Over the past 60 years, important examples of Noetherian domains have been constructed using power series, homomorphic images, and intersections. In these constructions it is often crucial that the resulting domain is computable as a directed union. In this article we analyse this construction and s
Maximal Non-Noetherian Subrings of a Domain
✍ Scribed by Ahmed Ayache; Noômen Jarboui
- Publisher
- Elsevier Science
- Year
- 2002
- Tongue
- English
- Weight
- 144 KB
- Volume
- 248
- Category
- Article
- ISSN
- 0021-8693
No coin nor oath required. For personal study only.
✦ Synopsis
The main purpose of this paper is to study maximal non-Noetherian subrings R of a domain S. We give characterizations of such domains in several cases. If the ring R is semi-local, R S is a residually algebraic pair and R is a maximal non-Noetherian subring of S, we give sharp upper bounds for the number of rings and the length of chains of rings in R S , the set of intermediary rings. 2002 Elsevier Science (USA)
📜 SIMILAR VOLUMES
## Abstract It is proved that there is no weight pair (__v,w__) for which the Hardy–Littlewood maximal operator defined on a domain Ω in **R**^__n__^ is compact from the weighted Lebesgue space __L^p^~w~__(Ω) to __L^p^~v~__ (Ω). Results of a similar character are also obtained for the fractional ma
In this note we give the L ޒ = ޒ boundedness of a class of maximal Ž q . 2 Ž ny 1 my1 . singular integral operators with kernel function ⍀ in L log L S = S .
We present an example of a non-simplicial five-dimensional L-type domain of forms on five variables. Its closure has 10 non-simplicial facets each having five extreme rays. This domain is the L-type domain of the form 42.240 of Table 2 of [4] and of the lattice D \* 5 , the dual of the root lattice
In this paper it is shown that given a non-degenerate elliptic quadric in the projective space PG(2n -1, q), q odd, then there does not exist a spread of PG(2n -1, q) such that each element of the spread meets the quadric in a maximal totally singular subspace. An immediate consequence is that the c
A new method, based on the Kelvin transformation and the Fokas integral method, is employed for solving analytically a potential problem in a non-convex unbounded domain of R 2 , assuming the Neumann boundary condition. Taking advantage of the property of the Kelvin transformation to preserve harmon