2013
DOI: 10.1016/j.geomphys.2013.03.002
|View full text |Cite
|
Sign up to set email alerts
|

Quantum field theory overF1

Abstract: Abstract. In this paper we discuss some questions about geometry over the field with one element, motivated by the properties of algebraic varieties that arise in perturbative quantum field theory. We follow the approach to F 1 -geometry based on torified schemes. We first discuss some simple necessary conditions in terms of Euler characteristic and classes in the Grothendieck ring, then we give a blowup formula for torified varieties and we show that the wonderful compactifications of the graph configuration … Show more

Help me understand this report
View preprint versions

Search citation statements

Order By: Relevance

Paper Sections

Select...
2
1
1
1

Citation Types

0
12
0

Year Published

2016
2016
2022
2022

Publication Types

Select...
3
2
2

Relationship

2
5

Authors

Journals

citations
Cited by 10 publications
(12 citation statements)
references
References 37 publications
0
12
0
Order By: Relevance
“…Following the line of thoughts of Manin in [86], there should be a link between F 1 -schemes and motives that explains the similar structure of their zeta functions. There are further connections of motives and F 1 -schemes to non-commutative geometry, see Connes, Consani and Marcolli's papers [25] and [26], Bejleri and Marcolli's paper [7] and Marcolli's appendix of Sujatha and Plazas' lecture notes [107].…”
Section: Results and New Directionsmentioning
confidence: 99%
“…Following the line of thoughts of Manin in [86], there should be a link between F 1 -schemes and motives that explains the similar structure of their zeta functions. There are further connections of motives and F 1 -schemes to non-commutative geometry, see Connes, Consani and Marcolli's papers [25] and [26], Bejleri and Marcolli's paper [7] and Marcolli's appendix of Sujatha and Plazas' lecture notes [107].…”
Section: Results and New Directionsmentioning
confidence: 99%
“…r t e η e,r η e, j β r . One obtains in this way a formulation of the Feynman integral where the relevant variety replacing the graph hypersurface complement XG is the variety Λ G defined above, see [45]. In terms of motivic properties, the varieties Λ G were introduced by Esnault and Bloch in relation to Hodge structures and shown to be always mixed-Tate, [46].…”
Section: This Determines a Complete Intersection Varietymentioning
confidence: 99%
“…Thus, if we consider the product torification on (P d ) n , the morphism π : Bl ∆ ((P d ) n ) → (P d ) n is compatible with torifications only in the weak sense: there is a decomposition (the cell decomposition) of the variety such that there are isomorphisms on the pieces of the decomposition that perform the change of torification that makes the morphism torified, but these isomorphisms do not extend globally to the variety. Thus, in a construction of geometric or constructible torifications on the compactifications P d [n] based on the iterated blowups, as in [1] the maps π : P d [n] → (P d ) n will only be weak F 1 -morphisms, that is, morphisms in the category CT w of Proposition 5.4.…”
Section: Moduli Spaces and Wonderful Compactificationsmentioning
confidence: 99%