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Freed-Witten anomaly and D-brane gauge theories
High Energy Physics - Theory · Submitted 16 Jan 2012
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The Freed-Witten anomaly, which is a global world-sheet anomaly, imposes some constraints on such fields: we will show for each case what is the nature of the corresponding gauge theory on the D-brane or stack of D-branes.
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We discuss the different nature of the gauge theories on a D-brane or a stack of D-branes, in type II superstring theory, as follows from the Freed-Witten anomaly. Usually on a D-brane world-volume there is a standard gauge theory, described by the A-field thought of as a connection on a complex vector bundle. Actually, this is a particular case, even if it is the most common one. In order to get a complete picture, within the framework provided by the geometry of gerbes with connection, it is necessary to give a joint geometrical description of the A-field and the B-field, via the language of Cech hypercohomology. The Freed-Witten anomaly, which is a global world-sheet anomaly, imposes some constraints on such fields: we will show for each case what is the nature of the corresponding gauge theory on the D-brane or stack of D-branes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We discuss the different nature of the gauge theories on a D-brane or a stack of D-branes, in type II superstring theory, as follows from the Freed-Witten anomaly. | contribution 0.93 | 0.79 | 0.26 | asserted 0.96 |
| s1 | Usually on a D-brane world-volume there is a standard gauge theory, described by the A-field thought of as a connection on a complex vector bundle. | background 1.00 | 0.07 | 0.06 | asserted 1.00 |
| s2 | Actually, this is a particular case, even if it is the most common one. | background 0.83 | 0.13 | 0.04 | asserted 1.00 |
| s3 | In order to get a complete picture, within the framework provided by the geometry of gerbes with connection, it is necessary to give a joint geometrical description of the A-field and the B-field, via the language of Cech hypercohomology. | method 0.76 | 0.30 | 0.14 | asserted 1.00 |
| s4 | The Freed-Witten anomaly, which is a global world-sheet anomaly, imposes some constraints on such fields: we will show for each case what is the nature of the corresponding gauge theory on the D-brane or stack of D-branes. | contribution 0.86 | 0.82 | 0.49 | asserted 1.00 |
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Original abstract
We discuss the different nature of the gauge theories on a D-brane or a stack of D-branes, in type II superstring theory, as follows from the Freed-Witten anomaly. Usually on a D-brane world-volume there is a standard gauge theory, described by the A-field thought of as a connection on a complex vector bundle. Actually, this is a particular case, even if it is the most common one. In order to get a complete picture, within the framework provided by the geometry of gerbes with connection, it is necessary to give a joint geometrical description of the A-field and the B-field, via the language of Cech hypercohomology. The Freed-Witten anomaly, which is a global world-sheet anomaly, imposes some constraints on such fields: we will show for each case what is the nature of the corresponding gauge theory on the D-brane or stack of D-branes.
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Cites as background 1 paper
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We recall that, for a single D-brane, the world-sheet path-integral measure contains the terms [ref] : [equation] where $Σ$ is the world-sheet, $ϕ$ is the trajectory of the world-sheet in the space-time, $D_ϕ$ is the pfaffian of the Dirac operator on the world-sheet, coupled to the space-time via $ϕ$, and $A$ and $B$ are the $A$-field and the $B$-field.
Anomalies in String Theory with D-Branes · Single D-brane · 0.81
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