The document is Ivan Martino's 2014 doctoral thesis from Stockholm University titled "Ekedahl Invariants, Veronese Modules and Linear Recurrence Varieties". It contains four papers at the intersection of algebraic geometry, commutative algebra, and combinatorics. The first two papers concern new geometric invariants for finite groups called Ekedahl invariants. The third paper discusses a combinatorial approach to studying Veronese modules. The fourth paper shows a recent result relating linear recurrence varieties to numerical semigroups.
This document provides notes for a course on nonlinear subelliptic equations on Carnot groups. The notes begin with an overview of the maximum principle and comparison principle for viscosity solutions of elliptic equations in Euclidean space. It introduces jets and viscosity solutions as a way to extend these principles to nonsmooth functions. Subsequent lectures generalize these ideas to the Heisenberg group and more general Carnot groups.
A general approach is presented to describing nonlinear classical Maxwell electrodynamics with conformal symmetry. We introduce generalized nonlinear constitutive equations, expressed in terms of constitutive tensors dependent on conformal-invariant functionals of the field strengths. This allows a characterization of Lagrangian and non-Lagrangian theories. We obtain a general formula for possible Lagrangian densities in nonlinear conformal-invariant electrodynamics. This generalizes the standard Lagrangian of classical linear electrodynamics so as to preserve the conformal symmetry.
This document summarizes Michael Kreisel's dissertation on the connection between Gabor frames for quasicrystals, the topology of the hull of a quasicrystal, and K-theory of an associated twisted groupoid algebra. The author constructs a finitely generated projective module over this algebra, where any multiwindow Gabor frame for the quasicrystal can be used to construct a projection representing this module in K-theory. As an application, results are obtained on the twisted version of Bellissard's gap labeling conjecture for quasicrystals.
Singula holomorphic foliations on cp3 shfc zakFrancisco Inuma
This document provides an introduction to singular holomorphic foliations on the complex projective plane CP2. It discusses how viewing real differential equations as complex equations allows applying methods of complex analysis and algebraic geometry. Specifically, it summarizes influential work by Il'yashenko in 1978 studying properties of integral curves of such equations from a topological standpoint. It also introduces the concept of monodromy mapping, which generalizes the Poincaré first return map and plays a key role in the dynamics of singular holomorphic foliations on CP2.
Geometric properties for parabolic and elliptic pdeSpringer
This document discusses recent advances in fractional Laplacian operators and related problems in partial differential equations and geometric measure theory. Specifically, it addresses three key topics:
1. Symmetry problems for solutions of the fractional Allen-Cahn equation and whether solutions only depend on one variable like in the classical case. The answer is known to be positive for some dimensions and fractional exponents but remains open in general.
2. The Γ-convergence of functionals involving the fractional Laplacian as the small parameter ε approaches zero. This characterizes the asymptotic behavior and relates to fractional notions of perimeter.
3. Regularity of interfaces as the fractional exponent s approaches 1/2 from above, which corresponds to a critical threshold
11.coupled fixed point theorems in partially ordered metric spaceAlexander Decker
The document presents two theorems proving the existence of coupled fixed points for mappings in partially ordered metric spaces. Specifically:
1. Theorem 3.1 proves that if a mapping has the mixed monotone property and satisfies a contraction condition, then it has a coupled fixed point.
2. Theorem 3.2 also proves the existence of a coupled fixed point for mappings with the mixed monotone property satisfying a contraction condition.
Both theorems construct Cauchy sequences to prove the existence of a coupled fixed point based on the mapping's properties in a complete partially ordered metric space.
On the Numerical Fixed Point Iterative Methods of Solution for the Boundary V...BRNSS Publication Hub
In this research work, we have studied the finite difference method and used it to solve elliptic partial differential equation (PDE). The effect of the mesh size on typical elliptic PDE has been investigated. The effect of tolerance on the numerical methods used, speed of convergence, and number of iterations was also examined. Three different elliptic PDE’s; the Laplace’s equation, Poisons equation with the linear inhomogeneous term, and Poisons equations with non-linear inhomogeneous term were used in the study. Computer program was written and implemented in MATLAB to carry out lengthy calculations. It was found that the application of the finite difference methods to an elliptic PDE transforms the PDE to a system of algebraic equations whose coefficient matrix has a block tri-diagonal form. The analysis carried out shows that the accuracy of solutions increases as the mesh is decreased and that the solutions are affected by round off errors. The accuracy of solutions increases as the number of the iterations increases, also the more efficient iterative method to use is the SOR method due to its high degree of accuracy and speed of convergence
This document discusses stochastic partial differential equations (SPDEs). It outlines several approaches that have been used to solve SPDEs, including methods based on diffusion processes, stochastic characteristic systems, direct methods from mathematical physics, and substitution of integral equations. It also discusses using backward stochastic differential equations to study SPDEs and introduces notation for the analysis of an Ito SDE with inverse time. The document is technical in nature and outlines the mathematical frameworks and equations involved in solving SPDEs through various probabilistic methods.
This document provides notes for a course on nonlinear subelliptic equations on Carnot groups. The notes begin with an overview of the maximum principle and comparison principle for viscosity solutions of elliptic equations in Euclidean space. It introduces jets and viscosity solutions as a way to extend these principles to nonsmooth functions. Subsequent lectures generalize these ideas to the Heisenberg group and more general Carnot groups.
A general approach is presented to describing nonlinear classical Maxwell electrodynamics with conformal symmetry. We introduce generalized nonlinear constitutive equations, expressed in terms of constitutive tensors dependent on conformal-invariant functionals of the field strengths. This allows a characterization of Lagrangian and non-Lagrangian theories. We obtain a general formula for possible Lagrangian densities in nonlinear conformal-invariant electrodynamics. This generalizes the standard Lagrangian of classical linear electrodynamics so as to preserve the conformal symmetry.
This document summarizes Michael Kreisel's dissertation on the connection between Gabor frames for quasicrystals, the topology of the hull of a quasicrystal, and K-theory of an associated twisted groupoid algebra. The author constructs a finitely generated projective module over this algebra, where any multiwindow Gabor frame for the quasicrystal can be used to construct a projection representing this module in K-theory. As an application, results are obtained on the twisted version of Bellissard's gap labeling conjecture for quasicrystals.
Singula holomorphic foliations on cp3 shfc zakFrancisco Inuma
This document provides an introduction to singular holomorphic foliations on the complex projective plane CP2. It discusses how viewing real differential equations as complex equations allows applying methods of complex analysis and algebraic geometry. Specifically, it summarizes influential work by Il'yashenko in 1978 studying properties of integral curves of such equations from a topological standpoint. It also introduces the concept of monodromy mapping, which generalizes the Poincaré first return map and plays a key role in the dynamics of singular holomorphic foliations on CP2.
Geometric properties for parabolic and elliptic pdeSpringer
This document discusses recent advances in fractional Laplacian operators and related problems in partial differential equations and geometric measure theory. Specifically, it addresses three key topics:
1. Symmetry problems for solutions of the fractional Allen-Cahn equation and whether solutions only depend on one variable like in the classical case. The answer is known to be positive for some dimensions and fractional exponents but remains open in general.
2. The Γ-convergence of functionals involving the fractional Laplacian as the small parameter ε approaches zero. This characterizes the asymptotic behavior and relates to fractional notions of perimeter.
3. Regularity of interfaces as the fractional exponent s approaches 1/2 from above, which corresponds to a critical threshold
11.coupled fixed point theorems in partially ordered metric spaceAlexander Decker
The document presents two theorems proving the existence of coupled fixed points for mappings in partially ordered metric spaces. Specifically:
1. Theorem 3.1 proves that if a mapping has the mixed monotone property and satisfies a contraction condition, then it has a coupled fixed point.
2. Theorem 3.2 also proves the existence of a coupled fixed point for mappings with the mixed monotone property satisfying a contraction condition.
Both theorems construct Cauchy sequences to prove the existence of a coupled fixed point based on the mapping's properties in a complete partially ordered metric space.
On the Numerical Fixed Point Iterative Methods of Solution for the Boundary V...BRNSS Publication Hub
In this research work, we have studied the finite difference method and used it to solve elliptic partial differential equation (PDE). The effect of the mesh size on typical elliptic PDE has been investigated. The effect of tolerance on the numerical methods used, speed of convergence, and number of iterations was also examined. Three different elliptic PDE’s; the Laplace’s equation, Poisons equation with the linear inhomogeneous term, and Poisons equations with non-linear inhomogeneous term were used in the study. Computer program was written and implemented in MATLAB to carry out lengthy calculations. It was found that the application of the finite difference methods to an elliptic PDE transforms the PDE to a system of algebraic equations whose coefficient matrix has a block tri-diagonal form. The analysis carried out shows that the accuracy of solutions increases as the mesh is decreased and that the solutions are affected by round off errors. The accuracy of solutions increases as the number of the iterations increases, also the more efficient iterative method to use is the SOR method due to its high degree of accuracy and speed of convergence
This document discusses stochastic partial differential equations (SPDEs). It outlines several approaches that have been used to solve SPDEs, including methods based on diffusion processes, stochastic characteristic systems, direct methods from mathematical physics, and substitution of integral equations. It also discusses using backward stochastic differential equations to study SPDEs and introduces notation for the analysis of an Ito SDE with inverse time. The document is technical in nature and outlines the mathematical frameworks and equations involved in solving SPDEs through various probabilistic methods.
Solution of a subclass of lane emden differential equation by variational ite...Alexander Decker
This document discusses applying He's variational iteration method to solve a subclass of Lane-Emden differential equations. The method constructs a sequence of correction functionals that generate iterative approximations to the solution. It is shown that under certain conditions, the iterative sequence converges to the exact solution of the Lane-Emden equation. The variational iteration method provides an efficient means of obtaining polynomial solutions without linearization, perturbation or discretization. Illustrative examples from literature are shown to produce exact polynomial solutions when treated with this method.
11.solution of a subclass of lane emden differential equation by variational ...Alexander Decker
This document discusses applying He's variational iteration method to solve a subclass of Lane-Emden differential equations. The method constructs a sequence of correction functionals that generate iterative approximations to the solution. It is shown that under certain conditions, the iterative sequence converges to the exact solution of the Lane-Emden equation. The variational iteration method provides an efficient means of obtaining analytical solutions and has been successfully used to solve many types of nonlinear problems. The method is illustrated through examples and shown to produce polynomial solutions.
This is a journal concise version (without diagrams and figures) of the preprint arXiv:1308.4060.
Abstract: Polyadic systems and their representations are reviewed and a classification of general polyadic systems is presented. A new multiplace generalization of associativity preserving homomorphisms, a 'heteromorphism' which connects polyadic systems having unequal arities, is introduced via an explicit formula, together with related definitions for multiplace representations and multiactions. Concrete examples of matrix representations for some ternary groups are then reviewed. Ternary algebras and Hopf algebras are defined, and their properties are studied. At the end some ternary generalizations of quantum groups and the Yang-Baxter equation are presented.
Successive approximation of neutral stochastic functional differential equati...Editor IJCATR
We establish results concerning the existence and uniqueness of solutions to neutral stochastic functional differential
equations with infinite delay and Poisson jumps in the phase space C((-∞,0];Rd) under non-Lipschitz condition with Lipschitz
condition being considered as a special case and a weakened linear growth condition on the coefficients by means of the successive
approximation. Compared with the previous results, the results obtained in this paper is based on a other proof and our results can
complement the earlier publications in the existing literatures.
Deductivereasoning and bicond and algebraic proof updated 2014sjbianco9910
This document contains a geometry lesson on biconditional statements, definitions, and deductive reasoning. It includes examples of writing conditional statements, converses, and biconditional statements. It also discusses using deductive reasoning to write geometric proofs through solving equations and identifying properties of equality and congruence. The document provides examples of writing definitions as biconditional statements and using properties of equality and congruence to justify steps in proofs. It concludes with a quiz reviewing the concepts covered in the lesson.
A Study of Permutation Groups and Coherent ConfigurationsJohn Batchelor
This document provides historical background on the study of permutation groups. It discusses how Lagrange initially studied permutations when solving polynomial equations. Later, Galois connected permutation groups to field theory by introducing Galois groups. The document also mentions contributions from mathematicians like Burnside, Frobenius, and Jordan that advanced the theory of permutation groups.
A presentation slide of the paper "Doubly Decomposing Nonparametric Tensor Regression" (Imaizumi & Hayashi 2016 ICML).
Full paper
http://www.jmlr.org/proceedings/papers/v48/imaizumi16.html
This document summarizes recent results from Mircea-Dan Hernest's PhD thesis on optimizing proof-theoretic techniques used by Ulrich Kohlenbach for extracting bounds from proofs in analysis. Specifically, it explores adapting Kohlenbach's "light monotone Dialectica" interpretation to proofs involving "non-computational" quantifiers. It describes how ε-arithmetization, elimination of extensionality, and model interpretation can be applied in this "non-computational" setting while maintaining certain restrictions. The goal is to more efficiently extract moduli from a larger class of non-trivial analytical proofs.
Microsoft Office 2013 is a version of the office suite for Windows designed to be used on touchscreen devices. It features new reading and collaboration tools as well as the ability to open and edit PDF files directly. The document provides instructions on how to create, save, open, and close documents in Word 2013. It also explains how to insert shapes, numbers, audio/video, headers, footers, endnotes, and equations. Formatting options like font style and size are also discussed.
Kelsall Swiftsure Sandwich (KSS) is a boat building system developed by Kelsall Catamarans using foam and fiberglass. It allows builders to start with flat panels and produce the curved hull shapes through a process of shaping and assembly. KSS aims to reduce build time by at least half compared to traditional methods by laminating panels on a table and assembling the boat from a kit of pre-made parts. The system has been refined over many years and can be used to build catamarans of all sizes from 8 to over 100 feet.
Eating a balanced diet provides nutrients that give the body energy and support various bodily functions. Nutrients help build bones, muscles, and tendons and regulate processes like blood pressure. The document then provides examples of recommended daily servings from various food groups, including vegetables, fruits, grains, proteins, dairy, fats, beans and nuts. It also lists some traditional Bulgarian dishes and describes some key Bulgarian holidays, their associated fasting traditions and characteristic meals, such as the coin-filled bread of Christmas Eve and the fish-based meal of Nikulden.
Eating a healthy, balanced diet provides nutrients that give the body energy and support important bodily functions like heart function, brain activity, and muscle movement. Nutrients also help build and maintain bones, muscles, and tendons, and regulate processes such as blood pressure. The document then provides examples of recommended daily servings from various food groups to achieve a balanced diet.
This document discusses key concepts that were explored by a teen philanthropy program over the past year, including team work, zeal, education, dedication, ability to make a difference, honor, respect, action, and loving kindness. When combined, these qualities form the heart of the program. This year, the teen advisors of the Iris Teen Tzedakah program allocated over $XX,XXX in contributions to agencies in the Greater MetroWest area and beyond.
Summary and celebration of the 3rd cohort of the SeniorITIS program, run by the Partnership for Jewish Learning and Life and organized by Michael Strom, Ast. Service Coordinator. SeniorITIS is made possible through a generous donation provided by the Cooperman Family Fund for a Jewish Future.
The document introduces a proposed Learning Commons that would shift away from traditional library and computer lab models. It argues that students today need an environment that fosters critical and creative thinking as well as skills like collaboration and problem solving. The Learning Commons is described as both a physical space and a new perspective on learning. It would be designed based on research and with input from students, staff, and parents to create an easy access, student-centered academic space beyond traditional classrooms. The school is currently in the consultation and funding stages of developing their Learning Commons.
1) O documento é uma edição de um jornal local que contém notícias sobre política e acontecimentos de várias cidades da região, incluindo encontros, projetos de lei e entrevistas com políticos locais.
