Equivariant Stable Homotopy Theory
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Symmetry Preserving Interpolation Erick Rodriguez Bazan, Evelyne Hubert
Symmetry Preserving Interpolation Erick Rodriguez Bazan, Evelyne Hubert To cite this version: Erick Rodriguez Bazan, Evelyne Hubert. Symmetry Preserving Interpolation. ISSAC 2019 - International Symposium on Symbolic and Algebraic Computation, Jul 2019, Beijing, China. 10.1145/3326229.3326247. hal-01994016 HAL Id: hal-01994016 https://hal.archives-ouvertes.fr/hal-01994016 Submitted on 25 Jan 2019 HAL is a multi-disciplinary open access L’archive ouverte pluridisciplinaire HAL, est archive for the deposit and dissemination of sci- destinée au dépôt et à la diffusion de documents entific research documents, whether they are pub- scientifiques de niveau recherche, publiés ou non, lished or not. The documents may come from émanant des établissements d’enseignement et de teaching and research institutions in France or recherche français ou étrangers, des laboratoires abroad, or from public or private research centers. publics ou privés. Symmetry Preserving Interpolation Erick Rodriguez Bazan Evelyne Hubert Université Côte d’Azur, France Université Côte d’Azur, France Inria Méditerranée, France Inria Méditerranée, France [email protected] [email protected] ABSTRACT general concept. An interpolation space for a set of linear forms is The article addresses multivariate interpolation in the presence of a subspace of the polynomial ring that has a unique interpolant for symmetry. Interpolation is a prime tool in algebraic computation each instantiated interpolation problem. We show that the unique while symmetry is a qualitative feature that can be more relevant interpolants automatically inherit the symmetry of the problem to a mathematical model than the numerical accuracy of the pa- when the interpolation space is invariant (Section 3). -
The Adams-Novikov Spectral Sequence for the Spheres
BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 77, Number 1, January 1971 THE ADAMS-NOVIKOV SPECTRAL SEQUENCE FOR THE SPHERES BY RAPHAEL ZAHLER1 Communicated by P. E. Thomas, June 17, 1970 The Adams spectral sequence has been an important tool in re search on the stable homotopy of the spheres. In this note we outline new information about a variant of the Adams sequence which was introduced by Novikov [7]. We develop simplified techniques of computation which allow us to discover vanishing lines and periodic ity near the edge of the E2-term, interesting elements in E^'*, and a counterexample to one of Novikov's conjectures. In this way we obtain independently the values of many low-dimensional stems up to group extension. The new methods stem from a deeper under standing of the Brown-Peterson cohomology theory, due largely to Quillen [8]; see also [4]. Details will appear elsewhere; or see [ll]. When p is odd, the p-primary part of the Novikov sequence be haves nicely in comparison with the ordinary Adams sequence. Com puting the £2-term seems to be as easy, and the Novikov sequence has many fewer nonzero differentials (in stems ^45, at least, if p = 3), and periodicity near the edge. The case p = 2 is sharply different. Computing E2 is more difficult. There are also hordes of nonzero dif ferentials dz, but they form a regular pattern, and no nonzero differ entials outside the pattern have been found. Thus the diagram of £4 ( =£oo in dimensions ^17) suggests a vanishing line for Ew much lower than that of £2 of the classical Adams spectral sequence [3]. -
Sheaves and Homotopy Theory
SHEAVES AND HOMOTOPY THEORY DANIEL DUGGER The purpose of this note is to describe the homotopy-theoretic version of sheaf theory developed in the work of Thomason [14] and Jardine [7, 8, 9]; a few enhancements are provided here and there, but the bulk of the material should be credited to them. Their work is the foundation from which Morel and Voevodsky build their homotopy theory for schemes [12], and it is our hope that this exposition will be useful to those striving to understand that material. Our motivating examples will center on these applications to algebraic geometry. Some history: The machinery in question was invented by Thomason as the main tool in his proof of the Lichtenbaum-Quillen conjecture for Bott-periodic algebraic K-theory. He termed his constructions `hypercohomology spectra', and a detailed examination of their basic properties can be found in the first section of [14]. Jardine later showed how these ideas can be elegantly rephrased in terms of model categories (cf. [8], [9]). In this setting the hypercohomology construction is just a certain fibrant replacement functor. His papers convincingly demonstrate how many questions concerning algebraic K-theory or ´etale homotopy theory can be most naturally understood using the model category language. In this paper we set ourselves the specific task of developing some kind of homotopy theory for schemes. The hope is to demonstrate how Thomason's and Jardine's machinery can be built, step-by-step, so that it is precisely what is needed to solve the problems we encounter. The papers mentioned above all assume a familiarity with Grothendieck topologies and sheaf theory, and proceed to develop the homotopy-theoretic situation as a generalization of the classical case. -
