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Andrius Kulikauskas
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 Compare dualities with perspectives and dialectics. For example, "the truth is relative" switches us from an object to its arrows  but dialectic can ground an absolute truth.
 Understand the bijective proof between involutions and standard tableau. Understand
 Ištirti simetrinių funkcijų dualumus: elementary ir homogeneous, Schur ir power.
 How do Grothendieck's six operations (inverse image, direct image, proper direct image, proper inverse image, internal tensor product, internal Hom) fit in the map of dualities?
 Relate my combinatorial proof of the CayleyHamilton theorem to Nakayama's lemma making use of Atiyah's observation.
 Make a list of the central mathematical examples to study and relate.
 Make a list of the central objects in combinatorics  look at Stanley's books.
 Does category theory distinguish between automorphisms and isomorphisms?
 Dual problems in linear programming. What sort of duality is this? Is it related to adjoints?
 Study the duality between 1^N and N in symmetric functions (Young tableaux) but also Catalan numbers, etc. Study nonassociativity, as with the Lie bracket or subtraction.
See: John Baez: Duality in Logic and Physics
I am studying the various cases of duality in math. I imagine that at the heart is the duality between zero and infinity by way of one as in God's Dance. Duality is the basis for logic, and mathematics gives the ways of deviating from duality. Duality is also the structural mirror established within the foursome, fivesome, sixsome and sevensome.
Logic: Duality
Duality arises from a symmetry between two ways of looking at something where there is no reason to choose one over the other. This is driven by the sevensome in defining logic as the balancing of the conscious (not known) and the unconscious (known), what is and what is not (but complements it).
 Logic deals with syntax  external relationships, as in category theory, because it is the syntactic form of the argument which is independent of the actual content.
 Stone's representation theorem for Boolean algebras. Every Boolean algebra is isomorphic to a certain field of sets. Thank you to Eugenijus Paliokas for pointing that out.
 Generalized by Stone's duality: categorical dualities between certain categories of topological spaces and categories of partially ordered sets. They form a natural generalization of Stone's representation theorem for Boolean algebras. Stonetype dualities provide the foundation for pointless topology and are exploited in theoretical computer science for the study of formal semantics.
 Duality theory for distributive lattices provides three different (but closely related) representations of bounded distributive lattices via Priestley spaces, spectral spaces, and pairwise Stone spaces. This generalizes the wellknown Stone duality between Stone spaces and Boolean algebras. There are three equivalent ways of representing bounded distributive lattices. Each one has its own motivation and advantages, but ultimately they all serve the same purpose of providing better understanding of bounded distributive lattices.
Math is subtle deviations from pure duality
These subtle deviations seem to leverage infinity.
 Topology is based on defining open sets to require the inclusion of arbitrary unions but only finite intersections of open sets.
 In ring theory, there is a subtle distinction between the descending chain condition  Artinian rings, and the ascending chain condition  Noetherian rings.
Logic in Mathematics: The Kinds of Duality
Sources of examples of duality
Involutions
 Involutions
 Involutions are counted by Young tableaux (standard tableaux). So what do special rim hook tableaux count? And can we prove therefore that there is no involution for K1 K = 1 ? For if there was an involution then we would have a way to deal with all involutions?
 My dream of Young tableaux whose entries were short and long dashes  "this is the fundamental unit of information".
 Tableaux as the square root of a matrix.
 The asymptotic growth of the number of involutions grows as the square root of n. This supports the idea of the involutions as a "square root" of... matrices?
The fundamental antiduality (SchurWeyl duality) between external representations and internal structure
 Schur–Weyl duality is a mathematical theorem in representation theory that relates irreducible finitedimensional representations of the general linear and symmetric groups.
 Four flavors of SchurWeyl duality
 Tannaka duality An algebra A is reconstructible from the fiber functor on the category of all its modules. (I think: an algebra A is reconstructible from all of its representations.)
 Tannaka duality: A simple case of Tannaka duality is that of Gsets of a group, i.e. representations on a set. In this case, Tannaka duality follows entirely from repeated application of the ordinary Yoneda lemma.
Antiduality: Internal structure and external relationships
 This is the point of Hopf algebras: multiplication (generating external structure) is dual to comultiplication (generating internal structure)
 An automorphism (mapping a structure to itself) is an internal isomorphism. Typically, isomorphisms are external.
 This is the duality of category theory: External relationships can restate internal structure.
 Kategorijų teorijos prieštaringumas yra, kad pavyzdžiai yra "objektai" su vidinėmis sandaromis, nors tai kertasi su kategorijų teorijos dvasia.
 Matematika skiria vidines sandaras (semantika) ir išorinius santykius (sintaksė). Užtat labai svarbu mąstyti apie "viską", kuriam nėra išorinių santykių. Panašiai gal būtų galima mąstyti apie nieką, kur nėra vidinės sandaros. Nors viskas irgi neturi vidinės sandaros. Užtat viskam semantika ir sintaksė yra atitinkamai visiškai paprasta.
 Duality between matrices expressed explicitly (in terms of entries) and implicitly (in terms of eigenvalues).
Dualities in the symmetric functions: Elementary and homogeneous; Schur and power; monomial and forgotten?
