permitted to make fair use of the material, such as to copy a chapter for use in teaching or research. Permission is granted to quote brief passages from this publication in reviews, provided the customary acknowledgment of the source is given. Republication, systematic copying, or multiple reproduction of any material in this publication is permitted only under license from the American Mathematical Society. Requests for such permission should be addressed to the Acquisitions Department, American Mathematical Society, 201 Charles Street, Providence, Rhode Island 02904-2294 USA. -
Hep-Th/0101032V1 5 Jan 2001 Uhawyta H Eutn Trpoutcntuto Ol No Would Construction Star-Product O Resulting So field) the (Tensor Coordinates
WICK TYPE DEFORMATION QUANTIZATION OF FEDOSOV MANIFOLDS V. A. DOLGUSHEV, S. L. LYAKHOVICH, AND A. A. SHARAPOV Abstract. A coordinate-free definition for Wick-type symbols is given for symplectic manifolds by means of the Fedosov procedure. The main ingredient of this approach is a bilinear symmetric form defined on the complexified tangent bundle of the symplectic manifold and subject to some set of algebraic and differential conditions. It is precisely the structure which describes a deviation of the Wick-type star-product from the Weyl one in the first order in the deformation parameter. The geometry of the symplectic manifolds equipped by such a bilinear form is explored and a cer- tain analogue of the Newlander-Nirenberg theorem is presented. The 2-form is explicitly identified which cohomological class coincides with the Fedosov class of the Wick-type star-product. For the particular case of K¨ahler manifold this class is shown to be proportional to the Chern class of a complex manifold. We also show that the symbol construction admits canonical superexten- sion, which can be thought of as the Wick-type deformation of the exterior algebra of differential forms on the base (even) manifold. Possible applications of the deformed superalgebra to the noncommutative field theory and strings are discussed. 1. Introduction The deformation quantization as it was originally defined in [1], [2] has now been well established for every symplectic manifold through the combined efforts of many authors (for review see [3]). The question of existence of the formal associative deformation for the commutative algebra of smooth functions, so-called star product, has been solved by De Wilde and Lecomte [4]. -
Potential Theory of Schr~Dingew Operator
PROBABILITY. AND MATHEMAT[CAL STATISTICS POTENTIAL THEORY OF SCHR~DINGEWOPERATOR - BASED -ONFRACTIONAL LABLACIAN 5 BY - Abstract. We develop potential theory of Schrdinger operators based on fractional Laplacian on Euclidean spaces of arbitrary dimen- sion. We focus on questions related to gaugeability and existence of q-harmonic functions. Results are obtained by analyzing properties of a symmetric a-stable Gvy process on Rd, including the recurrent case. We provide some relevant techniques and apply them to give explicit examples of gauge functions for a general class of domains. 1W1 Mathematics Subject Claasificadon: Primary 31B25,60J50. Key words and phrases: symmetric a-stable Gvy process, Feyn- man-Kac semigroup, Schrodinger operator, q-harmonic functions, Kel- vin transform, conditional gauge theorem. 1. INTRODUCTION The paper deals with Schrodinger type operators corresponding to sym- metric a-stable Lbvy processes X,on Rd equipped with a multiplicative func- tional e,(t) = exp (lb q (X.)ds), where q is a given function (in a Kato class). We study the existence and properties of q-harmonic functions. In particular, we address ourselves to problems related to gaugeability. - - Many potential-theoretic properties of X, for aE(0, 2) are dramatically different from those of Brownian motion yet they may be regarded as typical for a general class of LCvy processes on Rd. This motivates a thorough study of the Feynman-Kac semigroups related to the symmetric stable Lbvy processes, especially that the explicit calculations are very often feasible in this particular case, which stimulates and enriches the general theory. Results of this paper complement the earlier ones contained in [6].Results of [6] were basically restricted to bounded Lipschitz domains and were based * Institute of Mathematics, Wroclaw University of Technology. -
Kepler's Area Law in the Principia: Filling in Some Details in Newton's
