PlanetPhysics/Superalgebroids in Higher Dimensions
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Definitions of double, and higher dimensional algebroids, superalgebroids and generalized superalgebras.
Double algebroids
A double --algebroid consists of a
double category , as detailed in ref.[1], such that each [[../IndexOfCategories/|category structure]] has the additional structure of an --algebroid. More precisely, a double [[../RAlgebroid/|--algebroid]] Failed to parse (unknown function "\D"): {\displaystyle \D} involves four related [[../RAlgebroid/|--algebroids]]:
Failed to parse (unknown function "\del"): {\displaystyle (D,D_1,\del^0_1 ,\del^1_1 , \vep_1 , +_1 , \circ _1 , ._1) ,\qquad &(D,D_2,\del^0_2 , \del ^1_2 , \vep_2 , +_2 , \circ _2 , ._2 )\\ (D_1,D_0, \delta^0_1 ,\delta^1_1 , \vep , + , \circ , .) ,\qquad &(D_2 , D_0 , \delta^0_2 , \delta^1_2 , \vep , + , \circ , .) } that satisfy the following rules:
\item[i)] Failed to parse (unknown function "\del"): {\displaystyle \delta^i_2 \del^j_2 = \delta ^j_1 \del ^i_1}
for </math>i,j \in \{0,1\}Failed to parse (unknown function "\med"): {\displaystyle \med \item[ii)] <math> \del^i_2 ( \a +_1 \be) = \del^i_2\a +\del^i_2\be , \qquad &\del^i_1 ( \a +_2 \be) = \del^i_1 \a +\del^i_1\be \\ \del^i_2 ( \a \circ _1 \be) = \del^i_2 \a \circ \del^i_2 \be ,\qquad & \del^i_1 (\a \circ _2 \be ) = \del^i_1\a \circ \del^i_1\be }
for Failed to parse (unknown function "\a"): {\displaystyle i = 0,1 , \a,\be \in D}
and both sides are defined. \med \item[iii)] Failed to parse (unknown function "\a"): {\displaystyle r ._1 (\a+_2 \be) = (r ._1 \a) +_2 (r ._1\be ) ,\qquad & r ._2 (\a +_1 \be ) = (r ._2 \a ) +_1 (r ._2\be )\\ r ._1 (\a \circ _2 \be ) = (r ._1\a ) \circ _2 (r ._1 \be ) , \qquad & r ._2 (\a \circ _1 \be ) = (r ._2 \a ) \circ _1 (r ._2\be )\\ r ._1 ( s ._2 \be ) &= s ._2 ( r._1 \be ) }
for all Failed to parse (unknown function "\a"): {\displaystyle \a ,\be \in D, ~r,s \in R}
and both sides are defined. \med \item[iv)] Failed to parse (unknown function "\a"): {\displaystyle (\a +_1 \be ) +_2 (\gamma +_1 \lambda )& = (\a +_2 \gamma ) +_1 (\be +_2 \lambda ) ,\\ (\a \circ _1 \be ) \circ _2 (\gamma \circ _1 \lambda )& = (\a \circ _2 \gamma ) \circ _1 (\be \circ _2 \lambda )\\ (\a +_i \be ) \circ _j (\gamma +_i \lambda ) &= (\a \circ _j \gamma ) +_i (\be \circ _j \lambda ) }
for , whenever both sides are defined.
The definition of a double algebroid specified above was introduced by Brown and Mosa [2]. Two [[../TrivialGroupoid/|functors]] can be then constructed, one from the [[../Cod/|category]] of double algebroids to the category of [[../CubicalHigherHomotopyGroupoid/|crossed modules]] of [[../Algebroids/|algebroids]], whereas the reverse functor is the unique adjoint (up to [[../IsomorphismClass/|natural equivalence]]). The construction of such functors requires the following definition.
Category of double algebroids
A morphism Failed to parse (unknown function "\D"): {\displaystyle f : \D \to \E} of double algebroids is then defined as a [[../TrivialGroupoid/|morphism]] of truncated cubical sets which [[../Commutator/|commutes]] with all the algebroid structures. Thus, one can construct a category of double algebroids and their morphisms. The main construction in this subsection is that of two functors from this category to the category of crossed modules of algebroids.
Let be a double algebroid. One can associate to a crossed module Failed to parse (unknown function "\lra"): {\displaystyle \mu : M \lra {D}_1} . Here will consist of elements of with [[../PiecewiseLinear/|boundary]] of the form: 0 1 Failed to parse (unknown function "\del"): {\displaystyle \del m = \quadr{a}{1_y}{1_x}{ 0_{xy}}~, } that is </math>M(x,y) = \{ m \in D : \del^1_1 m = 0_{xy} , \del^0_2 m = 1_x,\del^1_2 m = 1_y \}--algebroid and superalgebroid are however quite distinct from those of double, cubic,..., n--tuple algebroid, and have technically less complicated definitions.