AntiDuality: Symmetry and Structure
 A "transformation group" is a group acting as transformations of some set S. Every transformation group is the group of all permutations preserving some structure on S, and this structure is essentially unique. The bigger the transformation group, the less structure: symmetry and structure are dual, just like "entropy" and "information", or "relativity" and "invariance".
Duality: Translating structures
 Any two structures which have a nice map from one to the other have a duality in that you can start from one and go to the other.
 Galois theory: field extensions (solutions of polynomials) and groups
 Lie groups: solutions to differential equations. Lie's idée fixe was to develop a theory of symmetries of differential equations that would accomplish for them what Évariste Galois had done for algebraic equations: namely, to classify them in terms of group theory. Lie and other mathematicians showed that the most important equations for special functions and orthogonal polynomials tend to arise from group theoretical symmetries. In Lie's early work, the idea was to construct a theory of continuous groups, to complement the theory of discrete groups that had developed in the theory of modular forms, in the hands of Felix Klein and Henri Poincaré. The initial application that Lie had in mind was to the theory of differential equations. On the model of Galois theory and polynomial equations, the driving conception was of a theory capable of unifying, by the study of symmetry, the whole area of ordinary differential equations. However, the hope that Lie Theory would unify the entire field of ordinary differential equations was not fulfilled. Symmetry methods for ODEs continue to be studied, but do not dominate the subject. There is a differential Galois theory, but it was developed by others, such as Picard and Vessiot, and it provides a theory of quadratures, the indefinite integrals required to express solutions.
 de Rham cohomology links algebraic topology and differential topology
 Hilbert's Nullstellensatz
 Class field theory provides a onetoone correspondence between finite abelian extensions of a fixed global field and appropriate classes of ideals of the field or open subgroups of the idele class group of the field.
 One may ask analytic questions about algebraic numbers, and use analytic means to answer such questions; it is thus that algebraic and analytic number theory intersect. For example, one may define prime ideals (generalizations of prime numbers in the field of algebraic numbers) and ask how many prime ideals there are up to a certain size. This question can be answered by means of an examination of Dedekind zeta functions, which are generalizations of the Riemann zeta function, a key analytic object at the roots of the subject.[79] This is an example of a general procedure in analytic number theory: deriving information about the distribution of a sequence (here, prime ideals or prime numbers) from the analytic behavior of an appropriately constructed complexvalued function.
 In mathematics, monstrous moonshine, or moonshine theory, is a term devised by John Conway and Simon P. Norton in 1979, used to describe the unexpected connection between the monster group M and modular functions, in particular, the j function. It is now known that lying behind monstrous moonshine is a vertex operator algebra called the moonshine module or monster vertex algebra, constructed by Igor Frenkel, James Lepowsky, and Arne Meurman in 1988, having the monster group as symmetries. This vertex operator algebra is commonly interpreted as a structure underlying a conformal field theory, allowing physics to form a bridge between two mathematical areas. The conjectures made by Conway and Norton were proved by Richard Borcherds for the moonshine module in 1992 using the noghost theorem from string theory and the theory of vertex operator algebras and generalized Kac–Moody algebras.
 Isbell duality relates higher geometry with higher algebra.
 Topos links geometry and logic.
 The AGT correspondence is a relationship between Liouville field theory on a punctured Riemann surface and a certain fourdimensional SU(2) gauge theory obtained by compactifying the 6D (2,0) superconformal field theory on the surface.
 The modularity theorem (formerly called the Taniyama–Shimura–Weil conjecture and several related names) states that elliptic curves over the field of rational numbers are related to modular forms.
Internal, Implicit Dualities
Duality: Conjugation
 Square roots of i. There are two square roots of 1. One we call +i, the other i, but neither should have priority over the other. Similarly, clockwise and counterclockwise rotations should not be favored. Complex conjugation is a way of asserting this. (Note that the integer +1 is naturally favored over 1. But there is no such natural favoring for i. It is purely conventional, a misleading artificial contrivance.)
 Conjugation (ab)* = b*a* is very important in the CayleyDickson construction of the numbers: real, complex, quaternion, octonion.
 Conjugation establishes the twosome by way of the Complex numbers. The Reals give the onesome. And this is followed by the Quaternions defining the threesome and so presumably the Octonions define the foursome.
Duality: Halving space: Rotation: Reversing orientation
 Coxeter groups are built from reflections. Reflections are dualities.
 A rectangular matrix can be written out from left to right or right to left. So we have the transpose matrix.
 If G is a group and ρ is a linear representation of it on the vector space V, then the dual representation ρ* is defined over the dual vector space V* as follows: ρ*(g) is the transpose of ρ(g−1), that is, ρ*(g) = ρ(g−1)T for all g ∈ G. A general ring module does not admit a dual representation. Modules of Hopf algebras do, however.
Duality: Reflection
 Dual root system  roots and coroots, given by the inner product, thus by reflection to match the shorter root with the longer root. This is generalized by the root datum of an algebraic group, which furthermore determines the center of a group. The dual root datum is gotten by switching the characters with the 1parameter subgroups, and the roots with the coroots.
