Hostname: page-component-6766d58669-kl59c Total loading time: 0 Render date: 2026-05-16T08:44:00.113Z Has data issue: false hasContentIssue false

Finite domination and Novikov homology over strongly $\mathbb {Z}^2$-graded rings

Published online by Cambridge University Press:  28 July 2023

Thomas Hüttemann
Affiliation:
Mathematical Sciences Research Centre, School of Mathematics and Physics, Queen's University Belfast, Belfast BT7 1NN, Northern Ireland, UK (t.huettemann@qub.ac.uk)
Luke Steers
Affiliation:
Mathematical Sciences Research Centre, School of Mathematics and Physics, Queen's University Belfast, Belfast BT7 1NN, Northern Ireland, UK (t.huettemann@qub.ac.uk)
Rights & Permissions [Opens in a new window]

Abstract

Let $R$ be a strongly $\mathbb {Z}^2$-graded ring, and let $C$ be a bounded chain complex of finitely generated free $R$-modules. The complex $C$ is $R_{(0,0)}$-finitely dominated, or of type $FP$ over $R_{(0,0)}$, if it is chain homotopy equivalent to a bounded complex of finitely generated projective $R_{(0,0)}$-modules. We show that this happens if and only if $C$ becomes acyclic after taking tensor product with a certain eight rings of formal power series,  the graded analogues of classical Novikov rings. This extends results of RanickiQuinn and the first author on Laurent polynomial rings in one and two indeterminates.

Information

Type
Research Article
Creative Commons
Creative Common License - CCCreative Common License - BY
This is an Open Access article, distributed under the terms of the Creative Commons Attribution licence (https://creativecommons.org/licenses/by/4.0/), which permits unrestricted re-use, distribution, and reproduction in any medium, provided the original work is properly cited.
Copyright
© The Author(s), 2023. Published by Cambridge University Press on behalf of The Royal Society of Edinburgh
Figure 0

Figure 1. Labelling and orientation of the faces of the square $S$.

Figure 1

Figure 2. Quasi-coherent diagram.

Figure 2

Figure 3. The quasi-coherent diagram $D(k)$.

Figure 3

Figure 4. The diagram $E_{v_{bl}}$.