## Abstract The functions __a(n)__ and __p(n)__ are defined to be the smallest integer Ξ» for which Ξ»βfold quasimultiples affine and projective planes of order __n__ exist. It was shown by Jungnickel [J. Combin. Designs 3 (1995), 427β432] that __a(n),p(n)__β<β__n__^10^ for sufficiently large __n__.
A Method for Constructing Quasimultiple Affine Planes of Arbitrary Order
β Scribed by J.F. Dillon; G.F. Stahly; M.A. Wertheimer
- Publisher
- Elsevier Science
- Year
- 1995
- Tongue
- English
- Weight
- 88 KB
- Volume
- 1
- Category
- Article
- ISSN
- 1071-5797
No coin nor oath required. For personal study only.
β¦ Synopsis
A quasimultiple affine plane of order (n) and multiplicity (\lambda) is a ((v, k, \lambda)=\left(n^{2}, n, \lambda\right)) balanced incomplete block design. For those cases where the Bruck-Ryser theorem rules out (\lambda=1) it is an interesting problem to determine the smallest actual value of (\lambda). Jungnickel [Discrete Math. 85 (1990), 177-189] has conjectured that (\lambda=\mathbf{2}) is possible for all orders. In this note we present a construction based on a result of Stahly which reduces a number of the bounds on (\lambda) given by Jungnickel. In particular, we construct quasidouble affine planes of orders 6 and 28 verifying the conjecture in these two cases. (1995 Academic Press, Inc.
π SIMILAR VOLUMES
The approximate solution of the differential equation d'+d? + Q'(z)+ = 0 by a general modification of certain phase-integral approximations of arbitrary order is considered. A consistent modification of these higher-order phase-integral approximations is derived on the assumption that one has found
In this paper, the boundary element method (BEM) is used to model acoustic radiation and scattering from bodies of arbitrary shape in close proximity of an infinite plane that has a general impedance boundary condition. A new half-space Green's function for positive reactance boundary conditions is
Following the approach of Jones, Low, and Young, a generalized O(2,l) expansion is developed for amplitudes that have a power bounded growth asymptotically. The expansion, set up in an 0(1, 1) basis, holds in a new kinematical region, where all the incoming and outgoing clusters have space-like 0(2,