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单词 AlgebroidStructuresAndExtendedSymmetries
释义

algebroid structures and extended symmetries


0.1 Algebroid Structures and Algebroid Extended Symmetries

Definition 0.1.

An algebroid structure A will be specifically defined to meaneither a ring, or more generally, any of the specifically defined algebrasPlanetmathPlanetmath, 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 R-algebroid A on a set of “objects” A0is a directed graphMathworldPlanetmath over A0 such that for each x,yA0,A(x,y) has an R-module structureMathworldPlanetmath and there is an R-bilinearfunction

:A(x,y)×A(y,z)A(x,z)

(a,b)ab called “compositionMathworldPlanetmathPlanetmath” and satisfying theassociativity condition, and the existence of identitiesPlanetmathPlanetmath.

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 1xA(x,x)is not assumed. For example, if A0 has exactly one object, thenan R-algebroid A over A0 is just an R-algebra. An idealin A is then an example of a pre-algebroid.

Let R be a commutative ring. An R-category A is a category equipped with an R-module structure on each hom set such that the composition is R-bilinear. More precisely, let us assume for instance that we are given a commutative ring R with identity. Then a small R-category–or equivalently an R-algebroid– will be defined as a category enriched in the monoidal category of R-modules, with respect to themonoidal structure of tensor productPlanetmathPlanetmath. This means simply that for all objects b,c of 𝒜, the set 𝒜(b,c) is given the structure of an R-module, and composition 𝒜(b,c)×𝒜(c,d)𝒜(b,d) is R–bilinear, or is a morphismMathworldPlanetmath of R-modules 𝒜(b,c)R𝒜(c,d)𝒜(b,d).

If 𝖦 is a groupoidPlanetmathPlanetmathPlanetmathPlanetmath (http://planetmath.org/Groupoids) (or, more generally, a category)then we can construct an R-algebroid R𝖦 asfollows. The object set of R𝖦 is the same as that of𝖦 and R𝖦(b,c) is the free R-module on theset 𝖦(b,c), with composition given by the usualbilinear rule, extending the composition of 𝖦.

Alternatively, one can define R¯𝖦(b,c) to be theset of functions 𝖦(b,c)R with finite supportPlanetmathPlanetmath, andthen we define the convolution productPlanetmathPlanetmath as follows:

(f*g)(z)={(fx)(gy)z=xy}.(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 functionPlanetmathPlanetmath with compact support’ (http://planetmath.org/SmoothFunctionsWithCompactSupport) (or locallycompact supportMathworldPlanetmathPlanetmath for the QFT (http://planetmath.org/QFTOrQuantumFieldTheories) extendedhttp://planetmath.org/?op=getobj&from=books&id=153symmetryPlanetmathPlanetmath sectors), and inthis case R . 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) 𝖦 by a semigroup G=G{0} in which thecompositions not defined in G are defined to be 0 in G. 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, R-algebroids, double algebroids , and so on.A ‘category’ of R-categories is however a super-categoryPlanetmathPlanetmathPlanetmath (http://planetmath.org/Supercategory) 𝕊, or it can also be viewed as a specific example of a metacategory (http://planetmath.org/AxiomsOfMetacategoriesAndSupercategories) (orR-supercategory, in the more general case of multiple operationsMathworldPlanetmath–categorical ‘composition laws’– being defined within the same structure, for the same class, C).

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. arXiv:0904.3644, doi:10.3842/SIGMA.2009.051,http://www.emis.de/journals/SIGMA/2009/051/Symmetry, Integrability and Geometry: Methods and Applications (SIGMA)
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