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The D0$-$D8 system revisited
High Energy Physics - Theory · Submitted 6 Sep 2009
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim The persistence of divergence for the potential in either sector in the presence of a flux on the D8 brane indicates that adding a flux/fluxes on the D8 brane doesn't help to improve its nature of existence as an independent object, therefore reenforcing the previous assertion on D8 branes.
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The paper's own sentences, arranged. Each label is drawn from a closed vocabulary; the number beside it is the probability the classifier gave that label. Numbers in the tables are the authors', checked by code. No sentence in this record was written by a model.
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The abstract, sentence by sentence
We address a few subtle issues regarding the interacting D0-D8 system. There are two existing interpretations for the counter-intuitive non-vanishing cylinder-diagram R-R potential. We improve them each by properly dealing with the divergence of potential in the R-R as well as the NS-NS sector, which has been ignored so far. We further test them by considering the D8 to carry a flux, electric or magnetic. We find that the improved interpretations continue to hold. We resolve a subtle issue regarding the regularization of fermionic zero-modes in the R-R sector when the D8 carries an electric flux so that a meaningful result for the potential can be calculated. The persistence of divergence for the potential in either sector in the presence of a flux on the D8 brane indicates that adding a flux/fluxes on the D8 brane doesn't help to improve its nature of existence as an independent object, therefore reenforcing the previous assertion on D8 branes.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We address a few subtle issues regarding the interacting D0-D8 system. | contribution 0.64 | 0.75 | 0.03 | asserted 0.59 |
| s1 | There are two existing interpretations for the counter-intuitive non-vanishing cylinder-diagram R-R potential. | background 1.00 | 0.05 | 0.03 | asserted 1.00 |
| s2 | We improve them each by properly dealing with the divergence of potential in the R-R as well as the NS-NS sector, which has been ignored so far. | contribution 0.88 | 0.92 | 0.08 | asserted 1.00 |
| s3 | We further test them by considering the D8 to carry a flux, electric or magnetic. | method 0.62 | 0.91 | 0.03 | asserted 0.89 |
| s4 | We find that the improved interpretations continue to hold. | result 1.00 | 0.93 | 0.23 | asserted 1.00 |
| s5 | We resolve a subtle issue regarding the regularization of fermionic zero-modes in the R-R sector when the D8 carries an electric flux so that a meaningful result for the potential can be calculated. | result 0.75 | 0.94 | 0.14 | asserted 1.00 |
| s6 | The persistence of divergence for the potential in either sector in the presence of a flux on the D8 brane indicates that adding a flux/fluxes on the D8 brane doesn't help to improve its nature of existence as an independent object, therefore reenforcing the previous assertion on D8 branes. | interpretation 0.93 | 0.82 | 0.61 | hedged possibility 0.77 |
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The paper
Original abstract
We address a few subtle issues regarding the interacting D0-D8 system. There are two existing interpretations for the counter-intuitive non-vanishing cylinder-diagram R-R potential. We improve them each by properly dealing with the divergence of potential in the R-R as well as the NS-NS sector, which has been ignored so far. We further test them by considering the D8 to carry a flux, electric or magnetic. We find that the improved interpretations continue to hold. We resolve a subtle issue regarding the regularization of fermionic zero-modes in the R-R sector when the D8 carries an electric flux so that a meaningful result for the potential can be calculated. The persistence of divergence for the potential in either sector in the presence of a flux on the D8 brane indicates that adding a flux/fluxes on the D8 brane doesn't help to improve its nature of existence as an independent object, therefore reenforcing the previous assertion on D8 branes.
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References
How the literature uses it
2 arXiv papers cite this in 6 sentences
Papers citing it · 5 sentences without a confident label
Cites it as background 1 paper
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However, it is known that this system has various subtle issues [ref] and we will not consider it in this paper for simplicity.
The compactified D-brane cylinder amplitude and T duality · Introduction · 0.86
What it cites · 32 sentences without a confident label
Contests 1 paper
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Note that the integration on the right above is not simply the gamma function $Γ(- 1/2)$ as usually taken in the literature, for example, in [ref] .
Branes, Orientifolds and the Creation of Elementary Strings · On the divergence · contest 0.80
Builds on 1 paper
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So we further improve the improved interpretation proposed in [ref] here.
Fermionic Zero Mode and String Creation between D4-Branes at Angles · On the divergence · 0.90
Uses the method or tool of 5 papers
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Using the newly defined $Γ$-matrices, we have $^ (0)_R-R⟨B_ψ^0,η^0 | B_ψ^8,η^8⟩_R-R^(0) = -_̣η^0η^8,-Tr(Γ̃^0Γ^9)$, where the trace can now be regularized following the regularization procedure given in [ref] since the $Γ̃^0$ is one along a NN-direction and $Γ^9$ is one along a DD-direction.
Microscopic string analysis of the D0-D8 brane system and dual R-R states · The D8 with an electric flux · 0.91
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This can be worked out in almost the same way as the case when the D8 doesn't carry any flux [ref] if a trick as adopted in [ref] is employed.
The open string pair-production rate enhancement by a magnetic flux · The D8 with an electric flux · 0.80
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This can be worked out in almost the same way as the case when the D8 doesn't carry any flux [ref] if a trick as adopted in [ref] is employed.
Comparing D-branes to Black-branes · The D8 with an electric flux · 0.80
Cites as support 1 paper
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This is supported by the existence of a coupling of a string, with its tension one-half of that of the fundamental string, with a worldvolume gauge field in the 8-brane effective action in the presence of a D0 brane [ref] .
Creation of Fundamental Strings by Crossing D-branes · Introduction · 1.00
Cites as background 7 papers
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For later convenience, we give a brief description of each and refer to [ref] for detail.
Interaction between two non-threshold bound states · The D8 with an electric flux · 0.97
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For later convenience, we give a brief description of each and refer to [ref] for detail.
Microscopic string analysis of the D0-D8 brane system and dual R-R states · The D8 with an electric flux · 0.97
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For later convenience, we give a brief description of each and refer to [ref] for detail.
The open string pair-production rate enhancement by a magnetic flux · The D8 with an electric flux · 0.97
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