 Given a connected reductive algebraic group G, the Langlands dual group is the complex connected reductive group whose root datum is dual to that of G.
Duality: Reversing order of operations
 Normality says conjugate invariancy: gN = Ng.
 Wikipedia: In applications to logic, this then looks like a very general description of negation (that is, proofs run in the opposite direction). If we take the opposite of a lattice, we will find that meets and joins have their roles interchanged. This is an abstract form of De Morgan's laws, or of duality applied to lattices.
 This is related to the duality between left and right multiplication. Examples include Polish notation.
 For a normal subgroup, the left cosets match the right cosets.
Duality: Bottomup and Topdown
 Coordinate systems can be organized "bottom up" or "top down". This yields the duality in projective geometry.
 Root systems relate reflections (hyperplanes) and root vectors. Given a root R, reflecting across its hyperplane, every root S is taken to another root S, and the difference between the two roots is an integer multiple of R. But this relates to the commutator sending the differences into the module based on R.
 Cotangent space and tangent space (or is this between covariant and contravariant?)
 For integers, decomposition into primes is a "bottom up" result which states that a typical number can be compactly represented as the product of its prime components. The "top down" result is that this depends on an infinite number of exceptions ("primes") for which this compact representation does not make them more compact.
 Duality of silence (topdown) and speaking (bottomup).
Duality: Complements
 Center and totality for a simplex and other infinite families of complex polytopes.
 Duality (projective geometry). Interchange the role of "points" and "lines" to get a dual truth: The plane dual statement of "Two points are on a unique line" is "Two lines meet at a unique point". (Compare with the construction of an equilateral triangle and the lattice of conditions.)
 Poincare duality states that if M is an ndimensional oriented closed manifold (compact and without boundary), then the kth cohomology group of M is isomorphic to the (n − k)th homology group of M, for all integers k. Verdier duality is a generalization.
 Twisted Poincaré duality is a theorem removing the restriction on Poincaré duality to oriented manifolds. The existence of a global orientation is replaced by carrying along local information, by means of a local coefficient system.
 Jordan curve theorem (separating the inside and outside of a curve) generalized by the Jordan–Brouwer separation theorem, generalized by Alexander duality about the Betti numbers of the simplicial complex, and in the modern statement, between the reduced homology or cohomology of a compact, locally contractible subspace X of a sphere and its complement Y, Hq(X) and Hnq1(Y). Generalized by Spanier–Whitehead duality. Sphere complements determine the homology, and the stable homotopy type, though not the homotopy type.
 Betadual space is a certain linear subspace of the algebraic dual of a sequence space.
 The RiemannRoch theorem relates the complex analysis of a connected compact Riemann surface with the surface's purely topological genus g, in a way that can be carried over into purely algebraic settings. First for Riemann surfaces, then for algebraic curves. Serre duality is present on nonsingular projective algebraic varieties V of dimension n (and in greater generality for vector bundles and further, for coherent sheaves). It shows that a cohomology group Hi is the dual space of another one, Hn−i. Coherent duality is a generalization applying to coherent sheaves. Grothendieck local duality is a duality theorem for cohomology of modules over local rings, analogous to Serre duality of coherent sheaves. The Grothendieck–Riemann–Roch theorem from about 1956 is usually cited as the key moment for the introduction of this circle of ideas. The more classical types of Riemann–Roch theorem are recovered in the case where S is a single point (i.e. the final object in the working category C). Using other S is a way to have versions of theorems 'with parameters', i.e. allowing for continuous variation, for which the 'frozen' version reduces the parameters to constants. In other applications, this way of thinking has been used in topos theory, to clarify the role of set theory in foundational matters. Assuming that we don’t have a commitment to one 'set theory' (all toposes are in some sense equally set theories for some intuitionistic logic) it is possible to state everything relative to some given set theory that acts as a base topos.
 In differential geometry, the Atiyah–Singer index theorem, proved by Michael Atiyah and Isadore Singer (1963), states that for an elliptic differential operator on a compact manifold, the analytical index (related to the dimension of the space of solutions) is equal to the topological index (defined in terms of some topological data). It includes many other theorems, such as the Riemann–Roch theorem, as special cases
 Dualizing sheaf.
 ArtinVerdier duality is a duality theorem for constructible abelian sheaves over the spectrum of a ring of algebraic numbers, introduced by Artin and Verdier (1964), that generalizes Tate duality. Tate duality or Poitou–Tate duality is a duality theorem for Galois cohomology groups of modules over the Galois group of an algebraic number field or local field.
 In Galois cohomology, local Tate duality (or simply local duality) is a duality for Galois modules for the absolute Galois group of a nonarchimedean local field. It is named after John Tate who first proved it. It shows that the dual of such a Galois module is the Tate twist of usual linear dual. This new dual is called the (local) Tate dual. Local duality combined with Tate's local Euler characteristic formula provide a versatile set of tools for computing the Galois cohomology of local fields. Tate duality is a version for global fields.
 The dualizing complex DX on X is defined to be ... where p is the map from X to a point. Part of what makes Verdier duality interesting in the singular setting is that when X is not a manifold (a graph or singular algebraic variety for example) then the dualizing complex is not quasiisomorphic to a sheaf concentrated in a single degree.
