Local Realizability Toposes and a Modal Logic For

Total Page:16

File Type:pdf, Size:1020Kb

Local Realizability Toposes and a Modal Logic For Electronic Notes in Theoretical Computer Science No URL httpwwwelsevier nll ocate entcs volume htm l pages Lo cal RealizabilityTop oses and a Mo dal Logic for Computability Extended Abstract Steven Awodey Department of Philosophy Carnegie Mel lon University Lars Birkedal School of Computer Science Carnegie Mel lon University Dana S Scott School of Computer Science Carnegie Mel lon University Abstract This work is a step toward developing a logic for typ es and computation that in cludes b oth the usual spaces of mathematics and constructions and spaces from logic and domain theory Using realizabilityweinvestigate a conguration of three top oses whichwe regard as describing a notion of relative computabilityAttention is fo cussed on a certain lo cal map of top oses whichwe study rst axiomatically and then by deriving a mo dal calculus as its internal logic The resulting framework is intended as a setting for the logical and categorical study of relative computability Intro duction We rep ort here on the current status of research on the Logic of Typ es and Computation at Carnegie Mellon University The general goal of this research program is to develop a logical framework for the theories of typ es and computability that includes the standard mathematical spaces alongside the many constructions and spaces known from typ e theory and domain theory One purp ose of this goal is to facilitate the study of computable op erations and maps on data that is not necessarily computable such as the space of all real numb ers Email awodeycmuedu birkedalcscmuedu danascottcscmuedu Lars Birkedal is supp orted in part by US National Science Foundation Grant CCR c Published by Elsevier Science B V Awodey et al Concretely in the research describ ed here we use the realizabilitytopos over the graph mo del P N of the untyp ed lamb da calculus together with the subgraph mo del given by the recursively enumerable subsets to repre sent the classical and computable worlds resp ectively There results a certain con guration of top oses that can b e regarded as describing a notion of rel ative computability We study this con guration axiomatically and derive a higherorder mo dal logic in which to reason ab out it The logic can then b e applied to the original mo del to formalize reasoning ab out computability in that setting Moreover the resulting logical framework provides a general categorical semantics and logical syntax for reasoning in a formal wayabout abstract computabilitywhich it is hop ed could also b e useful for formally similar concepts such as logical de nability In somewhat more detail Section b egins by recalling the standard re alizability top oses RT Aand RT A resulting from a partial combinatory algebra A and a subalgebra A We then identify a third category RT A A whichplays a key role very roughly sp eaking it represents the world of all continuous ob jects but with only computable maps b etween them This cat egory RT A A is a top os the relative realizability topos on A with resp ect to the subalgebra A The top oses RT AandRT A are not particularly wellrelated by them selves the purp ose of the relative realizabilitytopos RT A A is to remedy this defect The three top oses are related to each other as indicated in the following diagram in which the three functors on the left leg constitute a lo cal geometric morphism while the right leg is a logical morphism RT A A u H u H u u H u u u H u u u H u u u H u u u H u u zu u u RT A RT A The lo cal geometric morphism on the left is our chief concern and the fo cus of Section which also mentions some examples and prop erties of these fairly wellundersto o d maps of top oses When we rst encountered it wewere pleased to recognize our situation as an instance of one that FW Lawvere has already called attention to and dubb ed an adjoint cylinder or more colorfully a unity and identity of opposites In Section we present four axioms for lo cal maps of top oses and sketch the pro of that they are sound and complete Actually since the situation we are mainly interested inie realizabilityforces the lo cal map to b e lo calic we give the axioms in a form that implies this condition We simply mention here that a mo di