2) O prefeito de Sombrio concedeu entrevista coletiva para esclarecer detalhes e benefícios de um projeto de parceria entre o município e a Casan para gestão compartilhada de saneamento básico.
3) Em Jacinto Machado, um evento reuniu cerca de 1
This document presents a summary of research on finding recurrence relations in electromagnetic scattering calculations. Recurrence relations can reduce the dimensionality and complexity of calculations using the T-matrix method. The researchers examined integrals of vector spherical harmonics (K1, K2, L1, L2) involved in T-matrix calculations and found relationships between them. These relationships were expressed as equations relating a combination of the integrals. Future work aims to leverage these relations to more efficiently compute T-matrices by reducing the number of integrals that must be directly evaluated.
3 O Dnit retoma trabalhos de manutenção na BR-101 no Extremo Sul catarinense, com limpeza, tapa-buracos e outros serviços.
3 Uma família em Sombrio procura por um adolescente que desapareceu após sair de casa para uma volta.
3 Em Araranguá, o prefeito fará mudanças em secretarias municipais, com trocas em pastas como Saúde e Governo.
This document provides an overview of media and journalism in Brazil. It discusses that Brazil has a large media market but that journalism is facing a crisis due to economic pressures and competition from new technologies. Investigative journalism is under threat and Brazil has become the deadliest country for media personnel in the Western Hemisphere. Recent large protests in 2013 highlighted issues with the dominant media model and methods still used by state police. The future of journalism in Brazil will depend on continued democratization and economic reforms, as well as building public trust through integrity.
Solution of a subclass of lane emden differential equation by variational ite...Alexander Decker
This document discusses applying He's variational iteration method to solve a subclass of Lane-Emden differential equations. The method constructs a sequence of correction functionals that generate iterative approximations to the solution. It is shown that under certain conditions, the iterative sequence converges to the exact solution of the Lane-Emden equation. The variational iteration method provides an efficient means of obtaining polynomial solutions without linearization, perturbation or discretization. Illustrative examples from literature are shown to produce exact polynomial solutions when treated with this method.
11.solution of a subclass of lane emden differential equation by variational ...Alexander Decker
This document discusses applying He's variational iteration method to solve a subclass of Lane-Emden differential equations. The method constructs a sequence of correction functionals that generate iterative approximations to the solution. It is shown that under certain conditions, the iterative sequence converges to the exact solution of the Lane-Emden equation. The variational iteration method provides an efficient means of obtaining analytical solutions and has been successfully used to solve many types of nonlinear problems. The method is illustrated through examples and shown to produce polynomial solutions.
This is a journal concise version (without diagrams and figures) of the preprint arXiv:1308.4060.
Abstract: Polyadic systems and their representations are reviewed and a classification of general polyadic systems is presented. A new multiplace generalization of associativity preserving homomorphisms, a 'heteromorphism' which connects polyadic systems having unequal arities, is introduced via an explicit formula, together with related definitions for multiplace representations and multiactions. Concrete examples of matrix representations for some ternary groups are then reviewed. Ternary algebras and Hopf algebras are defined, and their properties are studied. At the end some ternary generalizations of quantum groups and the Yang-Baxter equation are presented.
Successive approximation of neutral stochastic functional differential equati...Editor IJCATR
We establish results concerning the existence and uniqueness of solutions to neutral stochastic functional differential
equations with infinite delay and Poisson jumps in the phase space C((-∞,0];Rd) under non-Lipschitz condition with Lipschitz
condition being considered as a special case and a weakened linear growth condition on the coefficients by means of the successive
approximation. Compared with the previous results, the results obtained in this paper is based on a other proof and our results can
complement the earlier publications in the existing literatures.
Deductivereasoning and bicond and algebraic proof updated 2014sjbianco9910
This document contains a geometry lesson on biconditional statements, definitions, and deductive reasoning. It includes examples of writing conditional statements, converses, and biconditional statements. It also discusses using deductive reasoning to write geometric proofs through solving equations and identifying properties of equality and congruence. The document provides examples of writing definitions as biconditional statements and using properties of equality and congruence to justify steps in proofs. It concludes with a quiz reviewing the concepts covered in the lesson.
A Study of Permutation Groups and Coherent ConfigurationsJohn Batchelor
This document provides historical background on the study of permutation groups. It discusses how Lagrange initially studied permutations when solving polynomial equations. Later, Galois connected permutation groups to field theory by introducing Galois groups. The document also mentions contributions from mathematicians like Burnside, Frobenius, and Jordan that advanced the theory of permutation groups.
A presentation slide of the paper "Doubly Decomposing Nonparametric Tensor Regression" (Imaizumi & Hayashi 2016 ICML).
Full paper
http://www.jmlr.org/proceedings/papers/v48/imaizumi16.html
This document summarizes recent results from Mircea-Dan Hernest's PhD thesis on optimizing proof-theoretic techniques used by Ulrich Kohlenbach for extracting bounds from proofs in analysis. Specifically, it explores adapting Kohlenbach's "light monotone Dialectica" interpretation to proofs involving "non-computational" quantifiers. It describes how ε-arithmetization, elimination of extensionality, and model interpretation can be applied in this "non-computational" setting while maintaining certain restrictions. The goal is to more efficiently extract moduli from a larger class of non-trivial analytical proofs.
Microsoft Office 2013 is a version of the office suite for Windows designed to be used on touchscreen devices. It features new reading and collaboration tools as well as the ability to open and edit PDF files directly. The document provides instructions on how to create, save, open, and close documents in Word 2013. It also explains how to insert shapes, numbers, audio/video, headers, footers, endnotes, and equations. Formatting options like font style and size are also discussed.
Kelsall Swiftsure Sandwich (KSS) is a boat building system developed by Kelsall Catamarans using foam and fiberglass. It allows builders to start with flat panels and produce the curved hull shapes through a process of shaping and assembly. KSS aims to reduce build time by at least half compared to traditional methods by laminating panels on a table and assembling the boat from a kit of pre-made parts. The system has been refined over many years and can be used to build catamarans of all sizes from 8 to over 100 feet.
Eating a balanced diet provides nutrients that give the body energy and support various bodily functions. Nutrients help build bones, muscles, and tendons and regulate processes like blood pressure. The document then provides examples of recommended daily servings from various food groups, including vegetables, fruits, grains, proteins, dairy, fats, beans and nuts. It also lists some traditional Bulgarian dishes and describes some key Bulgarian holidays, their associated fasting traditions and characteristic meals, such as the coin-filled bread of Christmas Eve and the fish-based meal of Nikulden.
Eating a healthy, balanced diet provides nutrients that give the body energy and support important bodily functions like heart function, brain activity, and muscle movement. Nutrients also help build and maintain bones, muscles, and tendons, and regulate processes such as blood pressure. The document then provides examples of recommended daily servings from various food groups to achieve a balanced diet.
This document discusses key concepts that were explored by a teen philanthropy program over the past year, including team work, zeal, education, dedication, ability to make a difference, honor, respect, action, and loving kindness. When combined, these qualities form the heart of the program. This year, the teen advisors of the Iris Teen Tzedakah program allocated over $XX,XXX in contributions to agencies in the Greater MetroWest area and beyond.
Summary and celebration of the 3rd cohort of the SeniorITIS program, run by the Partnership for Jewish Learning and Life and organized by Michael Strom, Ast. Service Coordinator. SeniorITIS is made possible through a generous donation provided by the Cooperman Family Fund for a Jewish Future.
The document introduces a proposed Learning Commons that would shift away from traditional library and computer lab models. It argues that students today need an environment that fosters critical and creative thinking as well as skills like collaboration and problem solving. The Learning Commons is described as both a physical space and a new perspective on learning. It would be designed based on research and with input from students, staff, and parents to create an easy access, student-centered academic space beyond traditional classrooms. The school is currently in the consultation and funding stages of developing their Learning Commons.
1) O documento é uma edição de um jornal local que contém notícias sobre política e acontecimentos de várias cidades da região, incluindo encontros, projetos de lei e entrevistas com políticos locais.
2) O prefeito de Sombrio concedeu entrevista coletiva para esclarecer detalhes e benefícios de um projeto de parceria entre o município e a Casan para gestão compartilhada de saneamento básico.
3) Em Jacinto Machado, um evento reuniu cerca de 1
This document presents a summary of research on finding recurrence relations in electromagnetic scattering calculations. Recurrence relations can reduce the dimensionality and complexity of calculations using the T-matrix method. The researchers examined integrals of vector spherical harmonics (K1, K2, L1, L2) involved in T-matrix calculations and found relationships between them. These relationships were expressed as equations relating a combination of the integrals. Future work aims to leverage these relations to more efficiently compute T-matrices by reducing the number of integrals that must be directly evaluated.
3 O Dnit retoma trabalhos de manutenção na BR-101 no Extremo Sul catarinense, com limpeza, tapa-buracos e outros serviços.
3 Uma família em Sombrio procura por um adolescente que desapareceu após sair de casa para uma volta.
3 Em Araranguá, o prefeito fará mudanças em secretarias municipais, com trocas em pastas como Saúde e Governo.
This document provides an overview of media and journalism in Brazil. It discusses that Brazil has a large media market but that journalism is facing a crisis due to economic pressures and competition from new technologies. Investigative journalism is under threat and Brazil has become the deadliest country for media personnel in the Western Hemisphere. Recent large protests in 2013 highlighted issues with the dominant media model and methods still used by state police. The future of journalism in Brazil will depend on continued democratization and economic reforms, as well as building public trust through integrity.
A recurrence relation defines a sequence based on a rule that gives the next term as a function of previous terms. There are three main methods to solve recurrence relations: 1) repeated substitution, 2) recursion trees, and 3) the master method. Repeated substitution repeatedly substitutes the recursive function into itself until it is reduced to a non-recursive form. Recursion trees show the successive expansions of a recurrence using a tree structure. The master method provides rules to determine the time complexity of divide and conquer recurrences.
To solve a linear recurrence equation, find the characteristic roots by setting the characteristic equation equal to 0. The characteristic equation for the given equation xn+2 + 2xn+1 - 24xn = 0 is λ2 + 2λ - 24 = 0, with characteristic roots of -6 and 4. The general solution is then xn = C1(-6)n + C24n, which is a linear combination of the basis sequences with the characteristic roots.
This document discusses recurrence relations and their use in defining sequences. It introduces key concepts like recurrence relations, initial conditions, explicit formulas, and solving recurrence relations using techniques like backtracking or finding the characteristic equation. As examples, it examines the Fibonacci sequence and linear homogeneous recurrence relations of varying degrees.
This document provides information about recurrence relations and their applications in higher mathematics. It begins by introducing different types of sequences and exploring whether they can be described by a formula or recurrence relation. It then discusses linear recurrence relations and how they can model growth and decay scenarios. The document also covers divergence and convergence of sequences, and provides examples of applying recurrence relations to problems involving populations, waste disposal, medication in hospitals, and other scenarios.
1) O prefeito de Sombrio anunciou a demissão de 64 funcionários públicos e abriu mão de seu próprio salário para adequar as finanças da prefeitura à realidade orçamentária.
2) O prefeito de São João do Sul solicitou recursos emergenciais ao governo estadual para a saúde municipal, que deixou de ter condições de arcar com os custos.
3) O deputado José Milton Scheffer viabilizou um convênio de R$ 200 mil para iniciar a pavimentação de uma rodovia em Bal
The document discusses recurrence relations and their applications. It begins by defining a recurrence relation as an equation that expresses the terms of a sequence in terms of previous terms. It provides examples of recurrence relations and their solutions. It then discusses solving linear homogeneous recurrence relations with constant coefficients by finding the characteristic roots and obtaining an explicit formula. Applications discussed include financial recurrence relations, the partition function, binary search, and the Fibonacci numbers. It concludes by discussing the case when the characteristic equation has a single root.
3 As paróquias que atendem comunidades do litoral intensificam as missas na praia para acolher moradores e veranistas durante o verão. Uma igreja em Balneário Gaivota realiza a Campanha das Talhas de Caná, com missas lotadas todas as noites.
3 A Igreja Matriz de Maracajá reabriu após reformas estruturais depois de ser interditada por risco de desabamento.
3 O Dnit concluiu obras de recuperação do asfalto e construção de três novos retorn
This document provides a preface and table of contents for a book on the theory of polynomials. The preface outlines the book's contents, which include discussions of roots of polynomials, irreducible polynomials, special classes of polynomials, properties of polynomials, Galois theory, Hilbert's theorems, and Hilbert's 17th problem on representing nonnegative polynomials as sums of squares. The table of contents provides further details on the chapters and sections.
The document summarizes 18 important mathematical problems for the next century as identified by Steve Smale. Some of the key problems discussed include:
1) The Riemann Hypothesis concerning the distribution of primes.
2) The Poincaré Conjecture regarding classifying 3-dimensional spaces.
3) The famous P vs. NP problem about the difference between solving and verifying solutions to problems.
This document summarizes research on simplifying calculations of scattering amplitudes, especially for tree-level amplitudes. It introduces the spinor-helicity formalism for writing compact expressions for amplitudes. It then discusses color decomposition in SU(N) gauge theory and the Yang-Mills Lagrangian. Specific techniques explored include BCFW recursion relations, an inductive proof of the Parke-Taylor formula, the 4-graviton amplitude and KLT relations, multi-leg shifts, and the MHV vertex expansion. The goal is to develop recursion techniques that vastly simplify calculations compared to traditional Feynman diagrams.
This document discusses categories of topological spaces and their isomorphism to categories of relational algebras for a monad. It begins with introductions to the topic and tools used, including categories, functors, natural transformations, monads, and relational algebras. The main content is divided into multiple parts, exploring the proposition that the category of topological spaces is isomorphic to the category of relational algebras. It concludes by restating the aim to formally prove this result using relational calculus.
This document provides an introduction to group theory with applications to quantum mechanics and solid state physics. It begins with definitions of groups and examples of groups that are important in physics. It then discusses several applications of group theory in classical mechanics, quantum mechanics, and solid state physics. Specifically, it explains how group theory can be used to evaluate matrix elements, understand degeneracies of energy eigenvalues, classify electronic states in periodic potentials, and construct models that respect crystal symmetries. It also briefly discusses the use of group theory in nuclear and particle physics.
This document provides an introduction to group theory from a physicist's perspective. It defines what a group is, including properties like closure, associativity, identity, and inverse. Examples of important groups in physics are given, including finite groups like Zn and Sn, and continuous groups like SU(n), SO(n), and the Lorentz group. The document outlines topics like discrete and finite groups, representation of groups, Lie groups and algebras, and applications of specific groups like SU(2) and SU(3) to physics.
Algebraic topology of finite topological spaces and applications sisirose
This presentation of the theory of finite topological spaces includes the
most fundamental ideas and results previous to our work and, mainly, our
contributions over the last years. It is intended for topologists and combinatorialists,
but since it is a self-contained exposition, it is also recommended
for advanced undergraduate students and graduate students with a modest
knowledge of Algebraic Topology.
This document is a literature review for a project on modeling fluid dynamics using spectral methods in MATLAB. It summarizes two key papers: (1) Balmforth et al.'s paper on modeling the dynamics of interfaces and layers in a stratified turbulent fluid, which derived coupled differential equations; and (2) Trefethen's book on spectral methods in MATLAB, which provided guidance on using Chebyshev polynomials and differentiation matrices. It also outlines the methodology used in Balmforth et al.'s paper and chapters from Trefethen's book on finite differences, Chebyshev points, and constructing Chebyshev differentiation matrices.