 The Hodge isomorphism or Hodge star operator is an important linear map introduced in general by W. V. D. Hodge. It is defined on the exterior algebra of a finitedimensional oriented vector space endowed with a nondegenerate symmetric bilinear form. The result when applied to an element is called the element's Hodge dual.
 Lefschetz duality is a version of Poincaré duality in geometric topology, applying to a manifold with boundary.
Duality: Complements: Plane duality
 Dual graph of a plane graph G is a graph that has a vertex for each face of G. The dual graph has an edge whenever two faces of G are separated from each other by an edge, and a selfloop when the same face appears on both sides of an edge.
 Dual polyhedron
 Tangents
 Dual curve of a given plane curve C is a curve in the dual projective plane consisting of the set of lines tangent to C. There is a map from a curve to its dual, sending each point to the point dual to its tangent line.
 Dual polygon: rectification; polar reciprocation (pole and polar); projective duality; combinatorially.
 Fenchel's duality theorem ... Fenchel's theorem states that the two problems have the same solution. The points having the minimum vertical separation are also the tangency points for the maximally separated parallel tangents.
 Stokes' theorem. Stokes' theorem is a vast generalization of the fundamental theorem of calculus, which states that the integral of a function f over the interval [a, b] can be calculated by finding an antiderivative F of f: General Stokes theorem: duality between the boundary operator on chains and the exterior derivative. Stokes' theorem says that the integral of a differential form ω over the boundary of some orientable manifold Ω is equal to the integral of its exterior derivative dω over the whole of Ω. Stokes' theorem says that this is a chain map from de Rham cohomology to singular cohomology with real coefficients; the exterior derivative, d, behaves like the dual of ∂ on forms. This gives a homomorphism from de Rham cohomology to singular cohomology.
Duality: Existing and nonexisting
 Switching of "existing" and "nonexisting", for example, edges in a graph. This underlies Ramsey's theorem. Tao: "the Ramseytype theorem, each one of which being a different formalisation of the newly gained insight in mathematics that complete disorder is impossible."
 Duality  parity  išsiaiškinimo rūšis
Intersections and Unions
 Stone duality are categorical dualities between certain categories of topological spaces and categories of partially ordered sets.
 The dual of the category of frames is called the category of locales and generalizes the category Top of all topological spaces with continuous functions. The consideration of the dual category is motivated by the fact that every continuous map between topological spaces X and Y induces a map between the lattices of open sets in the opposite direction as for every continuous function f: X → Y and every open set O in Y the inverse image f 1(O) is an open set in X.
 Jónsson–Tarski duality General frames bear close connection to modal algebras. ... In the opposite direction, it is possible to construct the dual frame ... A frame and its dual validate the same formulas, hence the general frame semantics and algebraic semantics are in a sense equivalent.
 Inclusionexclusion principle
 Esakia duality is the dual equivalence between the category of Heyting algebras and the category of Esakia spaces. Esakia duality provides an ordertopological representation of Heyting algebras via Esakia spaces.
 Alvis–Curtis duality is a duality operation on the characters of a reductive group over a finite field. Kawanaka introduced a similar duality operation for Lie algebras. The dual ζ* of a character ζ of a finite group G with a split BNpair is defined to be...
Generated by complements
 De Groot dual of a topology τ on a set X is the topology τ* whose closed sets are generated by compact saturated subsets of (X, τ). Saturated subset is an intersection of open subsets.
External, Explicit Dualities
Duality: Functionals
 Vectors and covectors. A vector is 1dimensional and a covector is n1 dimensional hyperplane (tangent plane), see Penrose chapter 12.
 A dual vector space (or just dual space for short) consisting of all linear functionals on V, together with the vector space structure of pointwise addition and scalar multiplication by constants.
 Internal vs. external geometry = implicit vs. embedding = vector space vs. dual space (functionals)
 dual set is a set B∗ of vectors in the dual space V∗ with the same index set I such that B and B∗ form a biorthogonal system. The dual set is always linearly independent but does not necessarily span V∗. If it does span V∗, then B∗ is called the dual basis or reciprocal basis for the basis B.
 Dual basis in a field extension
 Dual bundle of a vector bundle π : E → X is a vector bundle π∗ : E∗ → X whose fibers are the dual spaces to the fibers of E.
 Grothendieck's relative point of view studies and object X by considering instead morphisms f: X → S where S is a fixed object. This idea is made formal in the idea of the slice category of objects of C 'above' S. To move from one slice to another requires a base change; from a technical point of view base change becomes a major issue for the whole approach (see for example Beck–Chevalley conditions). A base change 'along' a given morphism g: T → S is typically given by the fiber product, producing an object over T from one over S.
 Pontryagin duality of a locally compact abelian group G is the group given by maps (characters) from it to the circle group T. The reciprocal lattice is related to this.
 Tannaka–Krein duality theory concerns the interaction of a compact topological group and its category of linear representations. It is a natural extension of Pontryagin duality, between compact and discrete commutative topological groups, to groups that are compact but noncommutative. ... In contrast to the case of commutative groups considered by Lev Pontryagin, the notion dual to a noncommutative compact group is not a group, but a category Π(G) with some additional structures, formed by the finitedimensional representations of G. The idea of Tannaka–Krein duality: category of representations of a group. A generalization of Tannaka–Krein theory provides the natural framework for studying representations of quantum groups, and is currently being extended to quantum supergroups, quantum groupoids and their dual Hopf algebroids.
