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(Pro-) Étale Cohomology 3. Exercise Sheet
(Pro-) Étale Cohomology 3. Exercise Sheet Department of Mathematics Winter Semester 18/19 Prof. Dr. Torsten Wedhorn 2nd November 2018 Timo Henkel Homework Exercise H9 (Clopen subschemes) (12 points) Let X be a scheme. We define Clopen(X ) := Z X Z open and closed subscheme of X . f ⊆ j g Recall that Clopen(X ) is in bijection to the set of idempotent elements of X (X ). Let X S be a morphism of schemes. We consider the functor FX =S fromO the category of S-schemes to the category of sets, given! by FX =S(T S) = Clopen(X S T). ! × Now assume that X S is a finite locally free morphism of schemes. Show that FX =S is representable by an affine étale S-scheme which is of! finite presentation over S. Exercise H10 (Lifting criteria) (12 points) Let f : X S be a morphism of schemes which is locally of finite presentation. Consider the following diagram of S-schemes:! T0 / X (1) f T / S Let be a class of morphisms of S-schemes. We say that satisfies the 1-lifting property (resp. !-lifting property) ≤ withC respect to f , if for all morphisms T0 T in andC for all diagrams9 of the form (1) there exists9 at most (resp. exactly) one morphism of S-schemes T X!which makesC the diagram commutative. Let ! 1 := f : T0 T closed immersion of S-schemes f is given by a locally nilpotent ideal C f ! j g 2 := f : T0 T closed immersion of S-schemes T is affine and T0 is given by a nilpotent ideal C f ! j g 2 3 := f : T0 T closed immersion of S-schemes T is the spectrum of a local ring and T0 is given by an ideal I with I = 0 C f ! j g Show that the following assertions are equivalent: (i) 1 satisfies the 1-lifting property (resp. -
Giraud's Theorem
Giraud’s Theorem 25 February and 4 March 2019 The Giraud’s axioms allow us to determine when a category is a topos. Lurie’s version indicates the equivalence between the axioms, the left exact localizations, and Grothendieck topologies, i.e. Proposition 1. [2] Let X be a category. The following conditions are equivalent: 1. The category X is equivalent to the category of sheaves of sets of some Grothendieck site. 2. The category X is equivalent to a left exact localization of the category of presheaves of sets on some small category C. 3. Giraud’s axiom are satisfied: (a) The category X is presentable. (b) Colimits in X are universal. (c) Coproducts in X are disjoint. (d) Equivalence relations in X are effective. 1 Sheaf and Grothendieck topologies This section is based in [4]. The continuity of a reald-valued function on topological space can be determined locally. Let (X;t) be a topological space and U an open subset of X. If U is S covered by open subsets Ui, i.e. U = i2I Ui and fi : Ui ! R are continuos functions then there exist a continuos function f : U ! R if and only if the fi match on all the overlaps Ui \Uj and f jUi = fi. The previuos paragraph is so technical, let us see a more enjoyable example. Example 1. Let (X;t) be a topological space such that X = U1 [U2 then X can be seen as the following diagram: X s O e U1 tU1\U2 U2 o U1 O O U2 o U1 \U2 If we form the category OX (the objects are the open sets and the morphisms are given by the op inclusion), the previous paragraph defined a functor between OX and Set i.e it sends an open set U to the set of all continuos functions of domain U and codomain the real numbers, F : op OX ! Set where F(U) = f f j f : U ! Rg, so the initial diagram can be seen as the following: / (?) FX / FU1 ×F(U1\U2) FU2 / F(U1 \U2) then the condition of the paragraph states that the map e : FX ! FU1 ×F(U1\U2) FU2 given by f 7! f jUi is the equalizer of the previous diagram. -
Notes and Solutions to Exercises for Mac Lane's Categories for The