cation of axiom ab out generators will accomo date all b ounded lo cal maps This axiomatization has b een found useful in working with the particular situation wehave in mind but its general utility for lo cal maps of top oses remains to b e seen Not to b e confused with the standard notion of computability relative to an oracle Awodey et al One application of sorts of the axioms for lo cal maps is the investigation of their logical prop erties These are given in Section in the form of a logical calculus involving two prop ositional op erations written and with left adjointto It turns out that satis es the S mo dal logic p ostulates for the boxop eration We here term the calculus a modal logic for computability since that is the interpretation wehave in mind but of course this mo dal logic can b e interpreted in any lo cal top os Weintend to use it to investigate the logical relations that hold in the relative realizability top os however this asp ect of our work is only just b eginning Note that any lo cal map also induces a closely related pair of adjoint op erations on logical types ob jects in addition to the ones on formulas sub ob jects studied here relating our work to The idea of a mo dal com putability op erator is due to the senior author January and was the original imp etus for this work parts of which are from the second authors do ctoral thesis The nal brief section of the pap er sp ells out the intended interpretation of the calculus in the relative realizability top os RT A A Realizability top oses for computability Let A K S b e a partial combinatory algebra PCA often we just denote it by its underlying set A The binary op erator is the partial application and combinators K and S are taken to b e part of the structure and not just required to exist Let A b e a subPCA of AthatisA is a subset of A containing K and S and closed under partial application Intuitivelywe are thinking of the realizers in A as continuous realizers and of theose in A as computable realizers This intuition comes from the main example where A is P N the graph mo del on the p owerset of the natural numb ers and A is RE the recursively enumerable subgraphmo del Note that the mo del P N has a con tinuum of countable subPCAs As another example one may consider van Oostens combinatory algebra B for sequential computation and its eective subalgebra B see e The PCAs A and A give rise to two realizability top oses RT A and RT A in the standard way One may think of RT Aasauniverse where all ob jects and all maps are realized bycontinuous realizers Likewise RT A may b e thought ofasauniverse where all ob jects and all maps are realized by computable realizers Unfortunately these two top oses are not very well related in particular it is not clear how to talk ab out computable maps op erating on continuous ob jects which is what one would liketodoforthe purp oses of eg computable analysis Thus one is led to intro duce an other realizability top os RT A A where intuitively equality on all ob jects is realized bycontinuous realizers and all maps are realized by computable Awodey et al realizers The top os RT A A is constructed by mo difying the underlying trip os for RT A in the following way The nonstandard predicates on a set I are still functions I P A into the p owerset of A and the Heyting prealgebra op erations are the same as in the trip os underlying RT A The mo di cation is in the de nition of the entailment relation wesay over I i there is a realizer a in A not just in Asuch that for all i in I allb i a b is de ned and a b i In the terminology of Pitts wehavechanged the designated truth values to b e those subsets of A whichhave a nonempty op intersection with A Denote this new trip os by P Set Cat Then RT A A isthetoposSetP represented by P Explicitly ob jects of RT A A are pairs X with X a set and X X X X P A a nonstandard equality predicate with computable realiz ers for symmetry and transitivity Morphisms from X toY are X Y equivalence classes of functional relations F X Y P A with computable realizers proving that F is a functional relation Two such functional rela tions F and G are equivalent i there are computable realizers showing them equivalent Wenow see that intuitivelyitmakes sense to think of ob jects as ob jects with continuous realizers for existence and equality of RT A A elements and of