 Given the lattice of characters of a maximal torus, the dual lattice is given by the 1parameter subgroups.
 The Langlands program seeks to relate Galois groups in algebraic number theory to automorphic forms and representation theory of algebraic groups over local fields and adeles.
 The Langlands conjectures imply, very roughly, that if G is a reductive algebraic group over a local or global field, then there is a correspondence between "good" representations of G and homomorphisms of a Galois group (or Weil group or Langlands group) into the Langlands dual group of G. A more general formulation of the conjectures is Langlands functoriality, which says (roughly) that given a (well behaved) homomorphism between Langlands dual groups, there should be an induced map between "good" representations of the corresponding groups. To make this theory explicit, there must be defined the concept of Lhomomorphism of an Lgroup into another. That is, Lgroups must be made into a category, so that 'functoriality' has meaning. The definition on the complex Lie groups is as expected, but Lhomomorphisms must be 'over' the Weil group.
 Geometric Langlands duality from six dimensions Edward Witten
 Langlands program. An Elementary Introduction to the Langlands Program by Stephen Gelbart.Langland Frenkel. 6D (2,0) superconformal field theory.
 Dual object is a category theory generalization of the concept of dual space in linear algebra.
 When dealing with topological vector spaces, one is typically only interested in the continuous linear functionals from the space into the base field F = C or R. A Continuous dual space or topological dual is a linear subspace of the algebraic dual space V and V'. For any finitedimensional normed vector space or topological vector space, such as Euclidean nspace, the continuous dual and the algebraic dual coincide.
 In functional analysis and related areas of mathematics a dual topology is a locally convex topology on a dual pair, two vector spaces with a bilinear form defined on them, so that one vector space becomes the continuous dual of the other space. The different dual topologies for a given dual pair are characterized by the Mackey–Arens theorem. All locally convex topologies with their continuous dual are trivially a dual pair and the locally convex topology is a dual topology.
 A dual pair or dual system is a pair of vector spaces with an associated bilinear map to the base field. A dual pair generalizes this concept of continuous dual to arbitrary vector spaces, with the duality being expressed as a bilinear map. Using the bilinear map, semi norms can be constructed to define a polar topology on the vector spaces and turn them into locally convex spaces, generalizations of normed vector spaces.
 A dual wavelet is the dual to a wavelet. In general, the wavelet series generated by a square integrable function will have a dual series, in the sense of the Riesz representation theorem. The Hilbert space representation theorem establishes an important connection between a Hilbert space and its (continuous) dual space. If the underlying field is the real numbers, the two are isometrically isomorphic; if the underlying field is the complex numbers, the two are isometrically antiisomorphic. The (anti) isomorphism is a particular, natural one.
 The Riesz–Markov–Kakutani representation theorem relates linear functionals on spaces of continuous functions on a locally compact space to measures.
 The dual space X' of a stereotype space is defined as the space of all linear continuous functionals f : X → C endowed with the topology of uniform convergence on totally bounded sets in X.
 Dual abelian variety can be defined from an abelian variety A, defined over a field K. To an abelian variety A over a field k, one associates a dual abelian variety Av (over the same field), which is the solution to the following moduli problem. ... the points of Av correspond to line bundles of degree 0 on A, so there is a natural group operation on Av given by tensor product of line bundles, which makes it into an abelian variety. There is a general form of duality between the Albanese variety of a complete variety V, and its Picard variety.
 Weil pairing is generalized by Cartier duality, which is an analogue of Pontryagin duality for noncommutative schemes.
Duality: Actions and Objects
 We can look at the operators that act or the objects they act upon. This brings to mind the two representations of the foursome.
 The Yoneda Lemma gives our connection to Why, and collapsing a network's node or relating it to its arrows. Relationship with Why as given by the eightfold way.
Duality: Adjunction
 Adjoint bendrai ir Adjoint functors. The minimialistic solution  the maximalist problem solved. The most efficient solution  the most difficult problem solved. Wikipedia: It can be said that an adjoint functor is a way of giving the most efficient solution to some problem via a method which is formulaic. A construction is most efficient if it satisfies a universal property, and is formulaic if it defines a functor. Universal properties come in two types: initial properties and terminal properties. Since these are dual (opposite) notions, it is only necessary to discuss one of them.
 A functor F : C ← D is a left adjoint functor if for each object X in C, there exists a terminal morphism from F to X. A functor G : C → D is a right adjoint functor if for each object Y in D, there exists an initial morphism from Y to G.
 A counit–unit adjunction between two categories C and D consists of two functors F : C ← D and G : C → D and two natural transformations...
 A homset adjunction between two categories C and D consists of two functors F : C ← D and G : C → D and a natural isomorphism...
 Example of adjoint functors Given inclusion i:Z>R, with morphism x>y in R whenever x<=y, then the right adjoint is the floor function and the left adjoint is the ceiling function. A pair of adjoint functors is what is needed to make two categories compatible in their objects and morphisms.