The document presents research on using a binary reproducing kernel Hilbert space (RKHS) approach to solve a Wick-type stochastic Korteweg-de Vries (KdV) equation with variable coefficients. It introduces the stochastic KdV equation model and discusses previous work analyzing it. The research aims to formulate white noise functional solutions for the stochastic KdV equations by applying Hermite transform, white noise theory, and binary RKHS. It explores representing the exact solution in a reproducing kernel space and investigating uniform convergence of approximate solutions.
This document discusses how catastrophe theory can be applied to physical systems using manifolds. It describes how potential functions from catastrophe theory can influence manifolds that are locally like 4D Euclidean space. Seven catastrophes from Thom's theory are structurally stable. In addition to catastrophe manifolds, other manifolds can arise without polar singularities or with a diagonal metric. Complex numbers, quaternions, and octonions can be added to the 4D space. Applications to bifurcations, measuring frames, particles, and effects on systems are discussed.
Some new exact Solutions for the nonlinear schrödinger equationinventy
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1. Ekedahl Invariants,
Veronese Modules and
Linear Recurrence Varieties
Ivan Martino
Doctoral Thesis in Mathematics at Stockholm University, Sweden 2014
8. Acknowledgements
I am very pleased and honored to have been given the opportunity to work with
Anders Björner, Torsten Ekedahl and Ralf Fröberg: three completely different
styles of doing mathematics and of being mathematicians.
First, I have to thank Torsten Ekedahl. Looking backward, I can see how
much I have learned from him. He has been an inspiration for me and it always
will be.
Then, I really thank my supervisor Anders Björner. He provided me a great
support and helped me to grow as a mathematician and as a person.
Last but not the least, I want to thank Ralf Fröberg. It is difficult to sum-marize
all the experiences I had with Ralf: conferences, discussions, fika, ...
but for all of them I really thank Ralf.
I am also grateful to Angelo Vistoli who took me as one of his students
during a visiting semester in Pisa.
Special thanks go to Alexander Engström, Boris Shapiro, Bruno Benedetti,
Jörgen Backelin, Mats Boji and Matthew Stamps, because they spent a lot of
time with me and I really thank them for this.
During my doctoral studies I met amazing people. My life in Stockholm
started with two Alessandro’s and Carlo: we shared the first steps into a new
unknown country. Then, my walk continued with Yohannes and Johan, won-derful
officemates. A big hug goes also to Kerstin, very important friend.
My life would be different without Alessandro (yes another one!) and
Olof: they have been incredible colleagues and we shared a really warm room!
Similarly, I have to thank (in random order) Afshin, Tony, Christian, Sarah,
Pinar, Martina, Rune, Stefano, Ketil, Christopher, Jens, Björn and Felix.
I am so deep in debt to my dear friends in Pisa: Augusto, Fabio, Federico,
Iga, LaFrancesca, Marco and Simone. Moreover, I also need to mention the
friends at the GIH-pool: Anna, Arianna, Bettina, Carolina, Dan, Ellinor, Jonas,
Michael, Nina, Patricia, Peter, Oxana and Stefanie. In particular a thank goes
to my diving friend Alexander.
Finally, I specially thank Ornella. I shared and I share with her all my
moments, sad or happy: you are all for me!
9.
10. List of Papers
The following papers, referred to in the text by their Capital letters, are in-cluded
in this thesis.
PAPER A: Introduction to the Ekedahl invariants
Ivan Martino, Submitted.
PAPER B: The Ekedahl Invariants for finite groups
Ivan Martino, Submitted.
PAPER C: Syzygies of Veronese Modules
Ornella Greco, Ivan Martino, Submitted.
PAPER D: On the variety of linear recurrences and numerical semigroups
Ivan Martino, Luca Martino, Semigroup Forum, Vol. 87, Issue 3
(2013) DOI: 10.1007/s00233-013-9551-2.
14. 1. Introduction
This work is a collection of four papers at the intersection of Algebraic Geo-metry,
Commutative Algebra and Combinatorics. The first two concern certain
new geometric invariants for finite groups due to Torsten Ekedahl. The third
one discusses a combinatorial approach to the study of Veronese modules. The
last one shows a recent result on linear recurrence varieties via the use of nu-merical
semigroups.
For this reason, the introduction is made of three parts: the Ekedahl invari-ants,
the Veronese modules and the linear recurrence varieties.
In each of these parts, there is a preliminary section where I try to describe
informally some of the concepts I will use. I give room to historical facts,
general knowledge and I set up notations. These preliminary parts should be
viewed as a short handbook for the results in the papers.
After these preliminaries, I conclude each section by highlighting my main
results in these topics.
13
15. 1.1 The Ekedahl Invariants
I begin by focusing on the Noether Problem and on the Bogomolov multiplier
and I try to blaze a trail from these to the recent research developments. I
give a definition of Ekedahl invariants not involving the theory of algebraic
stacks, because they can be defined in terms of classical geometry and, in
this version, the concept may be useful to a wider audience. All the known
examples where the Ekedahl invariants are nontrivial are counterexamples to
the Noether Problem, because the second Ekedahl invariant is equal to the class
of the dual of the Bogomolov multiplier in a Grothendieck type structure.
The study of the Ekedahl invariants is contained in works A and B. In the
first work I set up all the details one needs in Paper B. I also give a non-stacky
introduction to the Ekedahl invariants, because not all the technical notions of
the theory of algebraic stacks are necessary to work with these new invariants.
In Paper B, I study the Ekedahl invariants for the finite subgroups of GLn(C)
(in particular aiming to answer Question 1 in Section 1.1.1). Then I focus on
the discrete Heisenberg group Hp (see Questions 2 in Section 1.1.1).
1.1.1 Preliminaries
The Noether problem
Let F be a field, G be a finite group and F(xg : g 2 G) be the field of rational
functions with variables indexed by the elements of the group G. One sets
the G-action on F(xg : g 2 G) via h xg = xhg and so we consider the field of
invariants F(xg : g 2 G)G. In 1914, Amalie Emmy Noether wondered if the
field extension F F(xg : g 2 G)G is rational (i.e. purely transcendental).
To fix the idea let us consider an easy example. Let F = Q and G = Z=2Z.
The identity of Z=2Z acts on Q(x0;x1) by fixing both variables and the other ele-ment
switches them. The extension Q(x0;x1)Z=2Z Q(x0;x1) is proper because
x0 =2 Q(x0;x1)Z=2Z. One observes that x0+x1 and x0x1 are invariants generating
Q(x0;x1)Z=2Z. Therefore, the extension Q Q(x0;x1)Z=2Z is rational.
A positive answer to the Noether problem was conjectured until the break-through
result of of Swan [17] in 1969:
«... the conjecture has proved to be extremely intractable. I will
show here that there is a good reason for this. The conjecture is
false even in the simplest case of a cyclic permutation group ...».
Indeed, he proved that the extension Q Q(xg : g 2 Z=pZ)Z=pZ is not rational
for p = 47;113 and 233.
After this, a lot of effort was spent on the Noether problem, but one had
to wait for Saltman’s result [16] in 1984 to get a more complete picture. He
14
16. proved that for any field F and for any prime p with (charF; p) = 1, there
exists a group G of order p9 such that F F(xg : g 2 G)G is not rational. To
get his goal, Saltman used a cohomological invariant introduced by Artin and
Mumford [1].
In [3], Bogomolov improved Saltman’s statement from p9 to p6 by show-ing
a concrete way to compute this invariant, that is now called Bogomolov
multiplier and denoted by B0(G): it is a cohomological obstruction to the ra-tionality
of F(xg : g 2 G)G=F. In other words, the vanishing of B0(G) is a
necessary condition for the rationality of F(xg : g 2 G)G=F.
He proved that the Bogomolov multiplier is a subgroup of H2 (G;C), de-fined
as the cohomology classes in H2 (G;C) such that their restrictions to any
abelian subgroup of G is zero. This means that
B0(G) =
A
Ker
H2 (G;C))!H2 (A;C)
;
where the intersection runs over the abelian subgroups A G.
A question in the Kontsevich value ring
Let k be an algebraically closed field of characteristic zero. The Grothendieck
group of varieties K0(Vark) is the group generated by the isomorphism classes
fXg of algebraic k-varieties X modulo the relation
fXg = fZg+fX nZg;
for every closed subvariety Z of X. If one sets
fXgfYg = fX Yg;
then K0(Vark) has also a ring structure.
We denote by L = fA1
kg, the class of the affine line (called Lefschetz class).
The Motivic ring is the localization K0(Vark)[L1]. One can also define a
filtration
Filn
= ffXg=Li : dimX i ng:
K0(Vark)[L1]
The Kontsevich value ringcK0(Vark) is the completion of the Motivic ring with
respect to this filtration.
Let us consider a faithful k-representation V of a finite group G. Hence,
G GL(V). The beginning of the story of the Ekedahl invariants is the fol-lowing
natural question.
Question 1. For which finite groups G does the equality
fGL(V)=Gg = fGL(V)g (1.1)
hold in the Kontsevich value ring cK0(Vark) of algebraic k-varieties?
15
17. Ekedahl found out that all the known examples where the above equality does
not hold are counterexamples to the Noether Problem.
A non-stacky definition of the Ekedahl invariants
In mathematics, to study manifolds, varieties and more generally topological
spaces one constructs abstract structures like the cohomology groups, the ho-motopy
groups pj() for j 2 etc. These could be seen as functors from the
category of our objects C to the category of Abelian groups Ab.
The invariants we are going to define need a more refined target: let L0(Ab)
be the group generated by the isomorphism classes fGg of finitely generated
abelian groups G under the relation fABg = fAg+fBg. It is worth remark-ing
that in L0(Ab) there are differences of groups that do not correspond to any
group: while fZg+fZ=5g is equivalent to the class of fZZ=5g, the element
fZgfZ=5g is not the class of any group.
Let V be a faithful k-representation of the finite group G and let m be a
positive integer. Then G acts naturally componentswise on Vm and the quotient
scheme Vm=G is usually singular.
It is important to remark (see [2]) that K0(Vark) is generated by the class
of smooth and proper varieties subjects to the relations
fXg+fEg = fBlY (X)g+fYg;
where BlY (X) is the blow up of X along Y with exceptional divisor E:
BlY (X) X
^
[
E
^
[
Y:
Hence, if X is the compactification of a resolution of the singularities of
Vm=G, one could write fVm=Gg 2 K0(Vark) as the finite sum of classes of smooth
and proper varieties fXg and fXjg, fVm=Gg = fXg+åj njfXjg 2 K0(Vark).
Definition 1. Let X be a smooth and proper resolution of Vm=G:
X p
!Vm=G:
For m large enough and i 2 Z, the i-th Ekedahl invariant ei (G) is defined as:
ei (G) = fH2mi (X;Z)g+åj
njfH2mi (Xj;Z)g 2 L0(Ab);
where fVm=Gg 2 K0(Vark) is written as the sum finite of classes of smooth and
proper varieties fXg and fXjg and fVm=Gg = fXg+åj njfXjg 2 K0(Vark).
16
18. Open questions about the Ekedahl invariants
The next theorem links these new invariants to the Noether problem.
Theorem 1 (Theorem 5.1 in [10]). Let G be a finite group. The following
holds:
a) ei (G) = 0, for i 0;
b) e0 (G) = fZg;
c) e1 (G) = 0;
d) e2 (G) = fB0(G)_g, where B0(G)_ is the dual of the Bogomolov multiplier
of the group G.
We say that a group G has trivial Ekedahl invariants if ei (G)=0, for i6=0.
It is important to stress that the triviality of the Ekedahl invariants is related to
Question 1:
Lemma 1. If the equality (1.1) holds in cK0(Vark), then G has trivial Ekedahl
invariants.
There are certain results about the triviality of these invariants:
Proposition 1. In the following cases the equality (1.1) holds:
1) if G is the symmetric group and for every field k;
2) if G GL1 and for every field k (in particular, if G is a cyclic group);
3) if G is a unipotent finite group and for every field k;
4) if G is a finite subgroup of the group of affine transformations of A1
k and for
every algebraically closed field k.
In particular, their Ekedahl invariants are trivial.
Vice versa, to study if the Ekedahl invariants are not trivial, one uses that
e2 (G) = fB0(G)_g. Indeed B0(G)6= 0 implies that F(xg : g 2 G)G=F is not
rational, and therefore the given counterexamples to the Noether problem (with
B0(G)6= 0) are also the first examples of finite groups with non trivial Ekedahl
invariants.
Corollary 1 (Non triviality). The second Ekedahl invariant is non trivial for
every algebraically closed field k with char(k) = 0 and for the groups of order
p9 in Saltman’s paper [16] and of order p6 in Bogomolov’s paper [3].
Another connection between the Noether problem and Question 1 is also
given by the next proposition.
Proposition 2 (Corollary 5.8 in [10]). fGL(V)=Z=47Zg6= fGL(V)g in cK0(VarQ).
In the literature, there are no other examples of groups with non trivial
Ekedahl invariants. Following this point of view, it seems natural to ask:
17
19. Question 2. Is there any group G such that e3 (G)6= 0?
More generally:
Question 3. Is there any group G such that ei (G)6= 0 for some i 2?
1.1.2 Results
The class of the classifying stack
Our discussion about the Ekedahl invariants started with Question 1, that asks
about the equality fGL(V)=Gg = fGL(V)g in the Kontsevich value ring of alge-braic
k-varieties cK0(Vark). Since fGL(V)g is invertible in cK0(Vark), one can
consider, instead, the equality
fGL(V)=Gg=fGL(V)g = 1 2cK0(Vark):
The left hand side of the latter is actually the class of the classifying stack
BG of the group G. The reader who is not an expert in the theory of algebraic
stacks can take this as a formal notation and just continue reading from the next
Lemma-Notation: no other concepts are needed. Anyway, for completeness I
recall that a G-torsor P over a scheme X over k, P ! X, is a scheme with a
regular G-action.
Definition 2. The classifying stack BG of a group G is a pseudo-functor from
the category of schemes over k, Schk, to the category of groupoids over k,
Gpdk, sending an open scheme U to the groupoid of G-torsors over U:
BG : Schk ! Gpdk
U7! fG-torsors over Ug:
Equivalently, the classifying stack of the group G is usually defined as the stack
quotient BG = [=G].
Lemma-Notation. (see Proposition 2.6 in Paper A) The class of the classify-ing
stack of the group G in the Kontsevich value ring is
fBGg = fGL(V)=Gg
fGL(V)g 2cK0(Vark):
In paper B, I deal with the finite subgroups of GLn (C) and prove that:
Theorem 2 (Theorem 2.5 in Paper B). If G is a finite subgroup of GL3 (C),
then fBGg = 1.
18
20. This is a partial answer to Question 1. I tried also to approach the finite
subgroups of GL4, but this need the study of the resolutions of singularities of
C3=G. This could be done for few cases, but not with the same general approach
that I used for GL3 (C).
As an application of this theorem one gets:
Corollary 2. If G is a finite subgroup of GL3 (C), then the Ekedahl invariants
of G are trivial.
This result extends item 2) in Proposition 1.
A stacky definition of the Ekedahl invariants
For any integer k, Ekedahl defined a cohomological map
Hk :cK0(Vark)!L0(Ab);
sending fXg=Lm to fHk+2m (X;Z)g, for any smooth and proper X. This is an
extension of the natural map that associates to every smooth and proper k-variety
X the class fHk (X)g of its integral cohomology group Hk (X). This
extension is well defined and it is a continuous group homomorphism (see
Theorem 3.1 in Paper B).
In [10], Ekedahl defines these new geometric invariants:
Definition 3. The i-th Ekedahl invariant is ei (G) = Hi (fBGg) 2 L0(Ab).
In Paper A, I prove that:
Theorem 3 (Proposition 4.1 in Paper A). Definition 1 and Definition 3 are
equivalent.