Stefan Dawydiak Version 0.3 July 2, 2020 Notes and Exercises from Categories for the Working Mathematician Contents 0 Preface 2 1 Categories, Functors, and Natural Transformations 2 1.1 Functors . .2 1.2 Natural Transformations . .4 1.3 Monics, Epis, and Zeros . .5 2 Constructions on Categories 6 2.1 Products of Categories . .6 2.2 Functor categories . .6 2.2.1 The Interchange Law . .8 2.3 The Category of All Categories . .8 2.4 Comma Categories . 11 2.5 Graphs and Free Categories . 12 2.6 Quotient Categories . 13 3 Universals and Limits 13 3.1 Universal Arrows . 13 3.2 The Yoneda Lemma . 14 3.2.1 Proof of the Yoneda Lemma . 14 3.3 Coproducts and Colimits . 16 3.4 Products and Limits . 18 3.4.1 The p-adic integers . 20 3.5 Categories with Finite Products . 21 3.6 Groups in Categories . 22 4 Adjoints 23 4.1 Adjunctions . 23 4.2 Examples of Adjoints . 24 4.3 Reflective Subcategories . 28 4.4 Equivalence of Categories . 30 4.5 Adjoints for Preorders . 32 4.5.1 Examples of Galois Connections . 32 4.6 Cartesian Closed Categories . 33 5 Limits 33 5.1 Creation of Limits . 33 5.2 Limits by Products and Equalizers . 34 5.3 Preservation of Limits . 35 5.4 Adjoints on Limits . 35 5.5 Freyd's adjoint functor theorem . 36 1 6 Chapter 6 38 7 Chapter 7 38 8 Abelian Categories 38 8.1 Additive Categories . 38 8.2 Abelian Categories . 38 8.3 Diagram Lemmas . 39 9 Special Limits 41 9.1 Interchange of Limits . -
On Modeling Homotopy Type Theory in Higher Toposes
Review: model categories for type theory Left exact localizations Injective fibrations On modeling homotopy type theory in higher toposes Mike Shulman1 1(University of San Diego) Midwest homotopy type theory seminar Indiana University Bloomington March 9, 2019 Review: model categories for type theory Left exact localizations Injective fibrations Here we go Theorem Every Grothendieck (1; 1)-topos can be presented by a model category that interprets \Book" Homotopy Type Theory with: • Σ-types, a unit type, Π-types with function extensionality, and identity types. • Strict universes, closed under all the above type formers, and satisfying univalence and the propositional resizing axiom. Review: model categories for type theory Left exact localizations Injective fibrations Here we go Theorem Every Grothendieck (1; 1)-topos can be presented by a model category that interprets \Book" Homotopy Type Theory with: • Σ-types, a unit type, Π-types with function extensionality, and identity types. • Strict universes, closed under all the above type formers, and satisfying univalence and the propositional resizing axiom. Review: model categories for type theory Left exact localizations Injective fibrations Some caveats 1 Classical metatheory: ZFC with inaccessible cardinals. 2 Classical homotopy theory: simplicial sets. (It's not clear which cubical sets can even model the (1; 1)-topos of 1-groupoids.) 3 Will not mention \elementary (1; 1)-toposes" (though we can deduce partial results about them by Yoneda embedding). 4 Not the full \internal language hypothesis" that some \homotopy theory of type theories" is equivalent to the homotopy theory of some kind of (1; 1)-category. Only a unidirectional interpretation | in the useful direction! 5 We assume the initiality hypothesis: a \model of type theory" means a CwF. -
Category Theory
CMPT 481/731 Functional Programming Fall 2008 Category Theory Category theory is a generalization of set theory. By having only a limited number of carefully chosen requirements in the definition of a category, we are able to produce a general algebraic structure with a large number of useful properties, yet permit the theory to apply to many different specific mathematical systems. Using concepts from category theory in the design of a programming language leads to some powerful and general programming constructs. While it is possible to use the resulting constructs without knowing anything about category theory, understanding the underlying theory helps. Category Theory F. Warren Burton 1 CMPT 481/731 Functional Programming Fall 2008 Definition of a Category A category is: 1. a collection of ; 2. a collection of ; 3. operations assigning to each arrow (a) an object called the domain of , and (b) an object called the codomain of often expressed by ; 4. an associative composition operator assigning to each pair of arrows, and , such that ,a composite arrow ; and 5. for each object , an identity arrow, satisfying the law that for any arrow , . Category Theory F. Warren Burton 2 CMPT 481/731 Functional Programming Fall 2008 In diagrams, we will usually express and (that is ) by The associative requirement for the composition operators means that when and are both defined, then . This allow us to think of arrows defined by paths throught diagrams. Category Theory F. Warren Burton 3 CMPT 481/731 Functional Programming Fall 2008 I will sometimes write for flip , since is less confusing than Category Theory F. -