 A very general comment of William Lawvere is that syntax and semantics are adjoint: take C to be the set of all logical theories (axiomatizations), and D the power set of the set of all mathematical structures. For a theory T in C, let F(T) be the set of all structures that satisfy the axioms T; for a set of mathematical structures S, let G(S) be the minimal axiomatization of S. We can then say that F(T) is a subset of S if and only if T logically implies G(S): the "semantics functor" F is left adjoint to the "syntax functor" G. Peter Smith. The Galois Connection between Syntax and Semantics.
 division is (in general) the attempt to invert multiplication, but many examples, such as the introduction of implication in propositional logic, or the ideal quotient for division by ring ideals, can be recognised as the attempt to provide an adjoint.
 Tensor products are adjoint to a set of homomorphisms.
 The two facts that this method of turning rngs into rings is most efficient and formulaic can be expressed simultaneously by saying that it defines an adjoint functor. Continuing this discussion, suppose we started with the functor F, and posed the following (vague) question: is there a problem to which F is the most efficient solution? The notion that F is the most efficient solution to the problem posed by G is, in a certain rigorous sense, equivalent to the notion that G poses the most difficult problem that F solves.
 Consider an object Y in a category with pullbacks. Any morphism f : X → Y induces a functor f ∗ : Sub ( Y ) ⟶ Sub ( X ) on the category that is the preorder of subobjects. It maps subobjects T of Y (technically: monomorphism classes of T → Y to the pullback X × Y T ). If this functor has a left or right adjoint, they are called ∃ f and ∀ f, respectively.[3] They both map from Sub ( X ) back to Sub ( Y ) . Very roughly, given a domain S ⊂ X to quantify a relation expressed via f over, the functor/quantifier closes X in X × Y T and returns the thereby specified subset of Y.
Duality: Reversing the maps
 Dual (category theory)
 Opposite category. Morphisms can be organized from left to right or from right to left. The opposite category turns all of the arrows around.
 If a category is equivalent to the opposite (or dual) of another category then one speaks of a duality of categories, and says that the two categories are dually equivalent.
 Colimits and limits
 Monomorphisms ("onetoone") and epimorphisms (forcing "onto").
 Coproducts and products
 Initial and terminal objects
 Covariance and contravariance
 Wikipedia: Fibrations and cofibrations are examples of dual notions in algebraic topology and homotopy theory. In this context, the duality is often called Eckmann–Hilton duality.
 Every isomorphism is a duality in that it goes hand in hand with its inverse. If the domain and codomain are the same, then it is selfdual.
 Duality (order theory). Every partially ordered set P gives rise to a dual (or opposite) partially ordered set which is often denoted by Pop or Pd. This dual order Pop is defined to be the set with the inverse order. Dual properties:
 Greatest elements and least elements
 Maximal elements and minimal elements
 Least upper bounds (suprema, ∨) and greatest lower bounds (infima, ∧)
 Upper sets and lower sets
 Ideals and filters
 Closure operators and kernel operators.
 Selfdual notions:
 Being a (complete) lattice
 Monotonicity of functions
 Distributivity of lattices, i.e. the lattices for which ∀x,y,z: x ∧ (y ∨ z) = (x ∧ y) ∨ (x ∧ z) holds are exactly those for which the dual statement ∀x,y,z: x ∨ (y ∧ z) = (x ∨ y) ∧ (x ∨ z) holds
 Being a Boolean algebra
 Being an order isomorphism.
 Since partial orders are antisymmetric, the only ones that are selfdual are the equivalence relations.
Duality: Reversing the ordering
 Wikipedia: Reversing the direction of inequalities in a partial order. (Partial orders correspond to a certain kind of category in which Hom(A,B) can have at most one element.)
 Analysis provides lower and upper bounds on a function or phenomenon which helps define the geometry of this space.
Other
 Araki duality for free fields: the commuting algebra of the local algebra of a region O in spacetime is equal to the local algebra of the set of points that are spacelike separated from O.
Mathematics: Almost Duality  Duality Breaking
The duality between zero and infinity, between nothing and everything, is broken in many subtle ways. Here are some examples:
 By definition, a topological space includes both an entire set X and the empty set. However, the intermediary sets are closed under arbitrary unions, but only finite intersections. What would happen if they were closed under infinite intersections?
 Perhaps similarly, having in mind the Zariski topology, ideals of a ring are defined with respect to multiplication (union) but not addition (intersection).
 Meromorphic function is the quotient of two holomorphic functions, thus compares them.
Dual values
 Usually the term "dual problem" refers to the Lagrangian dual problem but other dual problems are used, for example, the Wolfe dual problem and the Fenchel dual problem.
 In Wolfe duality, the objective function and constraints are all differentiable functions. Using this concept a lower bound for a minimization problem can be found because of the weak duality principle.
 In mathematical optimization theory, duality or the duality principle is the principle that optimization problems may be viewed from either of two perspectives, the primal problem or the dual problem. The solution to the dual problem provides a lower bound to the solution of the primal (minimization) problem.[1] However in general the optimal values of the primal and dual problems need not be equal. Their difference is called the duality gap. For convex optimization problems, the duality gap is zero under a constraint qualification condition.