The Ekedahl invariants for finite groups
We have already seen that if G is a subgroup of GL3 (C), then the Ekedahl
invariants of G are trivial. Therefore one could study groups with faithful
representations in higher dimension, but one should also be able to construct
the resolution in Definition 1. The discrete Heisenberg group Hp fits in this
description.
This is the subgroup of upper unitriangular matrices of GL3 (Fp):
Hp =
8
0
@
:
1 a b
0 1 c
0 0 1
1
A : a;b;c 2 Fp
9=
;:
19
21. It is also an interesting candidate for the study of ei (Hp), because B0(Hp)
vanishes and so the first unknown Ekedahl invariants is e3 (Hp).
Let V be a faithful linear p-dimensional complex representation of Hp. Let
Ap be Hp modulo its center. Then, I show in Theorem 4.4 of Paper B that
e3 (Hp) = e4 (Hp) = ftor(H2p5 (Xp;Z))g;
where Xp is smooth and projective resolution of P(V)=Ap.
I am able to construct X5 via toric resolutions of singularities: in Section
4.1 in Paper B I show that tor(H5 (X5;Z)) is zero.
Theorem 4 (Theorem 4.4 in Paper B). The Ekedahl invariants of the fifth dis-crete
Heisenberg group are trivial.
I actually give a general approach for the study of the Ekedahl invariants of
Hp, but we narrow down our investigation to p = 5 because of the difficulties
to extend (for every p) the technical result in Theorem 4.7 in Paper B.
The reduction of a finite group G in PGLn is denoted by H:
0 K G H 0
0 C _ GLn _ PGLn _ 0:
If H is commutative, I give a recurrence relation that the Ekedahl invariants
satisfy in L0(Ab):
Theorem 5 (Theorem 3.1 in Paper B). Let G be a finite subgroup of GLn (C)
and let H be the image of G under the canonical projection into PGLn(C).
If H is abelian and if Pn1
C =H has only zero dimensional singularities, then for
every integer k
ek (G)+ek+2 (G)++ek+2(n1) (G) = fHk (X;Z)g;
where X is a smooth and proper resolution of Pn1
C =H.
20
22. 1.2 The Veronese Modules
In the first part of this section, I recall some definitions about resolutions of
modules over a ring and I introduce some combinatorial objects, the squarefree
divisor complex and the pile simplicial complex, playing an important role in
the theory of semigroup rings. I also give some known facts about the Betti
numbers of the Veronese embeddings.
In [13] (work not included in this thesis), we gave an algebraic proof of
some polynomial identities among Betti numbers of (numerical) semigroup
rings. In Paper C, we deal with the Veronese embeddings and the Veronese
modules. First, we extend the results of Bruns and Herzog (see Theorem 6)
and Paul (see Theorem 7) to these modules. Then, we prove a closed formula
for their Hilbert series. We also show several applications of these results.
1.2.1 Preliminaries
Rings and their resolutions
In this section, I recall some well known concepts in commutative algebra to
set the notations and avoid ambiguities.
Let k be an algebraically closed field with characteristic zero. From now
on we denote by S the polynomial ring in n variables with degxi = 1.
Let R be a finitely generated k-algebra and M be a finitely generated R-module.
The depth of M, depthM, is the length of the longest possible M-sequence
in R. We denote by dimM the Krull dimension of R=AnnM, where
AnnM = fr 2 R : rm = 0;8m 2 Mg
is the annihilator of M. One sees that depthM dimM.
Definition 4. An R-module M is Cohen-Macaulay if and only if depthM =
dimM.
Let M = iMi be a finitely generated N-graded S-module. We recall that
the Hilbert series of the module M is
H(M; z) =
¥å
i=0
dimMi zi:
Since M is a module over the polynomial ring S = k[x1; : : : ;xn], then H(M; z)
has a rational form
H(M; z) =
h(z)
(1z)n ;
where the numerator of this fraction (called h-polynomial) plays an important
role in this subject.
21
23. A minimal free resolution of the S-module M is an exact sequence of free
modules
0!Fm
fm !Fm1
fm1 !
f1 !F0
f0 !M !0:
such that the homomorphisms fi are homogeneous and minimal (that is fi(Fi)
(x1; : : : ;xn)Fi1). In this case the resolution looks like
0!jS(j)bm; j(M) !jS(j)bm1; j(M) !!jS(j)b0; j(M) !M !0:
Here, S(j) is a module obtained by shifting the degrees of S by j, that is
S(j)l = Slj.
The polynomial ring S is naturally Nn-graded. Let S = jSj. (Without
any confusion with the field k, we always use bold font for vectors.) If m =
xa1
xa2
1 n is a monomial in S, then we set the notation m = xa, where a =
2 xan
(a1; : : : ;an) 2Nn. Similarly one could find a minimal free resolution and define
the numbers bi;j(M).
Definition 5. Let M = iMi be a finitely generated N-graded S-module. The
i-th Betti number of M is bi(M) = åj bi; j(M). The i-graded Betti number with
degree j of M is bi; j(M).
Similarly, if M = jMj is Nn-graded, then the i-graded Betti number with
degree j of M is bi;j(M).
It is an important fact that the Betti numbers do not depend on the resolution.
By the Hilbert’s syzygy theorem (see [9]), there are only a finite number
of non-zero Betti numbers and it is easy to see that bi; j = 0 if i j. For this
reason it is common in the literature to write down the Betti numbers in a table
like the following:
0 1 : : : p
0 b0;0 b1;1 : : : bp;p
1 b0;1 b1;2 : : : bp;p+1
2 b0;2 b1;3 : : : bp;p+2
...
... ...
. . .
...
i b0;i b1;1+i : : : bp;p+i
...
...
...
. . .
...
n b0;n b1;1+n : : : bp;p+n
The number p is called the projective dimension of M, pdimM, and we
have the Auslander-Buchsbaum formula (see [4; 12]):
pdimM+depthM = depthR:
Using the table above we state the last definition.
Definition 6. The S-module M has a linear resolution if there is only one row
of non-zero Betti numbers.
22
24. Semigroup rings
A monoid is a set equipped with an operation having an identity element and
being associative. A monoid is affine if it is a finitely generated submonoid
of Zd with respect to the addition operation. An affine monoid is positive
if it is isomorphic to an affine monoid inside Nd. For this reason, when we
consider an affine positive monoid H = hh1; : : : ;hNi, we can always assume
that H Nd. Moreover, if H N then it is called a numerical monoid (or
numerical semigroup).
As we said, the polynomial ring S is naturally Nn-graded, but one could use
a different multi-grading by a positive affine monoid H. Indeed, a semigroup
ring k[H] is the subalgebra of S defined as k[xh : h 2 H]. The ring k[H] is
generated by the monomials fxhig. In other words, a presentation of k[H] is
given by
f : k[y1; : : : ;yN] ! k[x1; : : : ;xn]
yi7! xhi :
and k[H] = k[y1;:::;yN]=kerf. Thus, k[H] is also a module over k[y1; : : : ;yN].
The squarefree divisor complex and the pile simplicial complex
Set [N] = f1; : : : ;Ng. An abstract simplicial complex D on [N] is a subfamily
of 2[N] such that if A 2 D and B A then B 2 D. An element of D is called face.
If A is a face, we set dimA = #A1 (and dim /0 = 1). Moreover dimD is the
maximal dimension of its faces.
The k-skeleton of D is denoted by Dhki and it is the subcomplex of D consisting
of the faces of dimension less then or equal to k.
Let H = hh1; : : : ;hNi be an affine positive monoid. Bruns and Herzog in
[5] defined the following simplicial complex.
Definition 7. Given h 2 H, the squarefree divisor complex of k[H] is
Dh(k[H]) =
fi1; : : : ; ikg [N]j xhi1++hik divides xh in H
:
They showed that one could read the graded Betti numbers of k[H] as the
reduced homology of Dh(k[H]):
Theorem 6 (Proposition 1.1 in [5]). bi;h(k[H]) = dimk ˜H
i1(Dh(k[H]);k).
Let us define the partial ordering in Zn as a b if and only if ba 2 Nn.
In the same direction Paul (see [15]) defined a combinatorial version of Dh:
23
25. Definition 8. Let A be a finite subset of Nn and let #A = N. For every c 2 Zn,
the pile simplicial complex of A is
Gc(A) = fF Aj å
a2F
a cg:
Paul proved that Gc(A)=Dc(k[H]) if and only if the semigroup generated by A
in Nn equals the group generated by A in Zn intersected by Nn (see Proposition
3 in [15]).
In Theorem 1 of [15], he also proved a duality formula for Gc(A), namely:
˜H
i1(Gc(A);k) = ˜H
Nni1(Gˆc(A);k)_; (1.2)
where c ˆ= åa2A ac1.
The Veronese modules
From now on, given a vector z = (z1; : : : ; zn) 2 Zn, we denote by jzj the total
degree of z, that is jzj = z1+z2++zn.
Definition 9. Let Ad = fa 2 Nn : jaj = dg. The Veronese subring S(d) of S is
the algebra S(d) = k[xa : a 2 Ad].
The embedding dimension, emb(S(d)), of S(d) is N =
d+n1
d
= #A.
Definition 10. Let S = k[x1; : : : ;xn]. The Veronese module Sn;d;k is defined as
Sn;d;k = i0Sdi+k with n;d;k 2 N.
Let us notice that Sn;d;0 = S(d). Furthermore, we have that Sn;d;k are S(d)-
modules. Finally Paul connected the homology of the pile simplicial complex
with the Betti numbers of the Veronese ring.
Theorem 7 (Theorem 7 in [15]). Let i 2 Z and c 2 Zn. If jcj is a multiple of d,
then
bi;c(S(d)) = dimk ˜H
Nni1(Gˆc(A);k):
Otherwise bi;c(S(d)) = 0.
1.2.2 Results
In Paper C, we study the Veronese modules of the polynomial ring in n vari-ables
over an algebraically close field of characteristic zero. The main result
generalizes the formulas of Paul and Bruns-Herzog to the Veronese modules.
24
26. Theorem (Theorem 3.1 in Paper C). If c is a vector in Zn such that jcj=k+ jd,
then
i1(Gh j1 c i;k);
bi;c(Sn;d;k) = dimk ˜H
where Ghcj1i is the ( j1)-skeleton of Gc. Moreover, bi;c =0 when jcj6=k+ jd.
As an application, we characterize combinatorially when these modules are
Cohen-Macaulay:
Theorem (Theorem 3.5 in Paper C). The Veronese module Sn;d;k is Cohen-
Macaulay if and only if k d. Moreover if Sn;d;k is not Cohen-Macaulay, then
it has maximal projective dimension, that is pdim(Snd+n1
;d;k) =
d
1.
Another application is Theorem 3.8, where we show that if k d(n1) n, then the resolution of the Veronese module Sn;d;k is pure (and actually bi =
bi;k+id for all i).
Another key result is that we find a general way to compute the rational
form of the Hilbert series of the Veronese modules:
Theorem (Theorem 2.1 in Paper C). d
dzH(Sn;d;k; z) = nH(Sn+1;d;k1; z).
Hence,
H(Sn;d;k; z) =
1
(n1)!
dn1
dzn1
zk+n1
1zd
:
By differentiating the latter with a computer algebra program, one could get
the Hilbert series for any Sn;d;k. In particular, this lets us write a closed formula
for H(S3;d;k; z).
25
27. 1.3 The Linear Recurrence Varieties
In this section I begin by stating the definition of a linear recurrences varie-ty
recently given by Ralf Fröberg and Boris Shapiro. This relates to certain
algebraic varieties generated by Schur polynomials. I introduce some open
questions and conjectures which I treat later. In addition, I discuss the con-nection
between the study of linear recurrence varieties and a conjecture by
Conca, Krattenthaler and Watanabe.
I studied Conjecture 1 and the related Question 5 (see the section below),
in the beginning of my doctoral studies. Indeed, in a published work not in-cluded
in this thesis [14], we treat some regular sequences of complete sym-metric
polynomials extending some of the results in [6]. In article D we study
the linear recurrence varieties by using the linear recurrence associated to a
numerical semigroup (giving a partial answer to Question 4).
1.3.1 Preliminaries
A linear recurrence equation of order k with constant complex coefficients is
an equation of the form
U : un+a1un1+a2un2++akunk = 0;
with n k 1 and ak6= 0. We denote by Lk the space of such linear recur-rences.
Obviously, Lk = Ck1C.
If the roots frig of its characteristic polynomial,
p(U; z) : zk +a1zk1+a2zk2++ak;
are distinct then a general solution of the recurrence equation is given by
un = c1rn
1 +c2rn
2 ++ckrn
k ;
where the ci are complex coefficients fixed by the initial constraints.
Fröberg and Shapiro in [11] introduced the following object:
Definition 11. Given I = fi1 i2 img N with m k, the linear
recurrence variety Vk;I is the subset of Lk consisting of all linear recurrences
having at least one non trivial solution vanishing at all points of I.
Proposition 4 in [11] shows that Vk;I is a quasi-affine variety (which ex-plains
its name). They also posed the following question:
Question 4. For which pairs (k; I) is the variety Vk;I not-empty and what is its
dimension?
26
28. This variety is related to various topics in mathematics. Indeed, let us
consider the following map from the k-dimensional complex affine space to
the mk complex matrices, Mm;k:
Mk;I : Ck ! Mm;k
(x1; : : : ;xk)7!
0
BBB@
xi1
1 xi1
2 : : : xi1
k
xi2
1 xi2
2 : : : xi2
k
...
...
. . .
...
xim
1 xim
2 : : : xim
k
1
CCCA
:
The matrix Mk;I(x1; : : : ;xk) is called a generalized Vandermonde matrix, well-known
for instance in Numerical Analysis.
Observation 1. If U 2 Vk;I , then there exists a non-trivial solution fung such
that ui = 0 for every i 2 I. Hence, rankMk;I(r1; : : : ;rk) k.
Consider Om;k Mm;k, the subset of matrices of non-maximal rank. The
braid hyperplane arrangement A Ck is defined by all the hyperplanes given
by xi = xj for all i6= j. Of course, if xi = xj (for some i and j) then the rank of
Mk;I(x1; : : : ;xk) is strictly less than k.
Definition 12. We denote by VdA
k;I the localization of M1
k;I (Om;k) into Ck nAk.
In Lemma 5 of [11], the authors showed that the variety VdA
k;I is the zero
set of
mk
Schur polynomials SJ(x1; : : : ;xk), where J = f j1 j2 jkg is
a k-subset of I and
SJ(x1; : : : ;xk) =
29.
30.
31.
32.
33.
34.
35.
36.
37.
38.
39.
40.
41. 2 : : : x j1
x j1
1 x j1
k
x j2
1 x j2
2 : : : x j2
k
...
...
. . .
...
x jk
1 x jk
2 : : : x jk
k
78. :
Since the codimension of Om;k inMm;k is mk+1 (see [8]) andVdA
k;I is the
localization of M1
k;I equals mk+1.
k;I (Om;k), the expected codimension of VdA
Definition 13. A pair (k; I) is A-regular if k m 2k1 and codim(VdA
k;I)=
mk+1.
Question 5. Set i1 = 0 and gcd(i2; : : : ; im) = 1. Which pairs (k; I) are A regular?
Theorem 11 in [11] shows that if m k and codim(VdA
k;I) = mk+1 then
i2 = 1.
27
79. If we fix (k;m) = (3;5), this leads to a conjecture posed by Conca, Krat-tenthaler
and Watanabe in [6]. Hence, I = f0;1; i3; i4; i5g. If VdA
3;I has the
expected codimension, then it is a complete intersection. After some compu-tations,
one can see that VdA
3;I is actually generated by hi32, hi42 and hi52,
where hn(x;y; z) is the complete homogeneous symmetric polynomial of de-gree
n in three variables. The authors in [6] proved the only if direction of the
following conjecture.