Left Kan Extensions Preserving Finite Products
Left Kan Extensions Preserving Finite Products Panagis Karazeris, Department of Mathematics, University of Patras, Patras, Greece Grigoris Protsonis, Department of Mathematics, University of Patras, Patras, Greece 1 Introduction In many situations in mathematics we want to know whether the left Kan extension LanjF of a functor F : C!E, along a functor j : C!D, where C is a small category and E is locally small and cocomplete, preserves the limits of various types Φ of diagrams. The answer to this general question is reducible to whether the left Kan extension LanyF of F , along the Yoneda embedding y : C! [Cop; Set] preserves those limits (see [12] x3). Such questions arise in the classical context of comparing the homotopy of simplicial sets to that of spaces but are also vital in comparing, more generally, homotopical notions on various combinatorial models (e.g simplicial, bisimplicial, cubical, globular, etc, sets) on the one hand, and various \realizations" of them as spaces, categories, higher categories, simplicial categories, relative categories etc, on the other (see [8], [4], [15], [2]). In the case where E = Set the answer is classical and well-known for the question of preservation of all finite limits (see [5], Chapter 6), the question of finite products (see [1]) as well as for the case of various types of finite connected limits (see [11]). The answer to such questions is also well-known in the case E is a Grothendieck topos, for the class of all finite limits or all finite connected limits (see [14], chapter 7 x 8 and [9]). -
A Godefroy-Kalton Principle for Free Banach Lattices 3
A GODEFROY-KALTON PRINCIPLE FOR FREE BANACH LATTICES ANTONIO AVILES,´ GONZALO MART´INEZ-CERVANTES, JOSE´ RODR´IGUEZ, AND PEDRO TRADACETE Abstract. Motivated by the Lipschitz-lifting property of Banach spaces introduced by Godefroy and Kalton, we consider the lattice-lifting property, which is an analogous notion within the category of Ba- nach lattices and lattice homomorphisms. Namely, a Banach lattice X satisfies the lattice-lifting property if every lattice homomorphism to X having a bounded linear right-inverse must have a lattice homomor- phism right-inverse. In terms of free Banach lattices, this can be rephrased into the following question: which Banach lattices embed into the free Banach lattice which they generate as a lattice-complemented sublattice? We will provide necessary conditions for a Banach lattice to have the lattice-lifting property, and show that this property is shared by Banach spaces with a 1-unconditional basis as well as free Banach lattices. The case of C(K) spaces will also be analyzed. 1. Introduction In a fundamental paper concerning the Lipschitz structure of Banach spaces, G. Godefroy and N.J. Kalton introduced the Lipschitz-lifting property of a Banach space. In order to properly introduce this notion, and as a motivation for our work, let us recall the basic ingredients for this construction (see [9] for details). Given a Banach space E, let Lip0(E) denote the Banach space of all real-valued Lipschitz functions on E which vanish at 0, equipped with the norm |f(x) − f(y)| kfk = sup : x, y ∈ E, x 6= y . Lip0(E) kx − yk E The Lipschitz-free space over E, denoted by F(E), is the canonical predual of Lip0(E), that is the closed ∗ linear span of the evaluation functionals δ(x) ∈ Lip0(E) given by hδ(x),fi = f(x) for all x ∈ E and all f ∈ Lip0(E). -
Higher-Dimensional Instantons on Cones Over Sasaki-Einstein Spaces and Coulomb Branches for 3-Dimensional N = 4 Gauge Theories
