Deformations of Bimodule Problems
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On Classification Problem of Loday Algebras 227
Contemporary Mathematics Volume 672, 2016 http://dx.doi.org/10.1090/conm/672/13471 On classification problem of Loday algebras I. S. Rakhimov Abstract. This is a survey paper on classification problems of some classes of algebras introduced by Loday around 1990s. In the paper the author intends to review the latest results on classification problem of Loday algebras, achieve- ments have been made up to date, approaches and methods implemented. 1. Introduction It is well known that any associative algebra gives rise to a Lie algebra, with bracket [x, y]:=xy − yx. In 1990s J.-L. Loday introduced a non-antisymmetric version of Lie algebras, whose bracket satisfies the Leibniz identity [[x, y],z]=[[x, z],y]+[x, [y, z]] and therefore they have been called Leibniz algebras. The Leibniz identity combined with antisymmetry, is a variation of the Jacobi identity, hence Lie algebras are antisymmetric Leibniz algebras. The Leibniz algebras are characterized by the property that the multiplication (called a bracket) from the right is a derivation but the bracket no longer is skew-symmetric as for Lie algebras. Further Loday looked for a counterpart of the associative algebras for the Leibniz algebras. The idea is to start with two distinct operations for the products xy, yx, and to consider a vector space D (called an associative dialgebra) endowed by two binary multiplications and satisfying certain “associativity conditions”. The conditions provide the relation mentioned above replacing the Lie algebra and the associative algebra by the Leibniz algebra and the associative dialgebra, respectively. Thus, if (D, , ) is an associative dialgebra, then (D, [x, y]=x y − y x) is a Leibniz algebra. -
Change of Rings Theorems
CHANG E OF RINGS THEOREMS CHANGE OF RINGS THEOREMS By PHILIP MURRAY ROBINSON, B.SC. A Thesis Submitted to the School of Graduate Studies in Partial Fulfilment of the Requirements for the Degree Master of Science McMaster University (July) 1971 MASTER OF SCIENCE (1971) l'v1cHASTER UNIVERSITY {Mathematics) Hamilton, Ontario TITLE: Change of Rings Theorems AUTHOR: Philip Murray Robinson, B.Sc. (Carleton University) SUPERVISOR: Professor B.J.Mueller NUMBER OF PAGES: v, 38 SCOPE AND CONTENTS: The intention of this thesis is to gather together the results of various papers concerning the three change of rings theorems, generalizing them where possible, and to determine if the various results, although under different hypotheses, are in fact, distinct. {ii) PREFACE Classically, there exist three theorems which relate the two homological dimensions of a module over two rings. We deal with the first and last of these theorems. J. R. Strecker and L. W. Small have significantly generalized the "Third Change of Rings Theorem" and we have simply re organized their results as Chapter 2. J. M. Cohen and C. u. Jensen have generalized the "First Change of Rings Theorem", each with hypotheses seemingly distinct from the other. However, as Chapter 3 we show that by developing new proofs for their theorems we can, indeed, generalize their results and by so doing show that their hypotheses coincide. Some examples due to Small and Cohen make up Chapter 4 as a completion to the work. (iii) ACKNOW-EDGMENTS The author expresses his sincere appreciation to his supervisor, Dr. B. J. Mueller, whose guidance and helpful criticisms were of greatest value in the preparation of this thesis. -
QUIVER BIALGEBRAS and MONOIDAL CATEGORIES 3 K N ≥ 0