morphisms f F as computable maps since the realizers for the functionalityof F are required to b e computable Geometry of the realizabili ty top oses for computabil ity op Let Q Set Cat b e the standard realizability trip os on A ie the trip os underlying RT A Wenow de ne three Setindexed functors b etween Q and P Q P and P Q and r Q P These are de ned as follows Over I wehave I P A i i I I P AiA i I S r I P A i A i I PA where and are calculated as in P Theorem Under these denitions it fol lows that isageometric morphism of triposes from P to Q r is a geometric morphism of triposes from Q to P We rst learned ab out the top os RT A A from Thomas Streicher in February but the construction has actually b een known for a long time see Page item ii Awodey et al For al l I Set and r areboth ful l and faithful I I By Prop osition in these
Recommended publications
  • Algebras in Which Every Subalgebra Is Noetherian
    PROCEEDINGS OF THE AMERICAN MATHEMATICAL SOCIETY Volume 142, Number 9, September 2014, Pages 2983–2990 S 0002-9939(2014)12052-1 Article electronically published on May 21, 2014 ALGEBRAS IN WHICH EVERY SUBALGEBRA IS NOETHERIAN D. ROGALSKI, S. J. SIERRA, AND J. T. STAFFORD (Communicated by Birge Huisgen-Zimmermann) Abstract. We show that the twisted homogeneous coordinate rings of elliptic curves by infinite order automorphisms have the curious property that every subalgebra is both finitely generated and noetherian. As a consequence, we show that a localisation of a generic Skylanin algebra has the same property. 1. Introduction Throughout this paper k will denote an algebraically closed field and all algebras will be k-algebras. It is not hard to show that if C is a commutative k-algebra with the property that every subalgebra is finitely generated (or noetherian), then C must be of Krull dimension at most one. (See Section 3 for one possible proof.) The aim of this paper is to show that this property holds more generally in the noncommutative universe. Before stating the result we need some notation. Let X be a projective variety ∗ with invertible sheaf M and automorphism σ and write Mn = M⊗σ (M) ···⊗ n−1 ∗ (σ ) (M). Then the twisted homogeneous coordinate ring of X with respect to k M 0 M this data is the -algebra B = B(X, ,σ)= n≥0 H (X, n), under a natu- ral multiplication. This algebra is fundamental to the theory of noncommutative algebraic geometry; see for example [ATV1, St, SV]. In particular, if S is the 3- dimensional Sklyanin algebra, as defined for example in [SV, Example 8.3], then B(E,L,σ)=S/gS for a central element g ∈ S and some invertible sheaf L over an elliptic curve E.WenotethatS is a graded ring that can be regarded as the “co- P2 P2 ordinate ring of a noncommutative ” or as the “coordinate ring of nc”.
    [Show full text]
  • Lie Group Homomorphism Φ: → Corresponds to a Linear Map Φ: →
    More on Lie algebras Wednesday, February 14, 2018 8:27 AM Simple Lie algebra: dim 2 and the only ideals are 0 and itself. Have classification by Dynkin diagram. For instance, , is simple: take the basis 01 00 10 , , . 00 10 01 , 2,, 2,, . Suppose is in the ideal. , 2. , , 2. If 0, then X is in the ideal. Then ,,, 2imply that H and Y are also in the ideal which has to be 2, . The case 0: do the same argument for , , , then the ideal is 2, unless 0. The case 0: , 2,, 2implies the ideal is 2, unless 0. The ideal is {0} if 0. Commutator ideal: , Span,: , ∈. An ideal is in particular a Lie subalgebra. Keep on taking commutator ideals, get , , ⊂, … called derived series. Solvable: 0 for some j. If is simple, for all j. Levi decomposition: any Lie algebra is the semi‐direct product of a solvable ideal and a semisimple subalgebra. Similar concept: , , , , …, ⊂. Sequence of ideals called lower central series. Nilpotent: 0 for some j. ⊂ . Hence nilpotent implies solvable. For instance, the Lie algebra of nilpotent upper triangular matrices is nilpotent and hence solvable. Can take the basis ,, . Then ,,, 0if and , if . is spanned by , for and hence 0. The Lie algebra of upper triangular matrices is solvable but not nilpotent. Can take the basis ,,,, ,,…,,. Similar as above and ,,,0. . So 0. But for all 1. Recall that any Lie group homomorphism Φ: → corresponds to a linear map ϕ: → . In the proof that a continuous homomorphism is smooth. Lie group Page 1 Since Φ ΦΦΦ , ∘ Ad AdΦ ∘.