 The duality gap is the difference between the values of any primal solutions and any dual solutions. The duality gap is zero if and only if strong duality holds. Otherwise the gap is strictly positive and weak duality holds.
 In computational optimization, another "duality gap" is often reported, which is the difference in value between any dual solution and the value of a feasible but suboptimal iterate for the primal problem. This alternative "duality gap" quantifies the discrepancy between the value of a current feasible but suboptimal iterate for the primal problem and the value of the dual problem; the value of the dual problem is, under regularity conditions, equal to the value of the convex relaxation of the primal problem
Mathematical Tension: Equivalence and Uniqueness
In Math, there is an everpresent tension between the notions of equivalence class and uniqueness. If something is mathematically significant, it should in some sense be unique. But math is a model and so, as such, can never be entirely unique but represents a variety of cases. Thus it is ever natural to define equivalence classes, especially in math itself. For example, a rational number is an equivalence class that establishes a proportion.
Ways of figuring things out
 Duality of the deep and the broad.
 Įvairios simetrijos  išsiaiškinimo būdų sandaros.
Duality in Physics
Duality in Mathematics and Physics by Sir Michael Atiyah
Conjugation
Complements
 Sduality strong coupling  weak coupling. Realizations include Seiberg duality, Montonen–Olive duality, Generalizes Maxwell duality. Anton Kapustin and Edward Witten suggested that the geometric Langlands correspondence can be viewed as a mathematical statement of Montonen–Olive duality.
Functionals
More:
The transpose of a linear map between two vector spaces, defined over the same field, is an induced map between the dual spaces of the two vector spaces
Duality breaking
 Duality breaking allows that God is good and not bad. Because we want to break the duality of good and bad, increasing and decreasing slack. Orientation is a complete, absolute, total distinction between inside and outside, their complete segregation and isolation. (In contrast to the yinyang symbol.) So it is highly tenuous  it can break at any single point  but it can eternally grow more weighty.
 Duality breaking (for slack)  disconnecting the local and the global  for example, defining locally Euclidean spaces  in lattice terms, as a consequence of limiting processes, disconnecting the inf from the sup, breaking their duality.
 The CayleyDickson construction is all about duality breaking. It thereby yields noncommutativity, nonassociativity, etc.
 A vector is 1dimensional (and its dimension) and its covector is n1 dimensional (it is normal to the vector). In this sense they complement each other.
 Vectors are described in terms of partial derivatives (based on the local coordinate systems) whereas covectors are described in terms of (total) forms dx.
 Inner products are sesquilinear  they have conjugate symmetry  so as not to yield lopsided answers. If they yield a complex root as an answer, then one version should yield one root and the other version should yield the other root. In other words, in a complex field, the inner product should be thought of as yielding two answers  both answers  distinguished by the notation, leftright or rightleft.
 Kai užsimirštame, kai žinojimas tampa nežinojimu (pavyzdžiui, metant monetą) tada iškyla jungtinės priešingybės (conjugates).
 Electrical duality Topology and Elementary Electric Circuit Theory, II: Duality Tony Phillips
Note that turns left and right are conjugates but not a division of everything because there can be no turn. Instead, the twosome is "turn" (left/right) and "noturn". "Turn" does not need to be marked, but "noturn" needs to be marked ("no"). Although, contentwise, notturning is unmarked and turning is marked.
This duality between compact and noncompact symmetric spaces is a generalization of the well known duality between spherical and hyperbolic geometry. Wikipedia: List of simple Lie groups: Symmetric spaces
Tannaka duality
Cohomology at nLab: Cohomology is dual to homotopy (as an operation): the cohomology of X with coefficients in A is the homotopy of A with cocoefficients in X. Cohomology should be thought of as "cohomotopy". For any {$A\in H$} the set {$H(S^n,A)$} is equivalently:
 the Acohomology of {$S^n$}
 the nth homotopy group of A
Examples in Math Companion:
 Platonic solids
 Points and lines in the projective plane
 Sets and their complements
 Dual vector spaces
 Polar bodies
 Duals of Abelian groups
 Homology and cohomology
 Differential forms: kforms and kdimensional surfaces
 Distributions: ...
 Mirror symmetry: (conjectural) CalabiYau manifolds and mirror manifolds
 Fourier transform?
 Representation theory: Langlands dual of certain nonAbelian groups
Another key concept for me is the idea of an "unmarked opposite" vs. a "marked opposite".
 We can have what is beyond a system be identified with an opposite within the system. For example, a blank sheet of paper can be noted by the empty set. The empty set is opposite to nonempty sets. And there is a sense in which the empty set is preferred, is central. Or we can have the identity element of a group which expresses no action at all. Similarly, good can be distinguished from bad by claiming that God is good, where God is what is beyond the system. So here in this sense I say that good is the marked opposite, the one identified with what is beyond the system.
 Also, in a different sense, in a system, a marked opposite is when you have two opposites (choices) that are clearly distinguished and one is the default (thus preferred) because it is unmarked, whereas the other one is marked to distinguish it and thus secondary. For example, 1 and 1. 1 is unmarked and 1 is marked (and it actually has an extra mark). And they are clearly distinct: 1 x 1 = 1 whereas 1 x 1 = 1.
