algebroid structures and extended symmetries
0.1 Algebroid Structures and Algebroid Extended Symmetries
Definition 0.1.
An algebroid structure will be specifically defined to meaneither a ring, or more generally, any of the specifically defined algebras, but with severalobjects instead of a single object, in the sense specified by Mitchell(1965). Thus, an algebroid has been defined (Mosa, 1986a; Brown and Mosa 1986b, 2008)as follows. An -algebroid on a set of “objects” is a directed graph
over such that for each has an -module structure
and there is an -bilinearfunction
called “composition” and satisfying theassociativity condition, and the existence of identities
.
Definition 0.2.
A pre-algebroid has the same structure as an algebroid and the sameaxioms except for the fact that the existence of identities is not assumed. For example, if has exactly one object, thenan -algebroid over is just an -algebra. An idealin is then an example of a pre-algebroid.
Let be a commutative ring. An -category is a category equipped with an -module structure on each hom set such that the composition is -bilinear. More precisely, let us assume for instance that we are given a commutative ring with identity. Then a small -category–or equivalently an -algebroid– will be defined as a category enriched in the monoidal category of -modules, with respect to themonoidal structure of tensor product. This means simply that for all objects of , the set is given the structure of an -module, and composition is –bilinear, or is a morphism
of -modules .
If is a groupoid (http://planetmath.org/Groupoids) (or, more generally, a category)then we can construct an -algebroid asfollows. The object set of is the same as that of and is the free -module on theset , with composition given by the usualbilinear rule, extending the composition of .
Alternatively, one can define to be theset of functions with finite support, andthen we define the convolution product
as follows:
(0.1) |
As it is very well known, only the second construction is naturalfor the topological case, when one needs to replace ‘function’ by‘continuous function with compact support’ (http://planetmath.org/SmoothFunctionsWithCompactSupport) (or locallycompact support
for the QFT (http://planetmath.org/QFTOrQuantumFieldTheories) extendedhttp://planetmath.org/?op=getobj&from=books&id=153symmetry
sectors), and inthis case . The point made here isthat to carry out the usual construction and end up with only an algebrarather than an algebroid, is a procedure analogous to replacing agroupoid (http://planetmath.org/Groupoids) by a semigroup in which thecompositions not defined in are defined to be in . Weargue that this construction removes the main advantage ofgroupoids (http://planetmath.org/Groupoids), namely the spatial component given by the set ofobjects.
Remarks:One can also define categories of algebroids, -algebroids, double algebroids , and so on.A ‘category’ of -categories is however a super-category (http://planetmath.org/Supercategory) , or it can also be viewed as a specific example of a metacategory (http://planetmath.org/AxiomsOfMetacategoriesAndSupercategories) (or-supercategory, in the more general case of multiple operations
–categorical ‘composition laws’– being defined within the same structure, for the same class, ).
References
- 1 I. C. Baianu , James F. Glazebrook, and Ronald Brown. 2009. Algebraic Topology Foundations of Supersymmetry and Symmetry Breaking in Quantum Field Theory and Quantum Gravity: A Review. SIGMA 5 (2009), 051, 70 pages. , ,http://www.emis.de/journals/SIGMA/2009/051/Symmetry, Integrability and Geometry: Methods and Applications (SIGMA)