1994
DOI: 10.2748/tmj/1178225715
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Moduli of pairs and generalized theta divisors

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Cited by 26 publications
(32 citation statements)
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“…For E T on T × X and Λ T on T , we shall exploit the natural isomorphism Hom(π * Λ T , E T ) ∼ = Hom(Λ T , π * E T ) to regard a family of Brill-Noether pairs as specified by a map j T : Λ T → π * E T such that, for each t ∈ T , E t is torsion-free and the induced map Λ t → H 0 (E t ) is injective. This last condition implies that j T is a sheaf injection, and we thus recover Definition 1.11 of [13]. Now the family on R ss comes from (i) the universal quotient sheaf E Q on Q × X, for which π * E Q can be identified with a subsheaf of V ⊗O Q over the good points corresponding to torsion-free sheaves, and (ii) the universal subsheaf L G ⊂ V ⊗O G on G. More accurately, let E R ss be the pull-back of E Q to R ss × X and let Λ R ss be the pull-back of L G to R ss .…”
Section: 5supporting
confidence: 63%
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“…For E T on T × X and Λ T on T , we shall exploit the natural isomorphism Hom(π * Λ T , E T ) ∼ = Hom(Λ T , π * E T ) to regard a family of Brill-Noether pairs as specified by a map j T : Λ T → π * E T such that, for each t ∈ T , E t is torsion-free and the induced map Λ t → H 0 (E t ) is injective. This last condition implies that j T is a sheaf injection, and we thus recover Definition 1.11 of [13]. Now the family on R ss comes from (i) the universal quotient sheaf E Q on Q × X, for which π * E Q can be identified with a subsheaf of V ⊗O Q over the good points corresponding to torsion-free sheaves, and (ii) the universal subsheaf L G ⊂ V ⊗O G on G. More accurately, let E R ss be the pull-back of E Q to R ss × X and let Λ R ss be the pull-back of L G to R ss .…”
Section: 5supporting
confidence: 63%
“…Such pairs are the common generalisation of the classical notion of a linear system, for which E is (the sheaf of sections of) a line bundle, and of Bradlow pairs [3], for which one may take Λ to be 1-dimensional -although strictly speaking Λ should be replaced by a single non-zero section φ. These more general pairs have also been studied by Bertram [2], Raghavendra and Vishwanath [13] (under the name of "pairs") and by Le Potier [8] (under the name of "coherent systems"), who works over varieties (or schemes) of arbitrary dimension. In this paper, we shall use the term "Brill-Noether pair", to emphasise the role that we hope they will play in higher rank Brill-Noether theory.…”
Section: Introductionmentioning
confidence: 99%
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“…In this section we review certain facts about coherent systems which we will need in what follows. We refer the reader to Bradlow et al 3, King‐Newstead 18, He 14, Le Potier 24 and Raghavendra‐Vishwanath 29 for more details. Roughly, a coherent system of type ( k , d , r ) is a pair ( E , V ) with E a vector bundle of rank r and degree d and V ∈ G ( k , H 0 ( E )).…”
Section: Preliminariesmentioning
confidence: 99%
“…The full subcategory S α,μ (X) of C(X) consisting of α-semistable coherent systems with fixed α-slope μ is a Noetherian and Artinian abelian category with simple objects that are precisely the α-stable coherent systems (see [15,23]).…”
Section: Coherent Systemsmentioning
confidence: 99%