Poincar\'E Duality for $ K $-Theory of Equivariant Complex Projective
POINCARE´ DUALITY FOR K-THEORY OF EQUIVARIANT COMPLEX PROJECTIVE SPACES J.P.C. GREENLEES AND G.R. WILLIAMS Abstract. We make explicit Poincar´eduality for the equivariant K-theory of equivariant complex projective spaces. The case of the trivial group provides a new approach to the K-theory orientation [3]. 1. Introduction In 1 well behaved cases one expects the cohomology of a finite com- plex to be a contravariant functor of its homology. However, orientable manifolds have the special property that the cohomology is covariantly isomorphic to the homology, and hence in particular the cohomology ring is self-dual. More precisely, Poincar´eduality states that taking the cap product with a fundamental class gives an isomorphism between homology and cohomology of a manifold. Classically, an n-manifold M is a topological space locally modelled n on R , and the fundamental class of M is a homology class in Hn(M). Equivariantly, it is much less clear how things should work. If we pick a point x of a smooth G-manifold, the tangent space Vx is a represen- tation of the isotropy group Gx, and its G-orbit is locally modelled on G ×Gx Vx; both Gx and Vx depend on the point x. It may happen that we have a W -manifold, in the sense that there is a single representation arXiv:0711.0346v1 [math.AT] 2 Nov 2007 W so that Vx is the restriction of W to Gx for all x, but this is very restrictive. Even if there are fixed points x, the representations Vx at different points need not be equivalent. -
Equivariant and Isovariant Function Spaces
UC Riverside UC Riverside Electronic Theses and Dissertations Title Equivariant and Isovariant Function Spaces Permalink https://escholarship.org/uc/item/7fk0p69b Author Safii, Soheil Publication Date 2015 Peer reviewed|Thesis/dissertation eScholarship.org Powered by the California Digital Library University of California UNIVERSITY OF CALIFORNIA RIVERSIDE Equivariant and Isovariant Function Spaces A Dissertation submitted in partial satisfaction of the requirements for the degree of Doctor of Philosophy in Mathematics by Soheil Safii March 2015 Dissertation Committee: Professor Reinhard Schultz, Chairperson Professor Julia Bergner Professor Fred Wilhelm Copyright by Soheil Safii 2015 The Dissertation of Soheil Safii is approved: Committee Chairperson University of California, Riverside Acknowledgments I would like to thank Professor Reinhard Schultz for all of the time and effort he put into being a wonderful advisor. Without his expansive knowledge and unending patience, none of our work would be possible. Having the opportunity to work with him has been a privilege. I would like to acknowledge Professor Julia Bergner and Professor Fred Wilhelm for their insight and valuable feedback. I am grateful for the unconditional support of my classmates: Mathew Lunde, Jason Park, and Jacob West. I would also like to thank my students, who inspired me and taught me more than I could have ever hoped to teach them. Most of all, I am appreciative of my friends and family, with whom I have been blessed. iv To my parents. v ABSTRACT OF THE DISSERTATION Equivariant and Isovariant Function Spaces by Soheil Safii Doctor of Philosophy, Graduate Program in Mathematics University of California, Riverside, March 2015 Professor Reinhard Schultz, Chairperson The Browder{Straus Theorem, obtained independently by S. -
Floer Homology, Gauge Theory, and Low-Dimensional Topology
Floer Homology, Gauge Theory, and Low-Dimensional Topology Clay Mathematics Proceedings Volume 5 Floer Homology, Gauge Theory, and Low-Dimensional Topology Proceedings of the Clay Mathematics Institute 2004 Summer School Alfréd Rényi Institute of Mathematics Budapest, Hungary June 5–26, 2004 David A. Ellwood Peter S. Ozsváth András I. Stipsicz Zoltán Szabó Editors American Mathematical Society Clay Mathematics Institute 2000 Mathematics Subject Classification. Primary 57R17, 57R55, 57R57, 57R58, 53D05, 53D40, 57M27, 14J26. The cover illustrates a Kinoshita-Terasaka knot (a knot with trivial Alexander polyno- mial), and two Kauffman states. These states represent the two generators of the Heegaard Floer homology of the knot in its topmost filtration level. The fact that these elements are homologically non-trivial can be used to show that the Seifert genus of this knot is two, a result first proved by David Gabai. Library of Congress Cataloging-in-Publication Data Clay Mathematics Institute. Summer School (2004 : Budapest, Hungary) Floer homology, gauge theory, and low-dimensional topology : proceedings of the Clay Mathe- matics Institute 2004 Summer School, Alfr´ed R´enyi Institute of Mathematics, Budapest, Hungary, June 5–26, 2004 / David A. Ellwood ...[et al.], editors. p. cm. — (Clay mathematics proceedings, ISSN 1534-6455 ; v. 5) ISBN 0-8218-3845-8 (alk. paper) 1. Low-dimensional topology—Congresses. 2. Symplectic geometry—Congresses. 3. Homol- ogy theory—Congresses. 4. Gauge fields (Physics)—Congresses. I. Ellwood, D. (David), 1966– II. Title. III. Series. QA612.14.C55 2004 514.22—dc22 2006042815 Copying and reprinting. Material in this book may be reproduced by any means for educa- tional and scientific purposes without fee or permission with the exception of reproduction by ser- vices that collect fees for delivery of documents and provided that the customary acknowledgment of the source is given. -