Conjecture 1. The ideal (ha(x;y; z);hb(x;y; z);hc(x;y; z)) is a complete inter-section
if and only if the following conditions are satisfied:
• abc 0 mod 6;
• gcd(a+1;b+1;c+1) = 1;
• For all positive integers grater than 2 there exists d 2 fa;b;cg such that
d+26 0;1 mod t.
1.3.2 Results
In Paper D, we present a partial answer to Question 4 by using the theory of
semigroups.
Given a numerical semigroup S = ha1; a2; : : : ; aNi under the assumption
gcd(a1;a2; : : : ;aN) = 1, it is well known that the number of its gaps
D(a1;a2; : : : ;aN) = NnS
is finite.
We define (in Paper D) the linear recurrence associate to the semigroup S
as the linear recurrence given by:
US : gk = w1gka1 +:::+wNgkaN ; 8 k 0; (1.3)
for every choice of strictly positive real numbers fwigN i=1 and with the initial
standard conditions g0 = 1, gj = 0, for aN j 0.
One proves that there exists a non-zero sequence fgkgk2N satisfying the linear
recurrence equation US (see Lemma 2.1 in Paper D). In Lemma 2.2 in Paper D
we also show that gk = 0 if and only if k is a gap of S.
Theorem 8 (Theorem 2.1 in Paper D). If S = ha1; a2; : : : ; aNi and
I D(a1;a2; : : : ;aN), then V(b;I)6= /0, for all b 2 S, with b aN.
This result has recently been extended by Contreras-Rojas in [7].
Theorem 9. If S and I are given as above, then V(s;I)6= /0, for all s 2 S.
Finally we could say something about the dimension of the linear recur-rence
variety.
28
80. Theorem 10 (Corollary 2.2 in Paper D). If S = ha1; a2; : : : ; aNi and
I D(a1;a2; : : : ;aN) then dim(V(aN;I)) N, that is the Krull dimension of
V(aN;I) is at least N.
Let us mention that the definition of the linear recurrence associated with
Ni
the semigroup S actually has a probabilistic interpretation: if the coefficients
wi 0 satisfy å1wi = 1, then fwig defines a probability distribution. Let
=Xt be a discrete random variable taking values in N, and t 2 N. We define a
random walk associated to the semigroup S = ha1;a2; : : : ;aNi as
Xt = Xt1+
8
:
a1 with probability w1;
a2 with probability w2;
...
...
aN with probability wN;
starting with X0 = 0.
The probability of visiting the state k is
gk = ProbfXt = k for some t 2 Ng; k 2 N
and their generating function, G(z) = åk gkzk, is obtained by
G(z) =
1
1w1za1 :::wNzaN
:
29
82. References
[1] M. ARTIN AND D. MUMFORD, Some elementary examples of unira-tional
varieties which are not rational, Proc. London Math. Soc. (3), 25
(1972), pp. 75–95. 15
[2] F. BITTNER, The universal Euler characteristic for varieties of charac-teristic
zero, Compos. Math., 140 (2004), pp. 1011–1032. 16
[3] F. A. BOGOMOLOV, The Brauer group of quotient spaces of linear rep-resentations,
Izv. Akad. Nauk SSSR Ser. Mat., 51 (1987), pp. 485–516,
688. 15, 17
[4] W. BRUNS AND J. HERZOG, Cohen-Macaulay rings, vol. 39 of Cam-bridge
Studies in Advanced Mathematics, Cambridge University Press,
Cambridge, 1993. 22
[5] , Semigroup rings and simplicial complexes, J. Pure Appl. Algebra,
122 (1997), pp. 185–208. 23
[6] A. CONCA, C. KRATTENTHALER, AND J. WATANABE, Regular se-quences
of symmetric polynomials, Rend. Semin. Mat. Univ. Padova, 121
(2009), pp. 179–199. 26, 28
[7] Y. CONTRERAS-ROJAS, On the variety of recurrences associated to
a numerical semigroup. Personal communication concerning work in
progress, April 2014. 28
[8] J. A. EAGON AND D. G. NORTHCOTT, Ideals defined by matrices and
a certain complex associated with them., Proc. Roy. Soc. Ser. A, 269
(1962), pp. 188–204. 27
[9] D. EISENBUD, Commutative algebra, vol. 150 of Graduate Texts in
Mathematics, Springer-Verlag, New York, 1995. With a view toward
algebraic geometry. 22
[10] T. EKEDAHL, A geometric invariant of a finite group.
arXiv:0903.3148v1, 2009. 17, 19
31
83. [11] R. FRÖBERG AND B. SHAPIRO, Vandermonde varieties and relations
among schur polynomials. Personal Website of Boris Shapiro. 26, 27
[12] S. B. IYENGAR, G. J. LEUSCHKE, A. LEYKIN, C. MILLER,
E. MILLER, A. K. SINGH, AND U. WALTHER, Twenty-four hours of
local cohomology, vol. 87 of Graduate Studies in Mathematics, Ameri-can
Mathematical Society, Providence, RI, 2007. 22
[13] N. KUMAR AND I. MARTINO, An algebraic proof for the identities for
degree of syzygies in numerical semigroup, Matematiche (Catania), 67
(2012), pp. 81–89. 21
[14] , Regular sequences of power sums and complete symmetric poly-nomials,
Matematiche (Catania), 67 (2012), pp. 103–117. 26
[15] S. PAUL, A duality theorem for syzygies of Veronese ideals of weighted
projective space. arXiv: 1311.5653v1. 23, 24
[16] D. J. SALTMAN, Noether’s problem over an algebraically closed field,
Invent. Math., 77 (1984), pp. 71–84. 14, 17
[17] R. G. SWAN, Invariant rational functions and a problem of Steenrod,
Invent. Math., 7 (1969), pp. 148–158. 14
32
86. Introduction to the Ekedahl Invariants
Ivan Martino
Abstract
In 2009 T. Ekedahl introduced certain cohomological invariants
for
87. nite groups. In this work we present these invariants and we
give an equivalent de
88. nition that does not involve the notion of alge-
braic stacks. Moreover we show certain properties for the class of the
classifying stack of a
89. nite group in the Kontsevich value ring.
In [5], Ekedahl studied whether the class of the classifying stack fB Gg
of a group G equals the class of a point fg in the Grothendieck group of
algebraic stacks. All the known examples of
90. nite groups when this does
not happen are the counterexamples to the Noether problem: one wonders
about the rationality of the
91. eld extension F F(xg : g 2 G)G (see [9]). To
show that fB Gg6= fg, Ekedahl introduced in [4] a new kind of geometric
invariants for
93. ned as the cohomology for the classifying stack
of G.
We denote by K0(Vark) the Grothendieck group of varieties. Let Li
be the class of the ane space Ai
k in K0(Vark) (so L0 = fg, the class
of a point). Let cK0(Vark) be the Kontsevich value ring of algebraic k-
varieties (see Section 1). We denote by L0(Ab) the group generated by the
isomorphism classes fGg of
94. nitely generated abelian groups G under the
relation fA Bg = fAg + fBg.
For every integer k, in [5] Ekedahl de
95. nes a cohomological map
Hk : cK0(Vark) ! L0(Ab)
by assigning Hk(fXg=Lm) = fHk+2m (X;Z)g for every smooth and proper k-
variety X (see Section 3). The class fB Gg of the classifying stack of G can
be seen as an element of cK0(Vark) (see Proposition 2.6) and so one de
98. nition 3.2. For every integer i, the i-th Ekedahl invariant ei (G) of the
group G is Hi(fBGg) in L0(Ab). We say that the Ekedahl invariants of G
are trivial if ei (G) = 0 for i6= 0.
The purpose of this paper is to introduce the theory of the Ekedahl in-variants
to a reader who is not used to the notion of the algebraic stacks. For
this reason we also present some unpublished results form [5, 4] aiming to
a complete and self contained survey of the topic. The author believes that
one could work with Ekedahl invariants with basic knowledge of algebraic
geometry and for this reason we present the following non-stacky de
100. nition 4.1. Let V be a n-dimensional faithful k-representation of a
101. nite
group G and let X be a smooth and proper resolution of V m=G:
X ! V m=G:
For m large enough, the i-th Ekedahl invariant is de
102. ned as follows:
ei (G) = fH2mi (X;Z)g +
X
j
njfH2mi (Xj ;Z)g 2 L0(Ab);
where fV m=Gg 2 K0(Vark) is written as the sum P
of classes of smooth and
proper varieties fXg and fXjg, fV m=Gg = fXg +
j njfXjg.
In Proposition 4.2 we prove that the two de
103. nitions are equivalent and we
use the latter to prove the following theorem due to Ekedahl (see Theorem
5.1 in [4]):
Theorem 4.3. We denote by B0(G)_ the dual of the Bogomolov multiplier
of the group G. If G is a
104. nite group, then
a) ei (G) = 0, for i 0;
b) e0 (G) = fZg;
c) e1 (G) = 0;
d) e2 (G) = fB0(G)_g + fZg for some integer .
Item d) is related to the Noether problem (see Section 1). Ekedahl ac-tually
proved a stronger version of this result since he showed that e2 (G) =
fB0(G)_g.
2
105. In Section 1, after a brief historical introduction, we set all the basic no-tions
and notations. In Section 2 we discuss some properties of the class of
the classifying stack fB Gg and in Section 3 we de
106. ne the Ekedahl invariants
as the cohomology of the classifying stack. In Section 4 we present the equiv-alent
non-stacky de
108. nition to
reprove partially Theorem 5.1 of [4]. In the end of the article we recall the
state of the art of the Ekedahl invariants.
Notation. In all this manuscript we work over an algebraically close
109. eld k
of characteristic zero.
1 Preliminaries
Let F be a
115. eld extension (1) is rational (i.e. purely transcendental).
Mathematicians conjectured a positive answer to the Noether problem, until
the breakthrough result of of Swan (see [12]) in 1969. He proved that the
extension Q Q(xg : g 2 Z=pZ)Z=pZ is not rational for p = 47; 113 and 233.
After this, Saltman in [10] proved that for every
116. eld F and for any prime p
with (char F; p) = 1, there exists a group G of order p9 such that the Noether
problem has negative answer. He used a cohomological invariant introduced
by Artin and Mumford in [1]. Bogomolov in [3], showed a concrete way to
compute this invariant that is now called Bogomolov multiplier B0(G):
B0(G) =
A
Ker
H2 (G;C)) ! H2 (A;C)
;
where the intersection runs over the abelian subgroups A G. This is a
cohomological obstruction to the rationality of (1), i.e. the rationality of (1)
implies B0(G) = 0. Bogomolov also improved Saltman's statement from p9
to p6.
3
117. In the rest of this section we introduce some de
118. nitions which we need
later. The Grothendieck group K0(Vark) of varieties over k is the group gen-erated
by the isomorphism classes fXg of algebraic k-varieties X, subjected
to the relation
fXg = fZg + fX n Zg;
for all closed subvarieties Z of X. It is possible to see that K0(Vark) has a
ring structure given by fXg fY g = fX Y g.
The class of the empty set f;g is also denoted with 0, the class of the point
fg with 1 and the class of the ane line L = fA1
kg is called Lefschetz
class. Using the multiplication operation, one gets fAn
kg = Ln and fPn
kg =
L0 + L1 + + Ln.
In [2], Bittner proves that K0(Vark) is generated by the class of smooth
and proper varieties modulo the relations fXg + fEg = fBlY (X)g + fY g
with BlY (X) being the blow up of X along Y with exceptional divisor E:
BlY (X) X
^
[
E
^
[
Y:
Therefore, with the help of compacti
119. cation and resolution of singularities
one writes the class of a scheme fXg 2 K0P
(Vark) as a sum of classes of
smooth and proper varieties fXjg: fXg =
j njfXjg, with nj 2 Z.
The Motivic ring of algebraic k-varieties is K0(Vark)[L1]. We naturally
de
123. nition 1.1. A G-torsor P over a scheme X over k, P ! X, is a scheme
with a regular G-action.
De
124. nition 1.2. The classifying stack B G of a group G is a pseudo-functor
from the category of schemes over k, Schk, to the category of groupoids over
k, Gpdk, sending any open scheme U to the groupoid of G-torsors over U:
B G : Schk ! Gpdk
U7! fG-torsors over Ug:
4
126. ned as the
stack quotient B G = [=G].
2 The class of the classifying stack
Recall that we denote by K0(Vark), K0(Vark)[L1] and cK0(Vark) the Grothendieck
ring, the Motivic ring and, respectively, the Kontsevich value ring of algebraic
k-varieties, where k is an algebraic closed
128. nition 2.1. We denote by K0(Stackk) the Grothendieck group of alge-
braic k-stacks. This is the group generated by the isomorphism classes fXg
of algebraic k-stacks X of
129. nite type all of whose automorphism group scheme
are ane (shortly, algebraic k-stack of
130. nite type with ane stabilizer). The
elements of this group ful
131. ll the following relations:
1. for each closed substack Y of X, fXg = fY g + fZg, where Z is the
complement of Y in X;
2. for each vector bundle E of constant rank n over X, fEg = fX Ang.
Similarly to K0(Vark), K0(Stackk) has a ring structure.
Lemma 2.2. One has that
K0(Stackk) = K0(Vark)[L1; (Ln 1)1; 8n 2 N]:
Moreover, the completion map K0(Vark)[L1] ! cK0(Vark) factors through
K0(Vark)[L1] ! K0(Stackk) ! cK0(Vark):
Proof. The
132. rst part is proved in Theorem 1.2 of [4]. Regarding the second
one, we observe that Ln1 = Ln(1Ln) is invertible in cK0(VarkP). Indeed,
(1 Ln)1 = 1 + Ln + L2n + : : : and each truncation xk =
k
j=0 Lkn
belongs to Filkn. So, the serie converges in cK0(Vark).
De
133. nition 2.3. A special group G is a connected algebraic group scheme of
136. Let G be a special group and let X ! Y be a G-torsor of algebraic stacks
of
137. nite type over k, then fXg = fGgfY g in K0(Stackk). Moreover, if F
is a G-space and Z ! Y is a F-
138. bration associated to the G-torsor X ! Y
and to the action on F, then fZg = fFgfY g in K0(Stackk).
Those two facts are not true for a general group G. Indeed special groups
play an important role in this topic (see Proposition 1.4 of [5]).
Lemma 2.4. If G is a special group and if H is a closed subgroup scheme
of G, then
a) fGgfB Gg = 1;
b) fBHg = fG=HgfB Gg.
Proof. Consider the G-torsor ! [=G]. Thus, fg = fGgf[=G]g. Moreover
! [=G] is also an H-torsor and the action of H makes G=H a H-space. There
is a natural G=H-
139. bration associated, [=H] ! [=G], given by BH = G=HGB G
and thus fBHg = fG=HgfB Gg.
We narrow down our investigation to
140. nite groups.
Lemma 2.5. If V be an n-dimensional linear representation of G, then
f[V m=G]g =
LnmfB Gg;
(2)
f[P(V )=G]g =
1 + L1 + + Ln1fB Gg: (3)
Proof. From the vector bundle [V=G] ! B G and from the second property
in De
141. nition 2.1, one has that f[V=G]g = LnfB Gg. Similarly, one proves the
142. rst equation.
Let O be the origin of V . The natural map [V nfOg=G] ! [P(V )=G] is a
Gm-torsor and this implies f[V nfOg=G]g = (L 1)f[P(V )=G]g. Moreover,
f[V nfOg=G]g = (Ln 1)fB Gg = (L 1)f[P(V )=G]g.