Two aspects of gauge theories higher-dimensional instantons on cones over Sasaki-Einstein spaces and Coulomb branches for 3-dimensional N = 4 gauge theories Von der Fakultät für Mathematik und Physik der Gottfried Wilhelm Leibniz Universität Hannover zur Erlangung des Grades Doktor der Naturwissenschaften – Dr. rer. nat. – genehmigte Dissertation von Dipl.-Phys. Marcus Sperling, geboren am 11. 10. 1987 in Wismar 2016 Eingereicht am 23.05.2016 Referent: Prof. Olaf Lechtenfeld Korreferent: Prof. Roger Bielawski Korreferent: Prof. Amihay Hanany Tag der Promotion: 19.07.2016 ii Abstract Solitons and instantons are crucial in modern field theory, which includes high energy physics and string theory, but also condensed matter physics and optics. This thesis is concerned with two appearances of solitonic objects: higher-dimensional instantons arising as supersymme- try condition in heterotic (flux-)compactifications, and monopole operators that describe the Coulomb branch of gauge theories in 2+1 dimensions with 8 supercharges. In PartI we analyse the generalised instanton equations on conical extensions of Sasaki- Einstein manifolds. Due to a certain equivariant ansatz, the instanton equations are reduced to a set of coupled, non-linear, ordinary first order differential equations for matrix-valued functions. For the metric Calabi-Yau cone, the instanton equations are the Hermitian Yang-Mills equations and we exploit their geometric structure to gain insights in the structure of the matrix equations. The presented analysis relies strongly on methods used in the context of Nahm equations. For non-Kähler conical extensions, focusing on the string theoretically interesting 6-dimensional case, we first of all construct the relevant SU(3)-structures on the conical extensions and subsequently derive the corresponding matrix equations. -
Lecture 11 Last Lecture We Defined Connections on Fiber Bundles. This Lecture We Will Attempt to Explain What a Connection Does
Lecture 11 Last lecture we defined connections on fiber bundles. This lecture we will attempt to explain what a connection does for differential ge- ometers. We start with two basic concepts from algebraic topology. The first is that of homotopy lifting property. Let us recall: Definition 1. Let π : E → B be a continuous map and X a space. We say that (X, π) satisfies homotopy lifting property if for every H : X × I → B and map f : X → E with π ◦ f = H( , 0) there exists a homotopy F : X × I → E starting at f such that π ◦ F = H. If ({∗}, π) satisfies this property then we say that π has the homotopy lifting property for a point. Now, as is well known and easily proven, every fiber bundle satisfies the homotopy lifting property. A much stronger property is the notion of a covering space (which we will not recall with precision). Here we have the homotopy lifting property for a point plus uniqueness or the unique path lifting property. I.e. there is exactly one lift of a given path in the base starting at a specified point in the total space. The point of a connection is to take the ambiguity out of the homotopy lifting property for X = {∗} and force a fiber bundle to satisfy the unique path lifting property. We will see many conceptual advantages of this uniqueness, but let us start by making this a bit clearer via parallel transport. Definition 2. Let B be a topological space and PB the category whose objects are points of B and whose morphisms are defined via {γ : → B : ∃ c, d ∈ s.t. -
Free Models of T-Algebraic Theories Computed As Kan Extensions Paul-André Melliès, Nicolas Tabareau