    [Show full text]
  • Gauging the Octonion Algebra
    UM-P-92/60_» Gauging the octonion algebra A.K. Waldron and G.C. Joshi Research Centre for High Energy Physics, University of Melbourne, Parkville, Victoria 8052, Australia By considering representation theory for non-associative algebras we construct the fundamental and adjoint representations of the octonion algebra. We then show how these representations by associative matrices allow a consistent octonionic gauge theory to be realized. We find that non-associativity implies the existence of new terms in the transformation laws of fields and the kinetic term of an octonionic Lagrangian. PACS numbers: 11.30.Ly, 12.10.Dm, 12.40.-y. Typeset Using REVTEX 1 L INTRODUCTION The aim of this work is to genuinely gauge the octonion algebra as opposed to relating properties of this algebra back to the well known theory of Lie Groups and fibre bundles. Typically most attempts to utilise the octonion symmetry in physics have revolved around considerations of the automorphism group G2 of the octonions and Jordan matrix representations of the octonions [1]. Our approach is more simple since we provide a spinorial approach to the octonion symmetry. Previous to this work there were already several indications that this should be possible. To begin with the statement of the gauge principle itself uno theory shall depend on the labelling of the internal symmetry space coordinates" seems to be independent of the exact nature of the gauge algebra and so should apply equally to non-associative algebras. The octonion algebra is an alternative algebra (the associator {x-1,y,i} = 0 always) X -1 so that the transformation law for a gauge field TM —• T^, = UY^U~ — ^(c^C/)(/ is well defined for octonionic transformations U.
    [Show full text]
  • Notes on Mathematical Logic David W. Kueker
    Notes on Mathematical Logic David W. Kueker University of Maryland, College Park E-mail address: [email protected] URL: http://www-users.math.umd.edu/~dwk/ Contents Chapter 0. Introduction: What Is Logic? 1 Part 1. Elementary Logic 5 Chapter 1. Sentential Logic 7 0. Introduction 7 1. Sentences of Sentential Logic 8 2. Truth Assignments 11 3. Logical Consequence 13 4. Compactness 17 5. Formal Deductions 19 6. Exercises 20 20 Chapter 2. First-Order Logic 23 0. Introduction 23 1. Formulas of First Order Logic 24 2. Structures for First Order Logic 28 3. Logical Consequence and Validity 33 4. Formal Deductions 37 5. Theories and Their Models 42 6. Exercises 46 46 Chapter 3. The Completeness Theorem 49 0. Introduction 49 1. Henkin Sets and Their Models 49 2. Constructing Henkin Sets 52 3. Consequences of the Completeness Theorem 54 4. Completeness Categoricity, Quantifier Elimination 57 5. Exercises 58 58 Part 2. Model Theory 59 Chapter 4. Some Methods in Model Theory 61 0. Introduction 61 1. Realizing and Omitting Types 61 2. Elementary Extensions and Chains 66 3. The Back-and-Forth Method 69 i ii CONTENTS 4. Exercises 71 71 Chapter 5. Countable Models of Complete Theories 73 0. Introduction 73 1. Prime Models 73 2. Universal and Saturated Models 75 3. Theories with Just Finitely Many Countable Models 77 4. Exercises 79 79 Chapter 6. Further Topics in Model Theory 81 0. Introduction 81 1. Interpolation and Definability 81 2. Saturated Models 84 3. Skolem Functions and Indescernables 87 4. Some Applications 91 5.
    [Show full text]
  • Borel Subgroups and Flag Manifolds
    Topics in Representation Theory: Borel Subgroups and Flag Manifolds 1 Borel and parabolic subalgebras We have seen that to pick a single irreducible out of the space of sections Γ(Lλ) we need to somehow impose the condition that elements of negative root spaces, acting from the right, give zero. To get a geometric interpretation of what this condition means, we need to invoke complex geometry. To even define the negative root space, we need to begin by complexifying the Lie algebra X gC = tC ⊕ gα α∈R and then making a choice of positive roots R+ ⊂ R X gC = tC ⊕ (gα + g−α) α∈R+ Note that the complexified tangent space to G/T at the identity coset is X TeT (G/T ) ⊗ C = gα α∈R and a choice of positive roots gives a choice of complex structure on TeT (G/T ), with the holomorphic, anti-holomorphic decomposition X X TeT (G/T ) ⊗ C = TeT (G/T ) ⊕ TeT (G/T ) = gα ⊕ g−α α∈R+ α∈R+ While g/t is not a Lie algebra, + X − X n = gα, and n = g−α α∈R+ α∈R+ are each Lie algebras, subalgebras of gC since [n+, n+] ⊂ n+ (and similarly for n−). This follows from [gα, gβ] ⊂ gα+β The Lie algebras n+ and n− are nilpotent Lie algebras, meaning 1 Definition 1 (Nilpotent Lie Algebra). A Lie algebra g is called nilpotent if, for some finite integer k, elements of g constructed by taking k commutators are zero. In other words [g, [g, [g, [g, ··· ]]]] = 0 where one is taking k commutators.