QUIVER BIALGEBRAS AND MONOIDAL CATEGORIES HUA-LIN HUANG (JINAN) AND BLAS TORRECILLAS (ALMER´IA) Abstract. We study the bialgebra structures on quiver coalgebras and the monoidal structures on the categories of locally nilpotent and locally finite quiver representations. It is shown that the path coalgebra of an arbitrary quiver admits natural bialgebra structures. This endows the category of locally nilpotent and locally finite representations of an arbitrary quiver with natural monoidal structures from bialgebras. We also obtain theorems of Gabriel type for pointed bialgebras and hereditary finite pointed monoidal categories. 1. Introduction This paper is devoted to the study of natural bialgebra structures on the path coalgebra of an arbitrary quiver and monoidal structures on the category of its locally nilpotent and locally finite representations. A further purpose is to establish a quiver setting for general pointed bialgebras and pointed monoidal categories. Our original motivation is to extend the Hopf quiver theory [4, 7, 8, 12, 13, 25, 31] to the setting of generalized Hopf structures. As bialgebras are a fundamental generalization of Hopf algebras, we naturally initiate our study from this case. The basic problem is to determine what kind of quivers can give rise to bialgebra structures on their associated path algebras or coalgebras. It turns out that the path coalgebra of an arbitrary quiver admits natural bial- gebra structures, see Theorem 3.2. This seems a bit surprising at first sight by comparison with the Hopf case given in [8], where Cibils and Rosso showed that the path coalgebra of a quiver Q admits a Hopf algebra structure if and only if Q is a Hopf quiver which is very special. -
Right Ideals of a Ring and Sublanguages of Science
RIGHT IDEALS OF A RING AND SUBLANGUAGES OF SCIENCE Javier Arias Navarro Ph.D. In General Linguistics and Spanish Language http://www.javierarias.info/ Abstract Among Zellig Harris’s numerous contributions to linguistics his theory of the sublanguages of science probably ranks among the most underrated. However, not only has this theory led to some exhaustive and meaningful applications in the study of the grammar of immunology language and its changes over time, but it also illustrates the nature of mathematical relations between chunks or subsets of a grammar and the language as a whole. This becomes most clear when dealing with the connection between metalanguage and language, as well as when reflecting on operators. This paper tries to justify the claim that the sublanguages of science stand in a particular algebraic relation to the rest of the language they are embedded in, namely, that of right ideals in a ring. Keywords: Zellig Sabbetai Harris, Information Structure of Language, Sublanguages of Science, Ideal Numbers, Ernst Kummer, Ideals, Richard Dedekind, Ring Theory, Right Ideals, Emmy Noether, Order Theory, Marshall Harvey Stone. §1. Preliminary Word In recent work (Arias 2015)1 a line of research has been outlined in which the basic tenets underpinning the algebraic treatment of language are explored. The claim was there made that the concept of ideal in a ring could account for the structure of so- called sublanguages of science in a very precise way. The present text is based on that work, by exploring in some detail the consequences of such statement. §2. Introduction Zellig Harris (1909-1992) contributions to the field of linguistics were manifold and in many respects of utmost significance. -
Rigidity of Some Classes of Lie Algebras in Connection to Leibniz
Rigidity of some classes of Lie algebras in connection to Leibniz algebras Abdulafeez O. Abdulkareem1, Isamiddin S. Rakhimov2, and Sharifah K. Said Husain3 1,3Department of Mathematics, Faculty of Science, Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia. 1,2,3Laboratory of Cryptography,Analysis and Structure, Institute for Mathematical Research (INSPEM), Universiti Putra Malaysia, 43400 UPM Serdang, Selangor Darul Ehsan, Malaysia. Abstract In this paper we focus on algebraic aspects of contractions of Lie and Leibniz algebras. The rigidity of algebras plays an important role in the study of their varieties. The rigid algebras generate the irreducible components of this variety. We deal with Leibniz algebras which are generalizations of Lie algebras. In Lie algebras case, there are different kind of rigidities (rigidity, absolutely rigidity, geometric rigidity and e.c.t.). We explore the relations of these rigidities with Leibniz algebra rigidity. Necessary conditions for a Lie algebra to be Leibniz rigid are discussed. Keywords: Rigid algebras, Contraction and Degeneration, Degeneration invariants, Zariski closure. 