Definition 1.1. a Group Is a Quadruple (G, E, ⋆, Ι)
GROUPS AND GROUP ACTIONS. 1. GROUPS We begin by giving a definition of a group: Definition 1.1. A group is a quadruple (G, e, ?, ι) consisting of a set G, an element e G, a binary operation ?: G G G and a map ι: G G such that ∈ × → → (1) The operation ? is associative: (g ? h) ? k = g ? (h ? k), (2) e ? g = g ? e = g, for all g G. ∈ (3) For every g G we have g ? ι(g) = ι(g) ? g = e. ∈ It is standard to suppress the operation ? and write gh or at most g.h for g ? h. The element e is known as the identity element. For clarity, we may also write eG instead of e to emphasize which group we are considering, but may also write 1 for e where this is more conventional (for the group such as C∗ for example). Finally, 1 ι(g) is usually written as g− . Remark 1.2. Let us note a couple of things about the above definition. Firstly clo- sure is not an axiom for a group whatever anyone has ever told you1. (The reason people get confused about this is related to the notion of subgroups – see Example 1.8 later in this section.) The axioms used here are not “minimal”: the exercises give a different set of axioms which assume only the existence of a map ι without specifying it. We leave it to those who like that kind of thing to check that associa- tivity of triple multiplications implies that for any k N, bracketing a k-tuple of ∈ group elements (g1, g2, . -
On the Product in Negative Tate Cohomology for Finite Groups 2
ON THE PRODUCT IN NEGATIVE TATE COHOMOLOGY FOR FINITE GROUPS HAGGAI TENE Abstract. Our aim in this paper is to give a geometric description of the cup product in negative degrees of Tate cohomology of a finite group with integral coefficients. By duality it corresponds to a product in the integral homology of BG: Hn(BG, Z) ⊗ Hm(BG, Z) → Hn+m+1(BG, Z) for n,m > 0. We describe this product as join of cycles, which explains the shift in dimensions. Our motivation came from the product defined by Kreck using stratifold homology. We then prove that for finite groups the cup product in negative Tate cohomology and the Kreck product coincide. The Kreck product also applies to the case where G is a compact Lie group (with an additional dimension shift). Introduction For a finite group G one defines Tate cohomology with coefficients in a Z[G] module M, denoted by H∗(G, M). This is a multiplicative theory: b Hn(G, M) ⊗ Hm(G, M ′) → Hn+m(G, M ⊗ M ′) b b b and the product is called cup product. For n > 0 there is a natural isomor- phism Hn(G, M) → Hn(G, M), and for n < −1 there is a natural isomorphism b Hn(G, M) → H (G, M). We restrict ourselves to coefficients in the triv- b −n−1 ial module Z. In this case, H∗(G, Z) is a graded ring. Also, in this case the b group cohomology and homology are actually the cohomology and homology of a topological space, namely BG, the classifying space of principal G bundles - n n arXiv:0911.3014v2 [math.AT] 27 Jul 2011 H (G, Z) =∼ H (BG, Z) and Hn(G, Z) =∼ Hn(BG, Z). -
Introduction to Equivariant Cohomology Theory 11
INTRODUCTION TO EQUIVARIANT COHOMOLOGY THEORY YOUNG-HOON KIEM 1. Definitions and Basic Properties 1.1. Lie group. Let G be a Lie group (i.e. a manifold equipped with di®erentiable group operations mult : G £ G ! G, inv : G ! G, id 2 G satisfying the usual group axioms). We shall be concerned only with linear groups (i.e. a subgroup of GL(n) = GL(n; C) for some n) such as the unitary group U(n), the special unitary group SU(n). A connected compact Lie group G is called a torus if it is abelian. Explicitly, they are products U(1)n of the circle group U(1) = feiθ j θ 2 Rg = S1. Since a complex linear (reductive) group is homotopy equivalent1 to its maximal compact subgroup, it su±ces to consider only compact groups. For instance, the equivariant cohomology for SL(n) (GL(n), C¤, resp.) is the same as the equivariant cohomology for SU(n) (U(n), S1, resp.). 1.2. Classifying space. Suppose a compact Lie group G acts on a topological space X continuously. We say the group action is free if the stabilizer group Gx = fg 2 G j gx = xg of every point x 2 X is the trivial subgroup. A topological space X is called contractible if there is a homotopy equivalence with a point (i.e. 9h : X £ [0; 1] ! X such that h(x; 0) = x0, h(x; 1) = x for x 2 X). Theorem 1. For each compact Lie group G, there exists a contractible topological space EG on which G acts freely. -
