PlanetPhysics/Homotopy Double Groupoid 2

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Homotopy double groupoid of a Hausdorff space

Let X be a Hausdorff space. Also consider the [[../InfinityGroupoid/|HDA]] [[../PreciseIdea/|concept]] of a [[../HigherDimensionalAlgebraHDA/|double groupoid]], and how it can be completely specified for a Hausdorff space, X. Thus, in ref. [1] Brown et al. associated to X a double groupoid, ρ2(X) , called the homotopy double groupoid of X which is completely defined by the data specified in Definitions 0.1 to 0.3 in this entry and related [[../TrivialGroupoid/|objects]].

Generally, the geometry of [[../PiecewiseLinear/|squares]] and their [[../Cod/|compositions]] leads to a common [[../CategoricalGroupRepresentation/|representation]] of a double groupoid in the following form:

Failed to parse (unknown function "\D"): {\displaystyle (1) \D = \vcenter{\xymatrix @=3pc {S \ar @<1ex> [r] ^{s^1} \ar @<-1ex> [r] _{t^1} \ar @<1ex> [d]^{\, t_2} \ar @<-1ex> [d]_{s_2} & H \ar[l] \ar @<1ex> [d]^{\,t} \ar @<-1ex> [d]_s \\ V \ar [u] \ar @<1ex> [r] ^s \ar @<-1ex> [r] _t & M \ar [l] \ar[u]}}, }

where M is a set of `points', H,V are `horizontal' and `vertical' [[../GroupoidHomomorphism2/|groupoids]], and S is a set of `squares' with two compositions.

The laws for a double groupoid are also defined, more generally, for any [[../CoIntersections/|topological]] space 𝕋, and make it also describable as a groupoid internal to the [[../GroupoidCategory/|category of groupoids]]. Further details of this general definition are provided next.

Given two groupoids H,V over a set M, there is a double groupoid (H,V) with H,V as horizontal and vertical edge groupoids, and squares given by quadruples \bigbreak

Failed to parse (unknown function "\begin{pmatrix}"): {\displaystyle \begin{pmatrix} & h& \<blockquote><math>-0.9ex] v & & v'\<blockquote><math>-0.9ex]& h'& \end{pmatrix} }

for which we assume always that h,hH,v,vV and that the initial and final points of these edges match in M as suggested by the notation, that is for example </math>sh=sv, th=sv', \ldots,etc.Thecompositionsaretobeinheritedfromthoseof<math>H,V, that is: \bigbreak

Failed to parse (unknown function "\quadr"): {\displaystyle \quadr{h}{v}{v'}{h'} \circ_1\quadr{h'}{w}{w'}{h''} =\quadr{h}{vw}{v'w'}{h''}, \;\quadr{h}{v}{v'}{h'} \circ_2\quadr{k}{v'}{v''}{k'}=\quadr{hk}{v}{v''}{h'k'} ~. }

Alternatively, the data for the above double groupoid Failed to parse (unknown function "\D"): {\displaystyle \D} can be specified as a triple of groupoid structures: (D2,D1,1,1+,+1,ε1),(D2,D1,2,2+,+2,ε2),(D1,D0,1,1+,+,ε),

where: D0=M,D1=V=H,D2=S, s1=2,t1=2+,s2=s=1 and t2=t=1+. Then, as a first step, consider this data for the homotopy double groupoid specified in the following definition; in order to specify completely such data one also needs to define the related concepts of thin equivalence and the relation of cubically thin homotopy , as provided in the two definitions following the homotopy double groupoid data specified above and in the (main) Definition 0.1.

The data for the homotopy double groupoid, ρ(X), will be denoted by :

Failed to parse (unknown function "\begin{matrix}"): {\displaystyle \begin{matrix} (\boldsymbol{\rho}^{\square}_2 (X), \boldsymbol{\rho}_1^{\square} (X) , \partial^{-}_{1} , \partial^{+}_{1} , +_{1} , \varepsilon _{1}) , \boldsymbol{\rho}^{\square}_2 (X), \boldsymbol{\rho}^{\square}_1 (X) , \partial^{-}_{2} , \partial^{+}_{2} , +_{2} , \varepsilon _{2})\<blockquote><math>3mm] (\boldsymbol{\rho}^{\square}_1 (X) , X , \partial^{-} , \partial^{+} , + , \varepsilon). \end{matrix}}