1 Introduction In 1951, Segal I.E. [11] introduced the notion of contractions of Lie algebras on physical grounds: if two physical theories (like relativistic and classical mechanics) are related by a limiting process, then the associated invariance groups (like the Poincar´eand Galilean groups) should also be related by some limiting process. If the velocity of light is assumed to go to infinity, relativistic mechanics ”transforms” into classical mechanics. This also induces a singular transition from the Poincar´ealgebra to the Galilean one. Another ex- ample is a limiting process from quantum mechanics to classical mechanics under ~ → 0, arXiv:1708.00330v1 [math.RA] 30 Jul 2017 that corresponds to the contraction of the Heisenberg algebras to the abelian ones of the same dimensions [2]. -
For a = Zg(O). (Iii) the Morphism (100) Is Autk-Equivariant. We
HITCHIN’S INTEGRABLE SYSTEM 101 (ii) The composition zg(K) → Z → zg(O) is the morphism (97) for A = zg(O). (iii) The morphism (100) is Aut K-equivariant. We will not prove this theorem. In fact, the only nontrivial statement is that (99) (or equivalently (34)) is a ring homomorphism; see ???for a proof. The natural approach to the above theorem is based on the notion of VOA (i.e., vertex operator algebra) or its geometric version introduced in [BD] under the name of chiral algebra.21 In the next subsection (which can be skipped by the reader) we outline the chiral algebra approach. 3.7.6. A chiral algebra on a smooth curve X is a (left) DX -module A equipped with a morphism ! (101) j∗j (A A) → ∆∗A where ∆ : X→ X × X is the diagonal, j :(X × X) \ ∆(X) → X. The morphism (101) should satisfy certain axioms, which will not be stated here. A chiral algebra is said to be commutative if (101) maps A A to 0. Then (101) induces a morphism ∆∗(A⊗A)=j∗j!(A A)/A A→∆∗A or, which is the same, a morphism (102) A⊗A→A. In this case the chiral algebra axioms just mean that A equipped with the operation (102) is a commutative associative unital algebra. So a commutative chiral algebra is the same as a commutative associative unital D D X -algebra in the sense of 2.6. On the other hand, the X -module VacX corresponding to the Aut O-module Vac by 2.6.5 has a natural structure of → chiral algebra (see the Remark below). -
A Computable Functor from Graphs to Fields
A COMPUTABLE FUNCTOR FROM GRAPHS TO FIELDS The MIT Faculty has made this article openly available. Please share how this access benefits you. Your story matters. Citation MILLER, RUSSELL et al. “A COMPUTABLE FUNCTOR FROM GRAPHS TO FIELDS.” The Journal of Symbolic Logic 83, 1 (March 2018): 326–348 © 2018 The Association for Symbolic Logic As Published http://dx.doi.org/10.1017/jsl.2017.50 Publisher Cambridge University Press (CUP) Version Original manuscript Citable link http://hdl.handle.net/1721.1/116051 Terms of Use Creative Commons Attribution-Noncommercial-Share Alike Detailed Terms http://creativecommons.org/licenses/by-nc-sa/4.0/ A COMPUTABLE FUNCTOR FROM GRAPHS TO FIELDS RUSSELL MILLER, BJORN POONEN, HANS SCHOUTENS, AND ALEXANDRA SHLAPENTOKH Abstract. We construct a fully faithful functor from the category of graphs to the category of fields. Using this functor, we resolve a longstanding open problem in computable model theory, by showing that for every nontrivial countable structure , there exists a countable field with the same essential computable-model-theoretic propeSrties as . Along the way, we developF a new “computable category theory”, and prove that our functorS and its partially- defined inverse (restricted to the categories of countable graphs and countable fields) are computable functors. 1. Introduction 1.A. A functor from graphs to fields. Let Graphs be the category of symmetric irreflex- ive graphs in which morphisms are isomorphisms onto induced subgraphs (see Section 2.A). Let Fields be the category of fields, with field homomorphisms as the morphisms. Using arithmetic geometry, we will prove the following: Theorem 1.1. -
Voevodsky's Univalent Foundation of Mathematics