Historia Mathematica 30 (2003) 441–456 www.elsevier.com/locate/hm Kepler’s area law in the Principia: filling in some details in Newton’s proof of Proposition 1 Michael Nauenberg Department of Physics, University of California, Santa Cruz, CA 95064, USA Abstract During the past 30 years there has been controversy regarding the adequacy of Newton’s proof of Prop. 1 in Book 1 of the Principia. This proposition is of central importance because its proof of Kepler’s area law allowed Newton to introduce a geometric measure for time to solve problems in orbital dynamics in the Principia.Itis shown here that the critics of Prop. 1 have misunderstood Newton’s continuum limit argument by neglecting to consider the justification for this limit which he gave in Lemma 3. We clarify the proof of Prop. 1 by filling in some details left out by Newton which show that his proof of this proposition was adequate and well-grounded. 2003 Elsevier Inc. All rights reserved. Résumé Au cours des 30 dernières années, il y a eu une controverse au sujet de la preuve de la Proposition 1 telle qu’elle est formulée par Newton dans le premier livre de ses Principia. Cette proposition est d’une importance majeure puisque la preuve qu’elle donne de la loi des aires de Kepler permit à Newton d’introduire une expression géometrique du temps, lui permettant ainsi de résoudre des problèmes dans la domaine de la dynamique orbitale. Nous démontrons ici que les critiques de la Proposition 1 ont mal compris l’argument de Newton relatif aux limites continues et qu’ils ont négligé de considérer la justification pour ces limites donnée par Newton dans son Lemme 3. -
Weight Functions on Non-Archimedean Analytic Spaces and the Kontsevich–Soibelman Skeleton
View metadata, citation and similar papers at core.ac.uk brought to you by CORE provided by Spiral - Imperial College Digital Repository Algebraic Geometry 2 (3) (2015) 365{404 doi:10.14231/AG-2015-016 Weight functions on non-Archimedean analytic spaces and the Kontsevich{Soibelman skeleton Mircea Mustat¸˘aand Johannes Nicaise Abstract We associate a weight function to pairs (X; !) consisting of a smooth and proper va- riety X over a complete discretely valued field and a pluricanonical form ! on X. This weight function is a real-valued function on the non-Archimedean analytification of X. It is piecewise affine on the skeleton of any regular model with strict normal crossings of X, and strictly ascending as one moves away from the skeleton. We apply these properties to the study of the Kontsevich{Soibelman skeleton of (X; !), and we prove that this skeleton is connected when X has geometric genus one and ! is a canonical form on X. This result can be viewed as an analog of the Shokurov{Koll´ar connectedness theorem in birational geometry. 1. Introduction 1.1 Skeleta of non-Archimedean spaces An important property of Berkovich spaces over non-Archimedean fields is that, in many geo- metric situations, they can be contracted onto some subspace with piecewise affine structure, a so- called skeleton. These skeleta are usually constructed by choosing appropriate formal models for the space, associating a simplicial complex to the reduction of the formal model and embedding its geometric realization into the Berkovich space. For instance, if C is a smooth projective curve of genus at least two over an algebraically closed non-Archimedean field, then it has a canonical skeleton, which is homeomorphic to the dual graph of the special fiber of its stable model [Ber90, x 4]. -
Absolute Irreducibility of Polynomials Via Newton Polytopes
ABSOLUTE IRREDUCIBILITY OF POLYNOMIALS VIA NEWTON POLYTOPES SHUHONG GAO DEPARTMENT OF MATHEMATICAL SCIENCES CLEMSON UNIVERSITY CLEMSON, SC 29634 USA [email protected] Abstract. A multivariable polynomial is associated with a polytope, called its Newton polytope. A polynomial is absolutely irreducible if its Newton polytope is indecomposable in the sense of Minkowski sum of polytopes. Two general constructions of indecomposable polytopes are given, and they give many simple irreducibility criteria including the well-known Eisenstein’s crite- rion. Polynomials from these criteria are over any field and have the property of remaining absolutely irreducible when their coefficients are modified arbi- trarily in the field, but keeping certain collection of them nonzero. 1. Introduction It is well-known that Eisenstein’s criterion gives a simple condition for a polyno- mial to be irreducible. Over the years this criterion has witnessed many variations and generalizations using Newton polygons, prime ideals and valuations; see for examples [3, 25, 28, 38]. We examine the Newton polygon method and general- ize it through Newton polytopes associated with multivariable polynomials. This leads us to a more general geometric criterion for absolute irreducibility of multi- variable polynomials. Since the Newton polygon of a polynomial is only a small fraction of its Newton polytope, our method is much more powerful. Absolute irre- ducibility of polynomials is crucial in many applications including but not limited to finite geometry [14], combinatorics [47], algebraic geometric codes [45], permuta- tion polynomials [23] and function field sieve [1]. We present many infinite families of absolutely irreducible polynomials over an arbitrary field. These polynomials remain absolutely irreducible even if their coefficients are modified arbitrarily but with certain collection of them nonzero.