Formula (2) expresses how fB Gg is connected with f[V m=G]g. The next
proposition links fB Gg to fV m=Gg. Behind this result there is the study of
the dierence between f[V m=G]g and fV m=Gg in K0(V ark)[L1].
We write an element of V m as
v = (v1; : : : ; vn; vn+1; : : : ; v2n; : : : ; v(k1)n+1; : : : ; vkn; vkn+1; : : : ; vm)
6
143. with k = bm=nc. In other words, we consider v 2 V m as a sequence of sets
made by n vectors each. Let U be the subset of V m such that at least one
of the sets fvjn+1; : : : ; vjn+ng is a basis for V .
We denote by M the complement of U in V m. This is a closed subset of
V , because it is de
144. ned by k equations det(vjn+1; : : : ; vjn+n) = 0, for j =
0; : : : ; k 1. Therefore, codim(M) = codim(M=G) = k. We also observe that
U is GLn (k)-invariant, because any linear transformation in GLn (k) moves
a basis of V into another one. Moreover, GLn (k) (and so G) acts freely on
it, hence [U=G] = U=G.
The dierence f[V m=G]g fV m=Gg becomes
f[V m=G]g fV m=Gg = (fZg + fU=Gg) (fM=Gg + fU=Gg)
= fZg fM=Gg; (4)
where Z is a stack, complement of U=G in [V m=G]. Similarly to M=G, Z has
codimension k because both are the complement of the same object U=G, but
in two dierent environments V m=G and [V m=G] with the same dimension. The
class of the dierence f[V m=G]gfV m=Gg is so determined by the class of these
complements. We see, in the next proposition, how this implies that
fB Gg = lim
m!1
fV m=Gg
Lmn
2 cK0(Vark):
Proposition 2.6 (Proposition 3.1 in [5]). If V is an n-dimensional faithful
linear representation of G, then
a) fB Gg = fGL(V )=Gg=fGL(V )g;
b) The image of fB Gg in cK0(Vark) is equal to limm!1fV m=GgLmn.
Proof. The general linear group is a special group and we apply Lemma 2.4.b
for G GL(V ): fB Gg = fGL(V )=GgfB GL(V )g. Using Lemma 2.4.a, one
gets fB GL(V )g = 1=fGL(V )g and so, we prove the
145. rst point.
Using formula (2) and formula (4) one has
fB Gg fV m=GgLmn = (f[V m=G]g fV m=Gg) Lmn
= (fZg fM=Gg) Lmn
where Z and M=G are respectively the complement of U=G
146. rstly seen inside
of [V m=G] and then inside of V m=G. The open set U was de
148. Remark that Filj(K0(Vark)[L1]) = ffXg=Li : dimX i jg. Then,
fM=GgLmn belongs to Filj(K0(Vark)[L1]) if and only if dimM=Gmn j.
One knows that dimM=Gmn = codim(M=G) = k. Thus fM=GgLmn be-longs
to Filj for any j k = bm=nc. Therefore, limm!1fM=GgLmn =
0 and, with a similar argument, limm!1fZgLmn = 0. Thus, fB Gg
fV m=GgLmn converges to zero in cK0(Vark).
3 The Ekedahl invariants for
152. ned target: Let L0(Ab)
be the group generated by the isomorphism classes fGg of
153. nitely generated
abelian groups G under the relation fABg = fAg+fBg. We equip L0(Ab)
with the discrete topology.
For clari
154. cation, fZg and fZ=png belong to L0(Ab) and there are elements
in L0(Ab) that do not correspond to any group: while fZg + fZ=5g is the
class of fZ Z=5g, the element fZg fZ=5g is not the class of any group.
It is natural to de
155. ne a cohomological map
Hk : K0(Vark) ! L0(Ab);
by assigning to every smooth and proper k-variety X the class of its in-tegral
cohomology group Hk (X;Z). Next theorem shows that this map is
well de
156. ned and that it can be extended to cK0(Vark) sending fXg=Lm to
fHk+2m (X;Z)g for any smooth and proper variety X,
Hk : cK0(Vark) ! L0(Ab):
Theorem 3.1. The following cohomological map
H : cK0(Vark) ! L0(Ab)((t))
fY g7!
X
k2Z
Hk (fY g) tk:
is well de
157. ned. For each k 2 Z, Hk : cK0(Vark) ! L0(Ab) is also a contin-
uous group homomorphism.
8
158. Proof. The proof is given by Ekedahl in [5] via Proposition 3.2.i), ii) and
Proposition 3.3.ii). We give an alternative proof.
We
159. rst prove that the map Hk : K0(Vark) ! L0(Ab) is well de
160. ned.
~We know that K0X
~X
(Vark) is generated by the class of smooth and proper
varieties modulo the relations fXg + fEg = f g + fY g with being the
blow up of X along Y (smooth subvariety of codimension d) with exceptional
divisor E (note that E is also smooth because it is a projective bundle over
Y , r = jE : E ! Y ):
~X
X
^
h
[
E
^
j
[
r
Y:
Moreover, by the Leray-Hirsch Theorem (see for instance [7]),
Hk (E) =
Hk (Y ) Hk2 (Y ) Hk2(d1) (Y ) :
We want to show that fHk( ~X
)g + fHk (Y )g = fHk (E)g + fHk (X)g and
therefore it is enough to show that Hk( ~X
) =
Hk (X) Hk2 (Y )
Hk2(d1) (Y ).
Firstly we observe that the pushforward of the fundamental class of ~Xis
the fundamental class of X, [ ~X
] = [X] (see [6]). Now, 1 is the dual of [ ~X
]
~X
and, respectively, of [X], 1 = 1. Using this and the projection formula one
gets that for every y in Hk (X) (1 y) = (1) y, that is y = y and
so = idHk(X). Therefore, : Hk( ) ! Hk (X) is surjective and one
constructs the isomorphism Hk( ~X
) = Hk (X) ker() sending x in Hk( ~X
)
into (x; x x).
Calling U = X n Y we also have the following commutative diagram:
: : : Hk1( ~X
) Hk1 (U) Hk2 (E)
h Hk( ~X
) Hk (U) : : :
_
: : : Hk1 (X)
id
_
Hk1 (U)
r
_
Hk2 (Y )
_
Hk (X)
j
id
_
Hk (U)
: : :
Firstly we observe that h : ker(r) ! ker() is an isomorphism. Indeed
let x be in ker(). Since x = 0, then jx = 0, but the diagram commutes
and x is also the kernel of Hk( ~X
) ! Hk (U) and hence, there exists in
9
161. Hk2 (E) mapping to x. It is easy to see that belongs to ker(r). Thus the
map is surjective.
It is also injective because if hx = 0 then there exist
162. in Hk1 (U)
mapping to x. The diagrams commutes and so in the second lines,
163. maps
to zero and, hence, there exists z in Hk1 (X) mapping to
164. . The map is
surjective and so there exists z0 in Hk1( ~X
) mapping to
167. has to map to zero and so x = 0. Finally we observe that ker(r) is
exactly Hk2 (Y ) Hk2(d1) (Y ). This shows that Hk : K0(Vark) !
L0(Ab) is well de
169. rst to the Motivic ring and then to
cK0(Vark).
Without confusion we denote by 1, the class of a point fg in cK0(Vark)
and we also denote by 1 = fZg 2 L0(Ab). With this notation, H (1) = 1.
We
175. nition of these invariants that do
not involve the concept of algebraic stacks.
Let V be a faithful representation of a
176. nite group G. The group G acts
component-wise on V m. Consider the quotient scheme V m=G that is usually
a singular scheme.
De
177. nition 4.1. Let V be a n-dimensional faithful k-representation of a
178. nite
group G and let X be a smooth and proper resolution of V m=G:
X ! V m=G:
For m large enough, the i-th Ekedahl invariant is de
179. ned as follows:
ei (G) = fH2mi (X;Z)g +
X
j
njfH2mi (Xj ;Z)g 2 L0(Ab);
where fV m=Gg 2 K0(Vark) is written as the sum P
of classes of smooth and
proper varieties fXg and fXjg, fV m=Gg = fXg +
j njfXjg.
10
180. We are going to prove that there exists a positive integer M such that for
any m greater then M the i-th Ekedahl invariant ei (G) stabilizes in L0(Ab).
Moreover we show that the two given de
183. nition
3.2.
Proof. We have seen in Proposition 2.6.b) that
fB Gg = lim
m!1
fV m=GgLmn 2 cK0(Vark):
From Theorem 3.1, the map Hk is continuous and so, for m large enough,
Hi (fB Gg) = Hi
= H2mni (fV m=Gg;Z) ;
fV m=GgLmn;Z
where the shifting 2mn comes from the multiplication for Lmn.
We, now, consider a compacti
184. cation and resolution of the singularities
of V m=G. This allows to write fV m=Gg as a suitable sum fXg +
P
j njfXjg
where fXg is smooth, proper and birational to V m=G, the Xj's are smooth
and proper with dimension strictly less then dim(V m=G) = mn and nj 2 Z.
Therefore,
ei (G) = Hi (fB Gg) = fH2mni (X;Z)g +
X
j
njfH2mni (Xj ; Z)g:
This proves that the two de
185. nitions are equivalent and well posed.
4.1 The state of the art
The following theorem links to the Noether problem.
Theorem 4.3 (Theorem 5.1 in [4]). We denote by B0(G)_ the dual of the
Bogomolov multiplier of the group G. If G is a
186. nite group, then
a) ei (G) = 0, for i 0;
b) e0 (G) = fZg;
c) e1 (G) = 0;
11
187. d) e2 (G) = fB0(G)_g + fZg for some integer .
Proof. By De
188. nition 4.1,
ei (G) = fH2mni (X;Z)g +
X
j
njfH2mni (Xj ;Z)g;
where X is a smooth and proper resolution of V m=G; V is a n-dimensional
faithful k-representation of a
189. nite group G and fV m=Gg is written in K0(Vark)
as the sum of classes of smooth and proper varieties fXjg, fV m P =Gg = fXg +
j njfXjg.
Let i = 0. The only surviving cohomology is H2mn (X;Z) = Z, because
dim(Xj) dim(V m=G) = mn. Thus, e0 (G) = fH2mn (X;Z)g = fZg.
If i = 1, for similar reasons, e1 (G) = fH2mn1 (X;Z)g. Since X is bira-tional
to V m=G, one has the inclusion k(X) ' k(V=G) k(V ) and hence X is
unirational and, therefore, simply connected. Thus, using the result of Serre
in [11], H2mn1 (X; Z) ' H1(X;Z) = 0 and thus e1 (G) = 0.
Regarding e2 (G), one
190. rstly observes, by Poincare duality, that
tor(H2mn2 (X;Z)) =
tor(H3(X;Z)):
Artin and Mumford have proved in [1] that tor(H3 (X;Z)) is a birational
invariant and Bogomolov in [3] proved that this is exactly B0(G). Therefore,
we have proved that e2 (G) = fB0(G)_g + fZg for some integer .
Observation 4.4. Bogomolov proved in Theorem 1.1 of [3] that if X is
smooth, proper and unirational the Brauer group Brv(K) is isomorphic to
tor(H3 (X;Z)), with K = k(X). Moreover he de
191. ned Brv(G) = Brv(k(X)),
where X is smooth, proper and birational to V=G with V being any generically
free representation of G. Thus, in Theorem 3.1 of [3], he has proved that
Brv(G) = B0(G).
Using these results, one
193. rst examples of group with non trivial
Ekedahl invariants.
Proposition 4.5 (Non triviality). The second Ekedahl invariant is non triv-
ial for every algebraically closed
194. eld k with char(k) = 0 and for the groups
of order p9 given by Saltman in [10] and of order p6 given by Bogomolov in
[3]. Moreover in these cases, fBGg6= 1 in cK0(Vark).
12
196. nite group and so if B0(G)6= 0,
then e2 (G) = fB0(G)_g + fZg6= 0.
Ekedahl actually proved a more precise statement.
Theorem 4.6 (Theorem 5.1 of [4]). For i 0, ei (G) is the sum (with signs)
of classes of
197. nite groups in L0(Ab).
Proof. We refer to point e) of Theorem 5.1 in [4].
Corollary 4.7. The second Ekedahl invariant is exactly e2 (G) = fB0(G)_g,
where B0(G)_ is the dual of the Bogomolov multiplier of the group G;
Proof. We already proved in Theorem 4.3.d) that e2 (G) = fB0(G)_g+fZg
for some integer . Using the previous theorem one gets = 0.
Another connection between the Noether problem and the non-triviality of
fB Gg is also the next proposition.
Proposition 4.8 (Corollary 5.8 in [4]). fB Z=47Zg6= 1 in cK0(VarQ).
To the authors knowledge, there are no examples in literature of
198. nite
group G such that B0(G) = 0 and e3 (G)6= 0. Vice versa a lot of groups
have trivial Ekedahl invariants.
Theorem (Prop 3.2, Cor 3.9, Thm 4.3 in [4]). Assume one of the following
cases:
1) if G is the symmetric group and for every
203. nite subgroup of the group of ane transformations of A1
k and
for every algebraically closed
204. eld k.
Then fB Gg = 1 2 cK0(Vark) and the trivial Ekedahl invariants are trivial.
Recently the author has proved also the following facts:
Theorem (Thm 2.5 in [8]). If G is a
205. nite subgroup of GL3(C), then fB Gg =
1 2 cK0(Vark) and it has trivial Ekedahl invariants.
13
206. The previous result extend point 2) in Theorem 4.1.
Theorem (Thm 4.4 in [8]). The Ekedahl invariants of the
207. fth discrete
Heisenberg group, ei (H5), are trivial.
Acknowledgements
I thank Angelo Vistoli for the great mathematical support in this subject.
References
[1] M. Artin and D. Mumford, Some elementary examples of unira-
tional varieties which are not rational, Proc. London Math. Soc. (3), 25
(1972), pp. 75{95.
[2] F. Bittner, The universal Euler characteristic for varieties of charac-
teristic zero, Compos. Math., 140 (2004), pp. 1011{1032.
[3] F. A. Bogomolov, The Brauer group of quotient spaces of linear rep-
resentations, Izv. Akad. Nauk SSSR Ser. Mat., 51 (1987), pp. 485{516,
688.
[4] T. Ekedahl, A geometric invariant of a
208. nite group.
arXiv:0903.3148v1, 2009.
[5] , The grothendieck group of algebraic stacks. arXiv:0903.3143v2,
2009.
[6] W. Fulton, Intersection theory, vol. 2 of Ergebnisse der Mathematik
und ihrer Grenzgebiete. 3. Folge. A Series of Modern Surveys in Mathe-matics
[Results in Mathematics and Related Areas. 3rd Series. A Series
of Modern Surveys in Mathematics], Springer-Verlag, Berlin, second ed.,
1998.
[7] A. Hatcher, Algebraic topology, Cambridge University Press, Cam-bridge,
2002.
[8] I. Martino, The ekedahl invariants for
209. nite groups. arXiv:1312.0476,
2013.
[9] E. Noether, Gleichungen mit vorgeschriebener Gruppe, Math. Ann.,
78 (1917), pp. 221{229.
14
210. [10] D. J. Saltman, Noether's problem over an algebraically closed
211. eld,
Invent. Math., 77 (1984), pp. 71{84.
[11] J.-P. Serre, On the fundamental group of a unirational variety, J.
London Math. Soc., 34 (1959), pp. 481{484.
[12] R. G. Swan, Invariant rational functions and a problem of Steenrod,
Invent. Math., 7 (1969), pp. 148{158.