Voevodsky's Univalent Foundation of Mathematics Thierry Coquand Bonn, May 15, 2018 Voevodsky's Univalent Foundation of Mathematics Univalent Foundations Voevodsky's program to express mathematics in type theory instead of set theory 1 Voevodsky's Univalent Foundation of Mathematics Univalent Foundations Voevodsky \had a special talent for bringing techniques from homotopy theory to bear on concrete problems in other fields” 1996: proof of the Milnor Conjecture 2011: proof of the Bloch-Kato conjecture He founded the field of motivic homotopy theory In memoriam: Vladimir Voevodsky (1966-2017) Dan Grayson (BSL, to appear) 2 Voevodsky's Univalent Foundation of Mathematics Univalent Foundations What does \univalent" mean? Russian word used as a translation of \faithful" \These foundations seem to be faithful to the way in which I think about mathematical objects in my head" (from a Talk at IHP, Paris 2014) 3 Voevodsky's Univalent Foundation of Mathematics Univalent foundations Started in 2002 to look into formalization of mathematics Notes on homotopy λ-calculus, March 2006 Notes for a talk at Standford (available at V. Voevodsky github repository) 4 Voevodsky's Univalent Foundation of Mathematics Univalent Foundations hh nowadays it is known to be possible, logically speaking, to derive practically the whole of known mathematics from a single source, the Theory of Sets ::: By so doing we do not claim to legislate for all time. It may happen at some future date that mathematicians will agree to use modes of reasoning which cannot be formalized in the language described here; according to some, the recent evolutation of axiomatic homology theory would be a sign that this date is not so far. -
Arxiv:1611.02437V2 [Math.CT] 2 Jan 2017 Betseiso Structures
UNIFIED FUNCTORIAL SIGNAL REPRESENTATION II: CATEGORY ACTION, BASE HIERARCHY, GEOMETRIES AS BASE STRUCTURED CATEGORIES SALIL SAMANT AND SHIV DUTT JOSHI Abstract. In this paper we propose and study few applications of the base ⋊ ¯ ⋊ F¯ structured categories X F C, RC F, X F C and RC . First we show classic ¯ transformation groupoid X//G simply being a base-structured category RG F . Then using permutation action on a finite set, we introduce the notion of a hierarchy of ⋊ ⋊ ⋊ base structured categories [(X2a F2a B2a) ∐ (X2b F2b B2b) ∐ ...] F1 B1 that models local and global structures as a special case of composite Grothendieck fibration. Further utilizing the existing notion of transformation double category (X1 ⋊F1 B1)//2G, we demonstrate that a hierarchy of bases naturally leads one from 2-groups to n-category theory. Finally we prove that every classic Klein geometry F ∞ U is the Grothendieck completion (G = X ⋊F H) of F : H −→ Man −→ Set. This is generalized to propose a set-theoretic definition of a groupoid geometry (G, B) (originally conceived by Ehresmann through transport and later by Leyton using transfer) with a principal groupoid G = X ⋊ B and geometry space X = G/B; F which is essentially same as G = X ⋊F B or precisely the completion of F : B −→ ∞ U Man −→ Set. 1. Introduction The notion of base structured categories characterizing a functor were introduced in the preceding part [26] of the sequel. Here the perspective of a functor as an action of a category is considered by using the elementary structure of symmetry on objects especially the permutation action on a finite set. -
Bimodule Categories and Monoidal 2-Structure Justin Greenough University of New Hampshire, Durham
University of New Hampshire University of New Hampshire Scholars' Repository Doctoral Dissertations Student Scholarship Fall 2010 Bimodule categories and monoidal 2-structure Justin Greenough University of New Hampshire, Durham Follow this and additional works at: https://scholars.unh.edu/dissertation Recommended Citation Greenough, Justin, "Bimodule categories and monoidal 2-structure" (2010). Doctoral Dissertations. 