 Finally, we can have "unmarked opposites" where two choices are distinct but otherwise not distinguishable. They have yet to be marked. For example, the two square roots of 1. One will imagined clockwise, the other counterclockwise, perhaps. But which is which doesn't matter. Only when we name them using + and , only when we attribute such a prejudice to them, do we lose touch with their original indistinguishability, thus ending up with i and i, forgetting that i is no less basic than +i.
So I'm very interested where such dualities and opposites come up in math.
Unmarked opposite
 turinys = raiška. "Those things are which show themselves to be." buvimo pagrindas
 inner 2cycle, kurio paprastai nebūna.
 complex numbers i=j iš kurio atsiveria 1<>1, i<>i. Paprastai i > j > i ... banguoja, o šitą sustabdžius gaunasi +1 +1 +1 +1 amžinai ir atitinkamai 1111 amžinai.
Notes
Duality
 Duality of nonrelevance in system (kernel) and nonrelevance beyond system (cokernel).
 Compare the kinds of dualities with the kind of transformations of perspectives and then with the kinds of geometric transformations.
 In the automata hierarchy, consider how to model duality of internal structure and external network.
 Duality of vectors and covectors (linear functionals)  flipsides of composition  what is "inside" and "outside" the composer.
 Conjugates can be thought of as "twins", whereas +1 and 1 are "spouses".
 Conjugate = mystery = false. (Hidden distinction).
 i>j is asymmetric, onedirectional. i<>i* is symmetric, twodirectional, breaks antisymmetry, hides antisymmetry (which is i and which is j?)
 Algebra  geometry duality. (Pullback). Morphism <> ring homomorphism. Intrinsic and extrinsic geometry. Ambient space. Relation between two spaces. Varieties [morphisms X to Y] <> Affine Falgebras [Flinear ring homomorphisms F[Y] to F[x]]
 Study the idea behind linear functionals, fundamental representations, eigenvectors, cohomology, and other maps into one dimension.
 Duality examples (conjugates)
 complex number "i" is not one number  it is a pair of numbers that are the square roots of 1
 spinors likewise
 Dn where n=2
 the smallest crosspolytope with 2 vertices
 taking a sphere and identifying antipodal elements  this is a famous group
 polar conjugates in projective geometry (see Wildberger)
 Study how Set breaks duality (the significance of initial and terminal objects).
 Each physical force is related to a duality:
 Charge (matter and antimatter)  electromagnetism
 Weak force  time reversal
 So the types of duality should give the types of forces.
 John Baez on duality: Dyson's Threefold Way: either X is not isomorphic to its dual (the complex case), or it is isomorphic to its dual (in the real or quaternionic cases). Study his slides!
 John Baez on duality in logic and physics
 Algebra (of the observer) and analysis (of the observed) exhibit a duality of worldviews.
 The interpretation {$\mathbb{C} \leftrightarrow \mathbb{R}^2$} gives meaning to the two axes. One axis the opposites 1 and 1 and the other axis is the opposites i and j. And they become related 1 to i to 1 to j. Thus multiplication by i is rotation by 90 degrees. It returns us not to 1 but sends us to 1.
 Composition algebra. Doubling is related to duality.
 Linear functionals. Onedimensional economic thinking is like linear functionals  the dual space of the multidimensional reality. In finite dimensions, the dual dual is the same as what we started. But in infinite dimensions not necessarily. Does this suggest that our life is infinitedimensional, which is to say, it can't be captured by a onedimensional shadow?
Opposites
 Exercise: Find all matrices with eigenvalues 1 and 1. {$\lambda=\frac{a_{11}+a_{22} \pm \sqrt{(a_{11}+a_{22})^2  4A}}{2}$} so A=1. {$\begin{pmatrix} \pm \sqrt{1 + a_{12}a_{21}} & a_{12} \\ a_{21} & \mp \sqrt{1 + a_{12}a_{21}} \end{pmatrix}$} such as {$\begin{pmatrix} 0 & 1 \\ 1 & 0 \end{pmatrix}$}{$\begin{pmatrix} i & 0 \\ 0 & i \end{pmatrix}${$\begin{pmatrix} 0 & i \\ i & 0 \end{pmatrix}$}
 Multiplying by {$\begin{pmatrix} x \\ y \end{pmatrix}$} yields three ways of coding opposites: {$\begin{pmatrix} iy \\ ix \end{pmatrix}$} {$\begin{pmatrix} y \\ x \end{pmatrix}$} {$\begin{pmatrix} ix \\ iy \end{pmatrix}$} where in each case two of three are applied: flipping, multiplying by i, multiplying by 1.
 Adjunction is a form of duality.
 Equality and equivalence, in general, are forms of duality.
 Duality is an extension of equivalence where the two sides of the equation are somehow different. For example, one side may be a variable and the other side a value that it is set to.
 Conjugates i and j are the form of duality that is the same as equality. Except that they are not identified as such.
 Duality (opposites coexist) and equality (all is the same) form a duality, as in the twosome.

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