15
224. eld k of characteristic zero. In [4], Ekedahl
investigates when the equality
fGL(V )=Gg = fGL(V )g (1)
holds in the Kontsevich value ring cK0(Vark) of algebraic k-varieties. One
of the motivations for Ekedahl investigations into cK0(Vark) was to make
Motivic versions of point counting over
233. ne Hk on cK0(Vark) is enough to set Hk(fXg=Lm) =
fHk+2m (X;Z)g for every smooth and proper k-variety X (see Section 3 in
[8]).
The class fB Gg of the classifying stack of G could be seen as an element
of cK0(Vark) (see Proposition 2.6.b in [8]) and so one can de
235. nition 1.2. For every integer i, the i-th Ekedahl invariant ei (G) of the
group G is Hi(fB Gg) in L0(Ab). We say that the Ekedahl invariants of G
are trivial if ei (G) = 0 for all integer i6= 0.
In Proposition 2.6.a of [8], the author rephrases the equality (1) in terms of
stacks, using the expression
fB Gg =
fGL(V )=Gg
fGL(V )g
2 cK0(Vark):
Therefore (1) holds if and only if fB Gg = 1 and, if this is the case, then
the Ekedahl invariants of G are trivial, because H0(1) = fZg and Hk(1) = 0
for k6= 0. These invariants seem a natural generalization of the Bogomolov
multiplier B0(G) (see [3]), because e2 (G) = fB0(G)_g (see Section 5 of [8]).
Here B0(G)_ stands for the dual of B0(G)_.
The Bogomolov multiplier B0(G) is an obstruction to the rationality of
F(xg; g 2 G)G=F and thus, if the second Ekedahl invariant of G is not zero,
then the group is a counterexample to the Noether Problem. It is not clear
if this assertion is true for higher Ekedahl invariants. Moreover fB Gg = 1
implies that all the invariants are trivial, but we have no information about
the converse.
In this paper we work over the complex numbers and we prove that:
Theorem 3.1. Let G be a
236. nite subgroup of GLn (C) and let H be the image
of G under the canonical projection GLn (C) ! PGLn(C).
If H is abelian and if Pn1
=H has only zero dimensional singularities, then for
C every integer k
ek (G) + ek+2 (G) + + ek+2(n1) (G) = fHk (X; Z)g;
where X is a smooth and proper resolution of Pn1
C =H.
In law dimensions, one can say more.
2
238. nite subgroup of GL3 (C), then fB Gg = 1 in
cK0(VarC) and the Ekedahl invariants of G are trivial.
The case when G is a
239. nite subgroup of GL4 (C) is more complicated because
it involves a deep study of the resolution of singularities of the ane varieties
C3=A, for a
240. nite group A GL3 (C), which are not well known a part few
cases.
For this reason we focus on the p-discrete Heisenberg group Hp, where
we only deal with cyclic quotient singularities.
Given a prime p we denote by Hp the subgroup of the upper triangular
matrices of GL3 (Fp). In particular, Hp GLp (C). This is an interesting
candidate for the study of the Ekedahl invariants, because B0(Hp) = 0 (using
Lemma 4.9 in [3]) and so the
241. rst unknown Ekedahl invariant is e3 (Hp).
Theorem 4.4. The Ekedahl invariants of the
242. fth discrete Heisenberg group
H5 are trivial.
We show a general approach for the study of the Ekedahl invariants of Hp,
but we narrow down our investigation to p = 5 because of the diculties to
extend the technical result in Theorem 4.7.
To author's knowledge, there are no examples of
243. nite group G such that
B0(G) = 0 (i.e. e2 (G) = 0) and e3 (G)6= 0.
After a preliminary section where we review the theory of the Ekedahl
invariants, in Section 2 we prove that these are trivial for all
247. nite group. In Section 1, we work over an
algebraically close
248. eld k of characteristic zero. In the rest of the paper, the
ground
249. eld is C.
1 Preliminaries
The Grothendieck ring of algebraic varieties K0(Vark) is the group generated
by the isomorphism classes fXg of algebraic k-varieties X, subject to the
relation fXg = fZg+fX nZg, for all closed subvarieties Z of X. The group
K0(Vark) has a ring structure given by fXg fY g = fX Y g. Let L be the
3
250. class of the ane line. The completion of K0(Vark)[L1] with respect to the
dimension
251. ltration
Filn
K0(Vark)[L1]
= ffXg=Li : dimX i ng
is called the Kontsevich value ring and denoted by cK0(Vark).
From now on, we denote by fg the class of a point in cK0(Vark). We also
use sometime the notation 1 = fg 2 cK0(Vark).
Remark 1.1. Let G be a special group and let X ! Y be a G-torsor of
algebraic stacks of
252. nite type over k, then fXg = fGgfY g in K0(Stackk)
(see [5]). Moreover, if F is a G-space and Z ! Y is a F-
253. bration associated
to the G-torsor X ! Y and to the action on F, then fZg = fFgfY g in
K0(Stackk).
We observe that the completion map from K0(Vark)[L1] to cK0(Vark)
factors through the Grothendieck ring K0(Stackk) of algebraic stacks of
254. nite
type over k (see Lemma 2.2 in [8]). The classifying stack of the group G is
usually de
255. ned as the stack quotient B G = [=G] and, via this map, one
sees the class of the classifying stack fB Gg as an element of cK0(Vark) (see
Lemma 2.6.b in [8]).
Using the Bittner presentation (see [2]), given a integer k Ekedahl de
256. nes
in [5] a cohomological map for the Kontsevich value ring, sending fXg=Lm to
fHk+2m (X;Z)g, for every smooth and proper k-variety X:
Hk : cK0(Vark) ! L0(Ab)
fXg=Lm7! fHk+2m (X; Z)g:
In Section 3 of [8], we prove that this map is well de
257. ned.
Notation. Every cohomology group (if not explicitly expressed dierently)
is the singular cohomology group with integer coecients, that is Hk () =
Hk (;Z).
De
258. nition 1.2. For every integer i, the i-th Ekedahl invariant ei (G) of the
group G is Hi(fB Gg) in L0(Ab). We say that the Ekedahl invariants of G
are trivial if ei (G) = 0 for all integer i6= 0.
The reason for the minus sign in the above de
262. nite groups where fB Gg6= 1 are counterexamples to
the Noether Problem. In [10], Noether wondered about the rationality of
the extension F(V )G=F for any
266. rst counterexample,
Q(V )Z=47Z=Q, was given by Swan in [13]. Later more counterexamples were
found: for every prime p Saltman (in [12]) and Bogomolov (in [3]) showed
that there exists a group of order p9 and, respectively, of order p6 such that
the extension C(V )G=C is not rational.
Saltman used the second unrami
268. eld C(V )G,
H2
nr(C(V )G; Q=Z), as a cohomological obstruction to the rationality. Later,
Bogomolov found a group cohomology expression for H2
nr(C(V )G; Q=Z) which
now takes his name and it is denoted by B0(G).
To see the connection to the Noether problem we use the following result.
Theorem 1.4 (Thm 5.1 of [4]). If G is a
269. nite group, then e0 (G) = fZg,
e1 (G) = 0 and e2 (G) = fB0(G)_g, where B0(G)_ is the dual of the Bogo-
molov multiplier of the group G.
Moreover, for i 0, the invariant ei(G) is a sum (with signs) of classes of
270. nite abelian groups.
Using that e2 (G) = fB0(G)_g, one proves that, for the Saltman and Bogo-molov
counterexamples, the Ekedahl invariants are non-trivial and so fB Gg6=
1. In addition, fB Z=47Zg6= 1 2 cK0(VarQ) (see page 7 of [4]).
Corollary 1.5. If G is one of the group de
271. ned in [12] and in [3] as coun-
terexample to the Noether problem, then the second Ekedahl invariant is non-
zero and so fB Gg6= 1.
Proposition 1.6 (State of the art). Assume one of the following cases:
1) if G is the symmetric group and for every
278. Then fB Gg = 1 2 cK0(Vark).
Proof. See Proposition 3.2, Corollary 3.9 and Theorem 4.3 in [4].
All these results imply the triviality for the Ekedahl invariants. We underline
that in this work we extend the result in item 2), because we prove that
fB Gg = 1 for every
279. nite subgroup of GL3.
A more complete and self contained introduction to the Ekedahl invariants
can be found in [8].
2 The
281. eld. Let G be a subgroup of GLn and
H be its reduction in PGLn:
0 K G H 0
_
0 C
_
GLn
_
PGLn
0:
In what follows we set V = Cn (as a linear representation of G).
Notation. We sometime use for simplicity Pn1 for the projective space
P(V ). We also denote by Idn the identity element of GLn.
To get information about fB Gg, we study f[P(V )=G]g.
Lemma 2.1 (Lemma 2.5 of [8]). f[P(V )=G]g = (1 + L + + Ln) fB Gg in
cK0(VarC).
By de
282. nition H acts on P(V ) and P(V )=G =
P(V )=H. Their stack quo-tients
are not isomorphic, but the classes of their stack quotients are equal
in cK0(VarC).
Proposition 2.2. f[P(V )=G]g = f[P(V )=H]g 2 cK0(VarC).
Proof. We denote by VO = V nfOg, where O is the origin of V . Since [VO=G] !
[P(V )=G] is a C-torsor, f[VO=G]g = (L 1)f[P(V )=G]g (we use Remark 1.1).
Similarly from [(VO=K)=H] ! [P(V )=H], one gets f[(VO=K)=H]g = (L1)f[P(V )=H]g.
The statement follows from [(VO=K)=H] = [VO=G].
6
283. We stress that the previous lemma and proposition holds for any algebraically
closed
286. nite groups.
Let Y be a smooth quasi-projective algebraic variety and let A be a
287. nite
group of automorphisms of Y . Let Y ! Y=A be the canonical quotient map
and y be the image of y.
The pseudo re
ection subgroup Pseudo (G) of G GL(V ) is its subgroup
generated by pseudo-re
ections. The Chevalley-Shephard-Todd Theorem
says that the quotient V=G is smooth if and only if G = Pseudo (G).
The well known Cartan Lemma says that for all the points y of Y , the action
of the stabilizer Staby(A) of y on Y induces an action of Staby(A) on the
tangent space on y, TyY . Moreover the analytic germ (Y=A; y) is isomorphic
to (TyY=A; O
), where O
is the image of the origin O 2 TyY under the quotient
map TyY ! TyY=A. An easy consequence is that for all the points y of Y ,
Staby(A) GLdim(Y ) and one also proves that p is a singular point of V=G,
p 2 Sing (V=G), if and only if Pseudo (Stabp(G))6= Stabp(G).
We are going to use also the following fact. A proof can be found, for instance,
in the lemma in Section 1.3 of [11].
Lemma 2.3. Let y 2 Y=A. The germ (Y=A; y) is a simplicial toroidal sin-
gularity (i.e. locally isomorphic, in the analytic topology, to the origin in a
simplicial toric ane variety) if and only if the quotient Staby(A)=Pseudo(Staby(A))
in TyY is abelian.
Comparing the classes f[P(V )=H]g and fP(V )=Hg, we are going to prove that
the Ekedahl invariants for every
288. nite subgroup G in GL3 (C) are trivial.
We prove it by induction and the base of such induction is the item 2) in
Proposition 1.6: if G is a
289. nite subgroup of GL1 (C) then fB Gg = 1 in
cK0(VarC).
Proposition 2.4. If G is a
290. nite subgroup of GL2 (C) then fB Gg = 1 in
cK0(VarC) and the Ekedahl invariants of G are trivial.
Proof. Let U be the open subset of P1 where H acts freely. Then
f[P1=H]g = fU=Hg +
X
p
f[p=Stabp(H)]g = fU=Hg +
X
p
fB Stabp(H)g;
7
291. where the sum runs over the points with non trivial stabilizer. Similarly
fP1=Hg = fU=Hg +
X
p
fg
and so
f[P1=H]g = fP1=Hg +
X
p
(fB Stabp(H)g fg):
Using (in order) that f[P1=G]g = (1 + L) fB Gg, Proposition 2.2, the previ-ous
formula and P1=H =
P1, one has
fB Gg(1 + L) = fP1g +
X
p
(fB Stabp(H)g fg):
Using Cartan's Lemma, Stabp(H) is a subgroup of GL1 and, hence, for Propo-sition
1.6.2), fB Stabp(H)g = fg for every non trivial stabilizer point p.
Hence, fB Gg(1 + L) = fP1g and this implies fB Gg = 1, because Ln 1 is
invertible in cK0(Vark), L2 1 = (L 1)(L + 1) and so 1 + L is invertible
too.
Theorem 2.5. If G is a
292. nite subgroup of GL3 (C) then fB Gg = 1 in
cK0(Vark) and the Ekedahl invariants of G are trivial.
Proof. Using equation f[P2=G]g = (1 + L + L2) fB Gg and Proposition 2.2,
we know that fB GgfP2g = f[P2=H]g. Since fP2g is invertible in cK0(Vark),
it is sucient to prove that f[P2=H]g = fP2g.
Let U be the open subset of P2 where H acts freely and let C be the
complement of U in P2. We denote by C0 and C1 respectively the dimension
zero and the dimension one closed subsets of C so that C = C0 t C1.
One observes that [C0=H] is the disjoint union of a
293. nite number of quotient
stacks [Oi=H] where Oi are the orbits of Pi 2 C0 under the action of H.
We note that [Oi=H] = [Pi=StabPi (H)] = B StabPi(H). By Cartan's Lemma,
StabPi(H) is a subgroup of GL2 (C) and then, by using Proposition 2.4,
f[Oi=H]g = fB StabPi(H)g = fOi=Hg = fg = 1:
Therefore f[C0=H]g = fC0=Hg.
We observe that f[S=H]g = fS=Hg holds for every
296. nite number of lines Li. We denote by I,
the subset of C1, made by the intersection points of those lines Li. We also
denote by C
1 the complement of I in C1.
Let L be a line in C1 and SL = StabL(H). Since H PGL3, then one sees
that SL StabL(PGL3) H. We observe that StabL(PGL3) =
GL2 nC2
because a class in StabL(PGL3) has the form
2
4
0
@
1 0 0
GL
2
1
A
3
5
and therefore StabL(PGL3) =
GL2 nC2. So one has the group homomor-phism
GL2 nC2 ! GL2 sending (g; x) to g. The kernel of such homomor-phism
restricted to SL is trivial, because ker(GL2 nC2 ! GL2) = C2 and
then ker(SL ! GL2) = SL C2 = 0. Thus, SL GL2 and, using the
Proposition 2.4, one gets f[L=SL]g = fL=SLg.
We set L0 = L C
1 . Then [L=SL] = [L0=SL] [ [LnL0=SL]. For what we said for
0j
the zero dimensional case f[LnL0=SL]g = fLnL0=SLg and so f[L0=SL]g = fL0=SLg.
We call Othe orbit of L0
j under H. Since C
1 is the disjoint union of a
297. nite
number of orbits O0j
, then
f[C1=H]g = f[C
1=H]g + f[I=H]g =
X
j
f[O0 j=H]g + f[I=H]g
=
X
j
f[L0
j=SLj ]g + f[I=H]g
=
X
j
fL0
j=Hg + fI=Hg = fC1=Hg:
Summarizing the proven facts, one has
f[P2=H]g = f[U=H]g+f[C0=H]g+f[C1=H]g = fU=Hg+fC0=Hg+fC1=Hg = fP2=Hg:
Therefore there remains to prove that fP2=Hg = fP2g. For this purpose let
X be a resolution of the singularities of P2=H, : X ! P2=H. An unirational
surface (over C) is rational and one can construct a birational morphism on
P2, 0 : X ! P2. The quotient singularities of P2=H are rational singularities
and the exceptional divisor Dy of y 2 Sing (P2=H) is a tree of P1. This implies
that Dy = [ny
j=1P1, where ny is the number of irreducible components of
Dy. Then fDyg = nyfP1g
P
i;jfg. Since the graph of the resolution is
9
298. a tree, then there are exactly ny 1 intersection points in
P
i;jfg. Hence
fDyg = nyfP1g (ny 1) = nyL + 1. Then,
fP2=Hg = fXg
X
y
(fDyg fyg) = fXg
X
y
(nyL + 1 1)
= fXg L
X
y
ny = fXg Ln;
where n =
P
y ny is the number of irreducible components in the full excep-tional
divisor D = [yDy. Similarly, one gets fP2g = fXg Lm, where m
is the number of irreducible components in the full exceptional divisor E of
the resolution X 0
! P2.