\bigbreak

Here ρ1(X) denotes the path groupoid of X from ref. [2] where it was defined as follows. The objects of ρ1(X) are the points of X. The [[../TrivialGroupoid/|morphisms]] of ρ1(X) are the equivalence classes of paths in X with respect to the following (thin) [[../TrivialGroupoid/|equivalence relation]] T, defined as follows. The data for ρ2(X) is defined last; furthermore, the symbols specified after the [[../PiecewiseLinear/|thin square]] symbol specify both the sides (or the groupoid `dimensions') of the square which are involved (i.e., 1 and 2, respectively), and also the order in which the shown [[../Cod/|operations]] (1, ε2... , etc) are to be performed relative to the thin square specified for each groupoid, ρ1orρ2; moreover, all such symbols are explicitly and precisely defined in the related entries of the concepts involved in this definition. These two groupoids can also be pictorially represented as the (H,V) pair depicted in the large [[../TrivialGroupoid/|diagram]] (0.1), or Failed to parse (unknown function "\D"): {\displaystyle \D} , shown at the top of this page.

Thin Equivalence

Let a,a:xy be paths in X. Then a is thinly equivalent to a, denoted aTa, if there is a thin relative homotopy between a and a.

We note that T is an equivalence relation, see [1]. We use a:xy to denote the T class of a path a:xy and call a<math>theπ‘ π‘’π‘šπ‘–π‘‘π‘Ÿπ‘Žπ‘π‘˜of a </math>. The groupoid structure of ρ1(X) is induced by concatenation, +, of paths. Here one makes use of the fact that if a:xx, a:xx, a:xx are paths then there are canonical thin relative homotopies

Failed to parse (unknown function "\begin{matrix}"): {\displaystyle \begin{matrix}{r} (a+a') + a'' \simeq a+ (a' +a'') : x \simeq x''' \ ({\it rescale}) \\ a+e_{x'} \simeq a:x \simeq x' ; \ e_{x} + a \simeq a: x \simeq x' \ ({\it dilation}) \\ a+(-a) \simeq e_{x} : x \simeq x \ ({\it cancellation}). \end{matrix} }

The source and [[../SmallCategory/|target maps]] of ρ1(X) are given by Failed to parse (unknown function "\enskip"): {\displaystyle \partial^{-}_{1} \langle a\rangle =x,\enskip \partial^{+}_{1} \langle a\rangle =y,} if a:xy is a semitrack. [[../Cod/|Identities]] and inverses are given by ε(x)=exresp.a=a.

At the next step, in order to construct the groupoid ρ2(X) data in Definition 0.1, R. Brown et al. defined as follows a \htmladdnormallink{relation {http://planetphysics.us/encyclopedia/Bijective.html} of [[../CubicallyThinHomotopy2/|cubically thin homotopy]]} on the set R2(X) of squares.

Cubically Thin Homotopy

Let u,u be squares in X with common vertices.

  1. A {\it cubically thin homotopy} U:uTu

between u and u is a cube UR3(X) such that

(i) U is a homotopy between u and u,

i.e. Failed to parse (unknown function "\enskip"): {\displaystyle \partial^{-}_1 (U)=u,\enskip \partial^{+}_1 (U)=u',}

(ii) U is rel. vertices of I2,

i.e. Failed to parse (unknown function "\enskip"): {\displaystyle \partial^{-}_2\partial^{-}_2 (U),\enskip\partial^{-}_2 \partial^{+}_2 (U),\enskip \partial^{+}_2\partial^{-}_2 (U),\enskip\partial^{+}_2 \partial^{+}_2 (U)} are

constant,

(iii) the faces iα(U) are thin for α=±1, i=1,2.

  1. The square u is {\it cubically} T-{\it equivalent} to

u, denoted uTu if there is a cubically thin homotopy between u and u.

By removing from the above double groupoid construction the condition that all morphisms must be invertible one obtains the prototype of a [[../HorizontalIdentities/|double category]].

All Sources

[2] [1]

References

  1. ↑ 1.0 1.1 1.2 R. Brown, K.A. Hardie, K.H. Kamps and T. Porter., A homotopy double groupoid of a Hausdorff space , {\it Theory and Applications of Categories} 10 ,(2002): 71-93.
  2. ↑ 2.0 2.1 K.A. Hardie, K.H. Kamps and R.W. Kieboom., A homotopy 2-groupoid of a Hausdorff Applied Categorical Structures , 8 (2000): 209-234.

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