The partial group algebra of a group G over a field K, denoted by K G , is par the algebra whose representations correspond to the partial representations of G over K-vector spaces. In this paper we study the structure of the partial group Ε½ . algebra K G , where G is a finite group. In particular,
Partial Fields and Matroid Representation
β Scribed by Charles Semple; Geoff Whittle
- Publisher
- Elsevier Science
- Year
- 1996
- Tongue
- English
- Weight
- 228 KB
- Volume
- 17
- Category
- Article
- ISSN
- 0196-8858
No coin nor oath required. For personal study only.
β¦ Synopsis
A partial field P is an algebraic structure that behaves very much like a field except that addition is a partial binary operation, that is, for some a, b g P, a q b may not be defined. We develop a theory of matroid representation over partial fields. It is shown that many important classes of matroids arise as the class of matroids representable over a partial field. The matroids representable over a partial field are closed under standard matroid operations such as the taking of minors, duals, direct sums, and 2-sums. Homomorphisms of partial fields are defined. It is shown that if : P Βͺ P is a non-trivial partial-field homomorphism, 1 2 then every matroid representable over P is representable over P . The connec-1 2 tion with Dowling group geometries is examined. It is shown that if G is a finite abelian group, and r ) 2, then there exists a partial field over which the rank-r Dowling group geometry is representable if and only if G has at most one element of order 2, that is, if G is a group in which the identity has at most two square roots.
π SIMILAR VOLUMES
## Sprbljig A new approach to the boundary value problem for the classic Dirac equation is proposed. This approach is based on a recent version of the metaharmonic quaternionic analysis developed in [14-161. In particular, the following problem is studied: when and how a given function on a surfac
## Abstract When complex structures are divided into subdomains for electromagnetic field computations, it is necessary to specify which of the tangential electromagnetic field components at the boundaries may be regarded as independent and which have to be treated as dependent. In this third of ou