We shall prove that m = n. Let us consider the following spectral se-quence
from the map : X ! P2=H:
2 = Hi
Ei;j
P2=H;Rj:QX
) Hi+j (X;Q) :
Since the map is an isomorphism a part a
300. ned over those points (and zero elsewhere). Let y be one of those:
(Rj:QX)y = Hi (1(y);Q) and so H0 (1(y);Q) = Qn and for i 0,
Hi (1(y);Q) = 0. The spectral sequence degenerates and then we obtain
0 ! Q ! H2 (X;Q) ! Qn ! 0:
This implies H2 (X;Q) = Qn+1. Similarly, for 0 : X ! P2, one gets
H2 (X;Q) = Qm+1 and, thus, the equality m = n.
The diculties to continue such induction up to GL4 (C) arise from the
study of the resolution of singularities of P3=H. In general for bigger n, Car-tan's
Lemma reduces this question to the study of the quotients Cn1=A for
certain A GLn1 and those are not well known.
3 Finite groups with abelian projective re-
duction
As in the previous section G is a subgroup of GLn and H is its reduction in
PGLn. If H is abelian and if the singularities of Pn1=H are zero dimensional,
then the Ekedahl invariants satisfy a recursive equation.
10
302. nite subgroup of GLn (C) and let H be the image
of G under the canonical projection GLn (C) ! PGLn(C).
If H is abelian and if Pn1=H has only zero dimensional singularities, then for
every integer k
ek (G) + ek+2 (G) + + ek+2(n1) (G) = fHk (X;Z)g;
where X is a smooth and proper resolution of Pn1=H.
We
303. rst show a technical lemma. We denote by pX(t) =
P
i0
304. i(X)ti the
virtual Poincare polynomial of a complex algebraic scheme X, where
305. i(X) =
dim(Hi (X;Q)) is the i-th Betti number of X. For every smooth projective
toric variety Y , the odd degree coecients of pY (t) are zero (Section 5.2 of
[6]). In addition, if G is a
306. nite subgroup of GLn as above, then pPn1=H(t) =
pPn1(t). Indeed H (Pn1=H;Q) = H (Pn1;Q)H = H (Pn1;Q).
Lemma 3.2. Let G, H, Pn1=H and X satisfy the hypothesis of Theorem 3.1.
Then:
i) fB Gg(1 + L + + Ln1) = fPn1=Hg and, in particular,
ek (G) + ek+2 (G) + + ek+2(n1) (G) = Hk (fPn1=Hg) :
ii) Every singularity of Pn1=H is a toroidal singularity and
fPn1=Hg = fXg
X
y
(fDyg fyg) ; (2)
where the sum runs over y 2 Sing (Pn1=H); fDyg is the exceptional di-
visor of the toric resolution of y with irreducible components decomposi-
tion Dy = D1
y[ [Dry
; fDyg =
P
q1(1)q+1P
i1;:::;iq
y Diq
fDi1
y g.
iii) If k is non-zero and even, one has
1 =
312. odd(X) = 0.
Proof. By assumptions Pn1=H has only zero dimensional singularities. Re-garding
item i) we observe that
f[Pn1=H]g = fPn1=Hg +
X
j
(fB StabPj (H)g fg)
where the sum runs over the orbits of points with nontrivial stabilizer in
Pn1 and Pj is a point in such an orbit. Every stabilizer group of H is
abelian and we know, by Proposition 1.6.2) that fB StabPj (H)g = 1. So
f[Pn1=H]g = fPn1=Hg. Using also Proposition 2.2, we obtain the
313. rst part of
i). For the second one, we note that applying the cohomological map Hk
on the left hand side, one has:
Hk
fB Gg(1 + + Ln1)
= Hk (fB Gg) + + Hk
fB GgLn1
= Hk (fB Gg) + + Hk2(n1) (fB Gg)
= ek (G) + + ek+2(n1) (G) :
Every stabilizer group of H is abelian and so it is for the quotient of
Stabx(H) modulo Pseudo (Stabx(H)) in TxX. Then, for Lemma 2.3, each
singularity of fPn1=Hg is an isolated simplicial toroidal singularities. One
produces a toric resolution with normal crossing toric exceptional divisors
(see Section 2.6 of [6]). We mean that calling Dy the exceptional divisor of
the resolution of the toroidal singularity y in Pn1=H, Dy = D1
y [ [ Dry
y Diq
and each intersection Di1
y is a smooth toric varieties. Hence, one
has equation (2) and fDyg =
P
q1(1)q+1P
i1;:::;iq
y Diq
fDi1
y g. Thus,
pDy (t) =
P
q1(1)q+1P
i1;:::;iq
pD
i1
y D
iq
y
(t) and the odd degree coecients
of pDy (t) are zero.
We want to compute the virtual Poincare polynomial of X. Via formula
(2) and using pPn1=H(t) = pPn1(t),
pPn1(t) = pX(t)
X
y
(pDy (t) 1):
Comparing, degree by degree, the polynomial in the left hand side and in the
right hand side, one gets the Betti numbers equalities and item iv).
12
315. rst item of the previous lemma, we know
that
ek (G) + ek+2 (G) + + ek+2(n1) (G) = Hk (fPn1=Hg) : (3)
We shall show that Hk (fPn1=Hg) = fHk (X;Z)g. For this, we study a
resolution of the singularities of Pn1=H. Using the previous technical lemma
we express P
fPn1=Hg in (2) as a sum of smooth and proper varieties and
fDyg =
q0(1)q+1P
i1;:::;iq
y Diq
fDi1
y g where Dy is the exceptional
divisor of the resolution of the singularity y in fPn1=Hg. Moreover Dy =
D1
y [ [ Dry
, where Djy
y Diq
and each intersection Di1
y are smooth
toric varieties.
If k 0 or k 2(n 2), Hk (fDyg fyg) = 0 for dimensional reason
and so the recurrence holds.
Similarly if k is odd integer between 0 and 2(n2) because the cohomology
of a smooth toric variety is torsion free.
It remains the case 0 k = 2j 2(n 2). For these values, in the left
hand side of (3), there are some negative Ekedahl invariants (so zero), e0 (G)
and some positive even Ekedahl invariants e2 (G) + + e2j+2(n1) (G) that
are sum (with sign) of classes of
316. nite abelian groups (we use the second part
of Theorem 1.4).
On the right hand side of (3) the only possible torsion part is ftorHk (X;Z)g,
because the cohomologies of a smooth toric variety is torsion free (see Section
5.2 in [6]). Hence, what remains to prove is that the free parts cancel each
others: for k6= 0,
fZg =
317. k(X)fZg
X
y
X
q1
(1)q+1
X
i1;:::;iq
y Diq
y )fZg
320. 0(Di1
fZg:
y Diq
y ) 1
These follow from the Lemma 3.2.iii).
13
321. 4 The discrete Heisenberg group Hp
Let p be a prime dierent from two. The p-discrete Heisenberg group Hp is
the following subgroup of GL3 (Fp):
Hp =
8
:
0
@
1 a b
0 1 c
0 0 1
1
A : a; b; c 2 Fp
9=
;:
If we denote by
M(a; b; c) =
0
@
1 a b
0 1 c
0 0 1
1
A;
then we observe that Hp is generated by X = M(1; 0; 0), Y = M(0; 0; 1) and
Z = M(0; 1; 0) modulo the relations ZYX = XY, Zp = Xp = Yp = Id,
ZX = XZ and ZY = YZ. The center of Hp, ZHp, is generated by Z and
we denote by Ap the group quotient Hp=ZHp
=
Z=pZ Z=pZ. Moreover, Hp is
the central extension of Z=pZ by Z=pZ Z=pZ:
1 ! Z=pZ ! Hp
!
Z=pZ Z=pZ ! 1;
and then, using Lemma 4.9 in [3], one proves that the Bogomolov multiplier
B0(Hp) is zero for every prime p.
We also remark that the discrete Heisenberg group has p2 +p1 irreducible
complex representations: p2 of them are one dimensional and the remaining
p 1 are faithful and p-dimensional.
Let V be a faithful irreducible p-dimensional complex representation of
Hp, Hp
!
GLp (C). There is a natural action of Hp on V and it induces an
action on Pp1. One so de
322. nes the quotient Pp1=Hp.
Since Z belongs to the center, (Z) = e
2i
p Idp, for some 0 i p. Hence,
the center acts trivially on Pp1 and Pp1=Hp
=
Pp1=Ap. From Lemma 2.3, we
know that if Pp1=Ap has singularities, then they are toroidal. We study these
singularities and so we focus on Stabx(Ap).
Proposition 4.1. Let x 2 Pp1. If the action of Ap at x is not free, then
j Stabx(Ap)j = p.
Proof. Let Wx be the one dimensional subvector-space of V corresponding
to x. The stabilizer of x is a subgroup of Ap and, by Lagrange's Theorem
14
323. (and using the assumptions), it could have order p or p2. If Stabx(Ap) = Ap,
then for every g 2 Ap; gWx = Wx and ApWx = Wx. Then HpWx = Wx. This
implies that Wx is an one dimensional irreducible Hp-subrepresentation of V
contradicting the fact that Hp acts irreducibly.
There are exactly p+1 subgroups of order p in Ap. Let B be one of them.
=
We de
324. ne B b as a subgroup of Hp such that j B b is a group isomorphism:
B b Z=pZ 1(B).
We restrict the representation Hp
!
GLp (C) to the subgroup b B = Z=pZ.
We write V as a direct sum of one dimensional irreducible representations:
V = 2Z=pZV, where V = fv 2 V : g v = (g) v; 8g 2 Z=pZg. In other
words, b B
325. xes p one dimensional linear subspaces V and so B
326. xes p points
P 2 Pp1, with StabP(Ap) = B, that is (Pp1)B = fP0 ; : : : ; Pp1g.
Proposition 4.2. If B and B0 are two distinct p-subgroups of Ap, then
(Pp1)B (Pp1)B0 = ;.
Proof. Trivially, Ap = BB0 and if P 2 (Pp1)B(Pp1)B0 , then StabP (Ap) =
Ap, contradicting Proposition 4.1.
We observe that Ap=B acts regularly on (Pp1)B. Thus, these points are a
unique orbit under the action of Ap=B and this means that they correspond
to a unique point yB in Pp1=Ap.
Theorem 4.3. The quotient Pp1=Ap has p + 1 simplicial toroidal singular
points.
=
Proof. There are exactly p+1 subgroups, B, of order p in Ap. Each of them
corresponds to a point yB in Pp1=Ap. By Proposition 4.2, these points are
distinct.
Let y 2 Pp1 such that y = yB. We consider the action of Staby(Ap) on
the tangent space TyPp1. The pseudo-re
ection group Pseudo (Staby(Ap))
is zero, because it is a subgroup of Staby(Ap) Z=pZ and, so, it is either the
trivial group or Staby(Ap). The latter is not possible because Staby(Ap) stabi-lizes
only the origin of the vector space TyPp1. Thus, Pseudo (Staby(Ap))6=
Staby(Ap) in TyPp1 and for Lemma 2.3 these singularities are also toroidal
and simplicial.
15
327. We now draw a method to calculate the Ekedahl invariants for Hp: we
write fPp1=Apg as a sum of classes of smooth and proper varieties and we use
Theorem 3.1.
Let Xp
f!
Pp1=Ap be the resolution of the p+1 toroidal singularities of Pp1=Ap.
One has the following geometrical picture:
P(V ) U
Xp
_
f
Pp1=Ap
^
[
Up
f
_
Up
where U is the open subset of P(V ) where Ap acts freely; Up = U=Ap and Xp
is a smooth and proper resolution of Pp1=Ap.
Since Ap is abelian, using Theorem 3.1 one gets
ek (G) + ek+2 (G) + + ek+2(p1) (G) = fHk (Xp;Z)g:
Because of Theorem 1.4, e0 (Hp) = fZg and e1 (Hp) = e2 (Hp) = 0. Thus, we
focus on e3 (Hp). We are going to show that e3 (H5) = e4 (H5) = 0. We set
p = 5 because of the hardness to compute tor(H (Xp;Z)), for every p.
Claim. tor(H5 (X5;Z)) = 0.
Using this, we prove the main results.
Theorem 4.4. The Ekedahl invariants of the
328. fth discrete Heisenberg group
H5 are trivial.
Proof. By using Theorem 3.1 for G = H5, n = 5, k = 2 5 + 5 and
X = X5 and also by applying the second part of Theorem 1.4, we have
e3 (H5) = ftor
H255 (X5; Z)
g = ftor
H5 (X5;Z)
g and then, for duality,
e3 (H5) = ftor
H5 (X5; :)Z
g = ftor
H4 (X5;Z)
g
and this is zero for the claim. Similarly, for k = 2 5 + 6,
e4 (H5) = ftor
H256 (X5;Z)
g = ftor
H4 (X5;Z)
g:
16
329. Moreover, e3 (H5) and e4 (H5) are the only invariants that could not be
zero. Indeed, e5 (H5) = ftor
H3 (X5;Z)
g = e2 (H5) = 0 and e6 (H5) =
ftor
H2 (X5; Z)
g = e1 (H5) = 0. In addition, ei (H5) = 0 for i 6 for
dimensional reason.
We observe that the same proof would follow for Hp having enough informa-tion
about the vanishing of the torsion in the cohomology of Xp.
4.1 Proof of the claim
To obtain the proof of the claim we need to show that Hodd (U5;Z) = 0 and
H5
E (X5;Z) = 0 are zero, where E is the union of exceptional divisors of the
resolution X5
f!
P51=A5. The
330. rst fact is actually true for Up.
Theorem 4.5. The cohomology of the smooth open subset Up of P(V )=Ap for
k 2p 2 is
Hk (Up;Z) =
8
:
Z if k = 0;
0 if k is odd;
Z (Z=pZ)
k
2 +1 if k6= 0 and even:
Proof. Since Ap acts freely on U, let us consider the Cartan-Leray spectral
sequence (see Section 5 or Theorem 8bis:9 in [9]) relative to the quotient map
: U ! Up:
2 = Hi
Ei;j
) Hi+j (Up;Z) :
Ap;Hj (U;Z)
Let Sp = Pp1 n U. One sees that Hi (U;Z) =
Hi (P(V ); Z) for i 2p 3,
H2p3 (U;Z) = Z[Sp]0 and H2p3 (U;Z) is zero otherwise. Here Z[Sp] is the
group freely generated by the p(p + 1) points in Sp and Z[Sp]0 is the kernel
of the argumentation map.
To read the Ei;j
2 -terms we observe that the cohomology of Ap has a Z-algebra
structure:
H (Ap;Z) =
Z[x1; x2; y]
(y2; px1; px2; py)
;
where deg(x1) = deg(x2) = 2 and deg(y) = 3. Indeed the Z-algebra structure
comes from the Bockstein operator for H (Z=pZ; Fp). (The reader may
331. nd a
detailed proof in Appendix A of [7].)
For what concerns this proof, we only care about the terms Ei;j
2 with
j 2p 3. The dierential di;j
2 is zero if j 2p 3.
17