    [Show full text]
  • Topoi for a Super-Noetherian Subalgebra Equipped with a Riemannian Number
    Topoi for a Super-Noetherian Subalgebra Equipped with a Riemannian Number M. Lafourcade, Q. Germain and H. D´escartes Abstract Let λ be a Gaussian, integrable, canonically Hadamard modulus. Re- cent developments in dynamics [32] have raised the question of whether V 2 i. We show that jm^j ∼ P. Now in this setting, the ability to char- acterize categories is essential. It is not yet known whether ξ 6= −∞, although [4, 4, 10] does address the issue of minimality. 1 Introduction In [33], the authors address the separability of Weierstrass, stochastically anti- hyperbolic graphs under the additional assumption that every subset is measur- able. Is it possible to compute Clifford sets? The work in [36] did not consider the meromorphic case. This could shed important light on a conjecture of Sylvester. Is it possible to characterize stable subgroups? It is well known that z ≥ !(f). In [32], the authors address the admissibility of sets under the additional assumption that every Fourier, contra-Gauss, contra-stable set is smoothly Lobachevsky and simply Bernoulli. This could shed important light on a con- jecture of Clairaut. The work in [29] did not consider the null case. The ground- breaking work of D. Anderson on regular homomorphisms was a major advance. 1 It is well known that 0p ∼ 1 . Recently, there has been much interest in the description of ultra-discretely tangential equations. It would be interesting to apply the techniques of [32] to prime vector spaces. In [23], the main result was the extension of unique monoids. In [27], the authors address the admissibility of intrinsic matrices under the additional assumption that there exists an orthogonal, stochastically pseudo- minimal and simply super-separable super-Artinian, almost everywhere intrin- sic, conditionally semi-onto random variable.
    [Show full text]
  • Chapter 5 Subalgebras and Unions
    CHAPTER 5 SUBALGEBRAS AND UNIONS §a Weak and relative subalgebras The subalgebra concept has two very natural weakenings. The first of these concerns the algebraic structure that is inherited by arbitrary subsets of the universe of an algebra, as opposed to subuniverses; one of the more compel- ling ways in which partial algebras arise in the study of total algebras. The second corresponds with the algebraic structure necessary for a mapping from another algebra to be a homomorphism. a1 Definition. Let A = 〈A, I〉 and B = 〈B, J〉 be algebras such that A ⊆ B. (a) A is a relative subalgebra of B, notation A ⊆ B, and B a outer extension of A, if Dom(I) = Dom(J), and for every symbol S ∈ Dom(J), I(S) = J(S)A. (b) A is a weak subalgebra of B, notation A ⊆w B, if Dom(I) = Dom(J), and for every symbol S ∈ Dom(I), I(S) ⊆ J(S). Observe that any subset A of the universe of an algebra B determines a unique relative subalgebra of B that has A for universe. We denote it by AB. On the other hand, there may be many weak subalgebras of B that have A for a universe. In particular, there may be many weak subalgebras of B that have B for a universe; we shall call them weakenings of B. If A is a weakening of B, then B is an inner extension of A. If B is a total algebra, and A is dense in B, we say that B is a completion of AB.