The Formalism of Segal Sections
THE FORMALISM OF SEGAL SECTIONS BY Edouard Balzin ABSTRACT Given a family of model categories E ! C, we associate to it a homo- topical category of derived, or Segal, sections DSect(C; E) that models the higher-categorical sections of the localisation LE ! C. The derived sections provide an alternative, strict model for various higher algebra ob- jects appearing in the work of Lurie. We prove a few results concerning the properties of the homotopical category DSect(C; E), and as an exam- ple, study its behaviour with respect to the base-change along a select class of functors. Contents Introduction . 2 1. Simplicial Replacements . 10 1.1. Preliminaries . 10 1.2. The replacements . 12 1.3. Families over the simplicial replacement . 15 2. Derived, or Segal, sections . 20 2.1. Presections . 20 2.2. Homotopical category of Segal sections . 23 3. Higher-categorical aspects . 27 3.1. Behaviour with respect to the infinity-localisation . 27 3.2. Higher-categorical Segal sections . 32 4. Resolutions . 40 4.1. Relative comma objects . 44 4.2. Sections over relative comma objects . 49 4.3. Comparing the Segal sections . 52 References . 58 2 EDOUARD BALZIN Introduction Segal objects. The formalism presented in this paper was developed in the study of homotopy algebraic structures as described by Segal and generalised by Lurie. We begin the introduction by describing this context. Denote by Γ the category whose objects are finite sets and morphisms are given by partially defined set maps. Each such morphism between S and T can be depicted as S ⊃ S0 ! T .A Γ-space is simply a functor X :Γ ! Top taking values in the category of topological spaces. -
Lecture Notes on Simplicial Homotopy Theory
Lectures on Homotopy Theory The links below are to pdf files, which comprise my lecture notes for a first course on Homotopy Theory. I last gave this course at the University of Western Ontario during the Winter term of 2018. The course material is widely applicable, in fields including Topology, Geometry, Number Theory, Mathematical Pysics, and some forms of data analysis. This collection of files is the basic source material for the course, and this page is an outline of the course contents. In practice, some of this is elective - I usually don't get much beyond proving the Hurewicz Theorem in classroom lectures. Also, despite the titles, each of the files covers much more material than one can usually present in a single lecture. More detail on topics covered here can be found in the Goerss-Jardine book Simplicial Homotopy Theory, which appears in the References. It would be quite helpful for a student to have a background in basic Algebraic Topology and/or Homological Algebra prior to working through this course. J.F. Jardine Office: Middlesex College 118 Phone: 519-661-2111 x86512 E-mail: [email protected] Homotopy theories Lecture 01: Homological algebra Section 1: Chain complexes Section 2: Ordinary chain complexes Section 3: Closed model categories Lecture 02: Spaces Section 4: Spaces and homotopy groups Section 5: Serre fibrations and a model structure for spaces Lecture 03: Homotopical algebra Section 6: Example: Chain homotopy Section 7: Homotopical algebra Section 8: The homotopy category Lecture 04: Simplicial sets Section 9: -
Infinite Loop Space Theory
BULLETIN OF THE AMERICAN MATHEMATICAL SOCIETY Volume 83, Number 4, July 1977 INFINITE LOOP SPACE THEORY BY J. P. MAY1 Introduction. The notion of a generalized cohomology theory plays a central role in algebraic topology. Each such additive theory E* can be represented by a spectrum E. Here E consists of based spaces £, for / > 0 such that Ei is homeomorphic to the loop space tiEi+l of based maps l n S -» Ei+,, and representability means that E X = [X, En], the Abelian group of homotopy classes of based maps X -* En, for n > 0. The existence of the E{ for i > 0 implies the presence of considerable internal structure on E0, the least of which is a structure of homotopy commutative //-space. Infinite loop space theory is concerned with the study of such internal structure on spaces. This structure is of interest for several reasons. The homology of spaces so structured carries "homology operations" analogous to the Steenrod opera tions in the cohomology of general spaces. These operations are vital to the analysis of characteristic classes for spherical fibrations and for topological and PL bundles. More deeply, a space so structured determines a spectrum and thus a cohomology theory. In the applications, there is considerable interplay between descriptive analysis of the resulting new spectra and explicit calculations of homology groups. The discussion so far concerns spaces with one structure. In practice, many of the most interesting applications depend on analysis of the interrelation ship between two such structures on a space, one thought of as additive and the other as multiplicative.