532. https://scholars.unh.edu/dissertation/532 This Dissertation is brought to you for free and open access by the Student Scholarship at University of New Hampshire Scholars' Repository. It has been accepted for inclusion in Doctoral Dissertations by an authorized administrator of University of New Hampshire Scholars' Repository. For more information, please contact [email protected]. BIMODULE CATEGORIES AND MONOIDAL 2-STRUCTURE BY JUSTIN GREENOUGH B.S., University of Alaska, Anchorage, 2003 M.S., University of New Hampshire, 2008 DISSERTATION Submitted to the University of New Hampshire in Partial Fulfillment of the Requirements for the Degree of Doctor of Philosophy in Mathematics September, 2010 UMI Number: 3430786 All rights reserved INFORMATION TO ALL USERS The quality of this reproduction is dependent upon the quality of the copy submitted. In the unlikely event that the author did not send a complete manuscript and there are missing pages, these will be noted. Also, if material had to be removed, a note will indicate the deletion. UMT Dissertation Publishing UMI 3430786 Copyright 2010 by ProQuest LLC. All rights reserved. This edition of the work is protected against unauthorized copying under Title 17, United States Code. ProQuest LLC 789 East Eisenhower Parkway P.O. Box 1346 Ann Arbor, Ml 48106-1346 This thesis has been examined and approved. -
Ringel-Hall Algebras Andrew W. Hubery
Ringel-Hall Algebras Andrew W. Hubery 1. INTRODUCTION 3 1. Introduction Two of the first results learned in a linear algebra course concern finding normal forms for linear maps between vector spaces. We may consider a linear map f : V → W between vector spaces over some field k. There exist isomorphisms V =∼ Ker(f) ⊕ Im(f) and W =∼ Im(f) ⊕ Coker(f), and with respect to these decompositions f = id ⊕ 0. If we consider a linear map f : V → V with V finite dimensional, then we can express f as a direct sum of Jordan blocks, and each Jordan block is determined by a monic irreducible polynomial in k[T ] together with a positive integer. We can generalise such problems to arbitrary configurations of vector spaces and linear maps. For example f g f g U1 −→ V ←− U2 or U −→ V −→ W. We represent such problems diagrammatically by drawing a dot for each vector space and an arrow for each linear map. So, the four problems listed above corre- spond to the four diagrams A: B : C : D : Such a diagram is called a quiver, and a configuration of vector spaces and linear maps is called a representation of the quiver: that is, we take a vector space for each vertex and a linear map for each arrow. Given two representations of the same quiver, we define the direct sum to be the representation produced by taking the direct sums of the vector spaces and the linear maps for each vertex and each arrow. Recall that if f : U → V and f 0 : U 0 → V 0 are linear maps, then the direct sum is the linear map f ⊕ f 0 : U ⊕ U 0 → V ⊕ V 0, (u,u0) 7→ (f(u), f 0(u0)). -
Basic Representation Theory [ Draft ]
Basic representation theory [ draft ] Incomplete notes for a mini-course given at UCAS, Summer 2017 Wen-Wei Li Version: December 10, 2018 Contents 1 Topological groups 2 1.1 Definition of topological groups .............................. 2 1.2 Local fields ......................................... 4 1.3 Measures and integrals ................................... 5 1.4 Haar measures ........................................ 6 1.5 The modulus character ................................... 9 1.6 Interlude on analytic manifolds ............................... 11 1.7 More examples ....................................... 13 1.8 Homogeneous spaces .................................... 14 2 Convolution 17 2.1 Convolution of functions .................................. 17 2.2 Convolution of measures .................................. 19 3 Continuous representations 20 3.1 General representations ................................... 20 3.2 Matrix coefficients ..................................... 23 3.3 Vector-valued integrals ................................... 25 3.4 Action of convolution algebra ................................ 26 3.5 Smooth vectors: archimedean case ............................. 28 4 Unitary representation theory 28 4.1 Generalities ......................................... 29 4.2 External tensor products .................................. 32 4.3 Square-integrable representations .............................. 33 4.4 Spectral decomposition: the discrete part .......................... 37 4.5 Usage of compact operators ................................