    [Show full text]
  • The Space of Measurement Outcomes As a Spectrum for Non-Commutative Algebras
    The space of measurement outcomes as a spectrum for non-commutative algebras Bas Spitters Bohrification defines a locale of hidden variables internal in a topos. We find that externally this is the space of partial measurement outcomes. By considering the ::-sheafification, we obtain the space of measurement outcomes which coincides with the spectrum for commutative C*-algebras. 1 Introduction By combining Bohr’s philosophy of quantum mechanics, Connes’ non-commutative geometry [Con94], constructive Gelfand duality [BM00b, BM00a, Coq05, CS09] and inspiration from Doering and Isham’s spectral presheaf [DI08], we proposed Bohrification as a spatial quantum logic [HLS09a, HLS09b]. Given a C*-algebra A, modeling a quantum system, consider the poset of Bohr’s classical concepts C (A) := fC j C is a commutative C*-subalgebra of Ag: In the functor topos SetsC (A) we consider the Bohrification A: the trivial functor C 7! C. This is an internal C*-algebra of which we can compute the spectrum, an internal locale S in the topos SetsC (A). This locale, or its externalization, is our proposal for an intuitionistic quantum logic [HLS09a, HLS09b]. In the present paper we explore a possible refinement of this proposal motivated by what happens for commutative algebras and by questions about maximal subalgebras. In section 4 we compute the externalization of this locale. It is the space of partial measurement outcomes: the points are pairs of a C*-subalgebra together with a point of its spectrum. This construction raises two natural questions: • Can we restrict to the maximal commutative subalgebras, i.e. total measurement frames? • Are we allowed to use classical logic internally? In section 5 we will see that, in a sense, the answers to both of these questions are positive.
    [Show full text]
  • LIE ALGEBRAS 1 Definition of a Lie Algebra K Is a Fixed Field. Let L Be a K-Vector Space (Or Vector Space). We Say That L Is
    LIE ALGEBRAS 1 Definition of a Lie algebra k is a fixed field. Let L be a k-vector space (or vector space). We say that L is a k-algebra (or algebra) if we are given a bilinear map L×L −! L denoted (x; y) 7! xy. If L; L0 are algebras, an algebra homomorphism f : L −! L0 is a linear map such that f(xy) = f(x)f(y) for all x; y. We say that f is an algebra isomorphism if it is an algebra homomorphism and a vector space isomorphism. In this case f −1 : L0 −! L is an algebra isomorphism. If L is an algebra, a subset L0 ⊂ L is a subalgebra if it is a vector subspace and x 2 L0; y 2 L0 =) xy 2 L0. Then L0 is itself an algebra in an obvious way. If L is an algebra, a subset I ⊂ L is an ideal if it is a vector subspace; x 2 L; y 2 I =) xy 2 I; x 2 I; y 2 L =) xy 2 I. Then I is a subalgebra. Moreover, the quotient vector space V=I is an algebra with multiplication (x + I)(y + I = xy + I. (Check that this is well defined.) The canonical map L −! L=I is an algebra homomorphism with kernel I. Conversely, if f : L −! L0 is any algebra homomorphism then ker(f) = f −1(0) is an ideal of L. We say that the algebra L is a Lie algebra if (a) xx = 0 for all x; (b) x(yz) + y(zx) + z(xy) = 0 for all x; y; z.
    [Show full text]
  • (Universal Algebra And) Category Theory in Foundations of Computer Science
    (Universal Algebra and) Category Theory in Foundations of Computer Science Andrzej Tarlecki Institute of Informatics Faculty of Mathematics, Informatics and Mechanics University of Warsaw http://www.mimuw.edu.pl/~tarlecki office: 4750 [email protected] phone: (48)(22)(55) 44475, 20443 This course: http://www.mimuw.edu.pl/~tarlecki/teaching/ct/ Andrzej Tarlecki: Category Theory, 2018 - 1 - Universal algebra and category theory: basic ideas, notions and some results • Algebras, homomorphisms, equations: basic definitions and results • Categories; examples and simple categorical definitions • Limits and colimits • Functors and natural transformations • Adjunctions • Cartesian closed categories • Monads • Institutions (abstract model theory, abstract specification theory) BUT: Tell me what you want to learn! Andrzej Tarlecki: Category Theory, 2018 - 2 - Literature Plenty of standard textbooks But this will be roughly based on: • D.T. Sannella, A. Tarlecki. Foundations of Algebraic Specifications and Formal Program Development. Springer, 2012. − Chap. 1: Universal algebra − Chap. 2: Simple equational specifications − Chap. 3: Category theory Andrzej Tarlecki: Category Theory, 2018 - 3 - One motivation Software systems (modules, programs, databases. ): sets of data with operations on them • Disregarding: code, efficiency, robustness, reliability, . • Focusing on: CORRECTNESS Universal algebra Category theory from rough analogy A language to further abstract away from the standard notions of univer- module interface ; signature sal algebra, to deal with their numer- module ; algebra ous variants needed in foundations of module specification ; class of algebras computer science. Andrzej Tarlecki: Category Theory, 2018 - 4 - Signatures Algebraic signature: Σ = (S; Ω) • sort names: S • operation names, classified by arities and result sorts: Ω = hΩw;siw2S∗;s2S Alternatively: Σ = (S; Ω; arity; sort) with sort names S, operation names Ω, and arity and result sort functions arity :Ω ! S∗ and sort :Ω ! S.
