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D-brane charge, flux quantisation and relative (co)homology
High Energy Physics - Theory · Submitted 3 Aug 2000
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim Therefore we conclude that for topologically nontrivial B-fields, there is strictly speaking no U(1) gauge field on the D-submanifold.
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The abstract, sentence by sentence
We reconsider the problem of U(1) flux and D0-charge for D-branes in the WZW model and investigate the relationship between the different definitions that have been proposed recently. We identify the D0-charge as a particular reduction of a class in the relative cohomology of the group modulo the D-submanifold. We investigate under which conditions this class is equivalent to the first Chern class of a line bundle on the D-submanifold and we find that in general there is an obstruction given by the cohomology class of the NS 3-form. Therefore we conclude that for topologically nontrivial B-fields, there is strictly speaking no U(1) gauge field on the D-submanifold. Nevertheless the ambiguity in the flux is not detected by the D0-charge. This has a natural interpretation in terms of gerbes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We reconsider the problem of U(1) flux and D0-charge for D-branes in the WZW model and investigate the relationship between the different definitions that have been proposed recently. | contribution 0.58 | 0.80 | 0.04 | asserted 0.54 |
| s1 | We identify the D0-charge as a particular reduction of a class in the relative cohomology of the group modulo the D-submanifold. | result 0.70 | 0.93 | 0.14 | asserted 1.00 |
| s2 | We investigate under which conditions this class is equivalent to the first Chern class of a line bundle on the D-submanifold and we find that in general there is an obstruction given by the cohomology class of the NS 3-form. | result 0.96 | 0.93 | 0.19 | asserted 1.00 |
| s3 | Therefore we conclude that for topologically nontrivial B-fields, there is strictly speaking no U(1) gauge field on the D-submanifold. | result 0.86 | 0.86 | 0.52 | asserted 1.00 |
| s4 | Nevertheless the ambiguity in the flux is not detected by the D0-charge. | result 0.98 | 0.84 | 0.16 | asserted 1.00 |
| s5 | This has a natural interpretation in terms of gerbes. | interpretation 1.00 | 0.45 | 0.06 | asserted 0.96 |
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Original abstract
We reconsider the problem of U(1) flux and D0-charge for D-branes in the WZW model and investigate the relationship between the different definitions that have been proposed recently. We identify the D0-charge as a particular reduction of a class in the relative cohomology of the group modulo the D-submanifold. We investigate under which conditions this class is equivalent to the first Chern class of a line bundle on the D-submanifold and we find that in general there is an obstruction given by the cohomology class of the NS 3-form. Therefore we conclude that for topologically nontrivial B-fields, there is strictly speaking no U(1) gauge field on the D-submanifold. Nevertheless the ambiguity in the flux is not detected by the D0-charge. This has a natural interpretation in terms of gerbes.
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5 arXiv papers cite this in 6 sentences
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Cites it as background 1 paper
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For a discussion see references [ref] .] can be defined as the first Chern class of the bundle $V$ with field strength $F$, q ≡ 1 2π ∫_T^2 tr F_89 = m + n 2π ∫_T^2 B_89 .
Comments on Orientifolds without Vector Structure · Relation to the $B$-flux · 0.88
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