Free models of T-algebraic theories computed as Kan extensions Paul-André Melliès, Nicolas Tabareau To cite this version: Paul-André Melliès, Nicolas Tabareau. Free models of T-algebraic theories computed as Kan exten- sions. 2008. hal-00339331 HAL Id: hal-00339331 https://hal.archives-ouvertes.fr/hal-00339331 Preprint submitted on 17 Nov 2008 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. Free models of T -algebraic theories computed as Kan extensions Paul-André Melliès Nicolas Tabareau ∗ Abstract One fundamental aspect of Lawvere’s categorical semantics is that every algebraic theory (eg. of monoid, of Lie algebra) induces a free construction (eg. of free monoid, of free Lie algebra) computed as a Kan extension. Unfortunately, the principle fails when one shifts to linear variants of algebraic theories, like Adams and Mac Lane’s PROPs, and similar PROs and PROBs. Here, we introduce the notion of T -algebraic theory for a pseudomonad T — a mild generalization of equational doctrine — in order to describe these various kinds of “algebraic theories”. Then, we formulate two conditions (the first one combinatorial, the second one algebraic) which ensure that the free model of a T -algebraic theory exists and is computed as an Kan extension. -
Double Homotopy (Co) Limits for Relative Categories
Double Homotopy (Co)Limits for Relative Categories Kay Werndli Abstract. We answer the question to what extent homotopy (co)limits in categories with weak equivalences allow for a Fubini-type interchange law. The main obstacle is that we do not assume our categories with weak equivalences to come equipped with a calculus for homotopy (co)limits, such as a derivator. 0. Introduction In modern, categorical homotopy theory, there are a few different frameworks that formalise what exactly a “homotopy theory” should be. Maybe the two most widely used ones nowadays are Quillen’s model categories (see e.g. [8] or [13]) and (∞, 1)-categories. The latter again comes in different guises, the most popular one being quasicategories (see e.g. [16] or [17]), originally due to Boardmann and Vogt [3]. Both of these contexts provide enough structure to perform homotopy invariant analogues of the usual categorical limit and colimit constructions and more generally Kan extensions. An even more stripped-down notion of a “homotopy theory” (that arguably lies at the heart of model categories) is given by just working with categories that come equipped with a class of weak equivalences. These are sometimes called relative categories [2], though depending on the context, this might imply some restrictions on the class of weak equivalences. Even in this context, we can still say what a homotopy (co)limit is and do have tools to construct them, such as model approximations due to Chach´olski and Scherer [5] or more generally, left and right arXiv:1711.01995v1 [math.AT] 6 Nov 2017 deformation retracts as introduced in [9] and generalised in section 3 below. -
Fibrations II - the Fundamental Lifting Property
Fibrations II - The Fundamental Lifting Property Tyrone Cutler July 13, 2020 Contents 1 The Fundamental Lifting Property 1 2 Spaces Over B 3 2.1 Homotopy in T op=B ............................... 7 3 The Homotopy Theorem 8 3.1 Implications . 12 4 Transport 14 4.1 Implications . 16 5 Proof of the Fundamental Lifting Property Completed. 19 6 The Mutal Characterisation of Cofibrations and Fibrations 20 6.1 Implications . 22 1 The Fundamental Lifting Property This section is devoted to stating Theorem 1.1 and beginning its proof. We prove only the first of its two statements here. This part of the theorem will then be used in the sequel, and the proof of the second statement will follow from the results obtained in the next section. We will be careful to avoid circular reasoning. The utility of the theorem will soon become obvious as we repeatedly use its statement to produce maps having very specific properties. However, the true power of the theorem is not unveiled until x 5, where we show how it leads to a mutual characterisation of cofibrations and fibrations in terms of an orthogonality relation. Theorem 1.1 Let j : A,! X be a closed cofibration and p : E ! B a fibration. Assume given the solid part of the following strictly commutative diagram f A / E |> j h | p (1.1) | | X g / B: 1 Then the dotted filler can be completed so as to make the whole diagram commute if either of the following two conditions are met • j is a homotopy equivalence. • p is a homotopy equivalence.