    [Show full text]
  • Quasi-Hermitian Locally Compact Groups Are Amenable
    1 QUASI-HERMITIAN LOCALLY COMPACT GROUPS ARE AMENABLE EBRAHIM SAMEI AND MATTHEW WIERSMA Abstract. A locally compact group G is Hermitian if the spectrum SpL1(G)(f) ⊆ R for every 1 ∗ f ∈ L (G) satisfying f = f , and quasi-Hermitian if SpL1(G)(f) ⊆ R for every f ∈ Cc(G) satisfying f = f ∗. We show that every quasi-Hermitian locally compact group is amenable. This, in particular, confirms the long-standing conjecture that every Hermitian locally compact group is amenable, a problem that has remained open since the 1960s. Our approach involves introducing the theory of “spectral interpolation of triple Banach ∗-algebras” and applying ∗ it to a family PFp(G) (1 ≤ p ≤ ∞) of Banach ∗-algebras related to convolution operators 1 ∗ ∗ that lie between L (G) and Cr (G), the reduced group C -algebra of G. We show that if ∗ ∗ G is quasi-Hermitian, then PFp(G) and Cr (G) have the same spectral radius on Hermitian elements in Cc(G) for p ∈ (1, ∞), and then deduce that G must be amenable. We also give an alternative proof to Jenkin’s result in [19] that a discrete group containing a free sub-semigroup on two generators is not quasi-Hermitian. This, in particular, provides a dichotomy on discrete elementary amenable groups: either they are non quasi-Hermitian or they have subexponential growth. Finally, for a non-amenable group G with either rapid decay or Kunze-Stein property, ∗ we prove the stronger statement that PFp(G) is not “quasi-Hermitian relative to Cc(G)” unless p = 2. 1. Introduction Let A be a Banach ∗-algebra, i.e.
    [Show full text]
  • Structural Co~Pleteness in Algebra and Logic
    COLLOQUIA MATHEMATICA SOCIETATIS JANOS BOLYAI 54, ALGEBRAIC LOGIC, BUDAPEST (HUNGARY), 1988 Structural Co~pleteness in Algebra and Logic CLIFFORD BERGMAN A number of authors, particularly those studying "intermediate" intu­ it\onistjc logic, have asked whether a given logic is structurally complete. See [14] and [12] for example. Roughly speaking, a logic is structurally com­ plete if every proper extension must contain new logical axioms (as opposed to nothing but new rules of inference). In particular, structural complete­ ness can be seen as a kind of maximality condition on a logic. Using techniques of algebraic logic, it is possible to study many log­ ics by finding an appropriate class of algebras in which various (algebraic) properties reflect the logical ones of interest. The property corresponding to structural completeness turns out to be quite interesting algebraically, and can be studied independently of any connections to logic. This has been done in a number of papers such as [7], [2] and [9]. In this paper we will briefly consider the notion of structural complete­ ness in its original logical context. We then go on to define and study the algebraic analog, as well as a hereditary version, called deductiveness. Unlike the situation in universal algebra, there is not yet any general agreement in algebraic logic on the definition of basic concepts (such as a logic!) or even on the motivating examples. Since our intent in section 1 is ' primarily motivational, we do not feel it is necessary to completely specify what we mean by a "logic". Instead we give what we hope is a minimal set of conditions that will hold in any reasonable definition of the term.
    [Show full text]