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(F,Dp) bound states from the boundary state
High Energy Physics - Theory · Submitted 28 Jun 1999
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We use the boundary state formalism to provide the full conformal description of (F,Dp) bound states.
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The abstract, sentence by sentence
We use the boundary state formalism to provide the full conformal description of (F,Dp) bound states. These are BPS configurations that arise from a superposition of a fundamental string and a Dp brane, and are charged under both the NS-NS antisymmetric tensor and the (p+1)-form R-R potential. We construct the boundary state for these bound states by switching on a constant electric field on the world-volume of a Dp brane and fix its value by imposing the Dirac quantization condition on the charges. Using the operator formalism we also derive the Dirac-Born-Infeld action and the classical supergravity solutions corresponding to these configurations.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We use the boundary state formalism to provide the full conformal description of (F,Dp) bound states. | contribution 0.92 | 0.95 | 0.42 | asserted 1.00 |
| s1 | These are BPS configurations that arise from a superposition of a fundamental string and a Dp brane, and are charged under both the NS-NS antisymmetric tensor and the (p+1)-form R-R potential. | background 0.93 | 0.15 | 0.14 | asserted 1.00 |
| s2 | We construct the boundary state for these bound states by switching on a constant electric field on the world-volume of a Dp brane and fix its value by imposing the Dirac quantization condition on the charges. | method 0.97 | 0.95 | 0.12 | asserted 1.00 |
| s3 | Using the operator formalism we also derive the Dirac-Born-Infeld action and the classical supergravity solutions corresponding to these configurations. | contribution 0.53 | 0.95 | 0.19 | asserted 1.00 |
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The paper
Original abstract
We use the boundary state formalism to provide the full conformal description of (F,Dp) bound states. These are BPS configurations that arise from a superposition of a fundamental string and a Dp brane, and are charged under both the NS-NS antisymmetric tensor and the (p+1)-form R-R potential. We construct the boundary state for these bound states by switching on a constant electric field on the world-volume of a Dp brane and fix its value by imposing the Dirac quantization condition on the charges. Using the operator formalism we also derive the Dirac-Born-Infeld action and the classical supergravity solutions corresponding to these configurations.
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References
How the literature uses it
21 arXiv papers cite this in 57 sentences
Papers citing it · 33 sentences without a confident label
Builds on it 1 paper
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The vanishing result for the special case of $(m_1, n_1) = (m_2, n_2)$ was previously shown in [ref] and we here generalize it to a general case.
Interaction between two non-threshold bound states · The long-range interactions · 0.99
Uses its method or tool 3 papers
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In this paper, we will use the description of a boundary state with a quantized world-volume flux given in [ref] for the bound state to calculate explicitly the interaction between two non-threshold (F, D$_p$) (or (D$_p - 2$, D$_p$)) bound states separated by a distance.
Interaction between two non-threshold bound states · Introduction · 0.99
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We compute first the closed-string cylinder amplitude using the closed string boundary state representation of D-brane [ref] , which has the advantage of holding true for a general worldvolume constant flux [ref] .
On D-brane interaction & its related properties · Introduction · 0.98
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Using Poisson's identity [equation] with $n=w$, $s=0$, $A=μR^2/L_s^2$, and changing the integration variable in ([ref]) according to $t→t=1/τ$, with the help of the modular transformation property [ref] [equation] we finally obtain
Geometry from D-branes in Nonrelativistic String Theory · Normalization of boundary state · 0.94
Compares with it 1 paper
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The couplings obtained above are in complete agreement with those obtained in [ref] using boundary state approach and will be used in the following section to obtain the long-range forces between two non-threshold bound states.
Interaction between two non-threshold bound states · The couplings with bulk massless modes · 0.99
Cites it as support 1 paper
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This can also be explained by the fact that a Dp brane carrying a constant worldvolume electric flux is actually a 1/2 BPS non-threshold bound state [ref] , therefore it is stable and cannot decay via the open string pair production.
On D-brane interaction & its related properties · Introduction · 0.98
Cites it as background 9 papers
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In addition to the simple strings and simple D-branes, i.e., extended objects charged under only one NS-NS potential or one R-R potential, there also exist their supersymmetry preserving bound states such as (F, D$_p$) [ref] and (D$_p - 2$, D$_p$) [ref] , i.e., extended objects charged under more than one potential.
Interaction between two non-threshold bound states · Introduction · 0.97
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When each Dp-brane carries fluxes, which can be electric and/or magnetic ones[ The electric flux on a Dp-brane stands for the presence of F-strings, forming the so-called (F, Dp) non-threshold bound state [ref] , while a magnetic flux stands for that of co-dimension 2 D-branes inside the original Dp brane, forming the so-called (D(p-2), Dp) non-threshold bound state [ref] , from the spacetime perspective.
Some aspects of interaction amplitudes of D branes carrying worldvolume fluxes · Introduction · 0.93
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As we know that D-branes carrying a single abelian electric or magnetic world volume flux are the non-threshold BPS (F, D$p$) bound state [ref] or the non-threshold BPS (D$(p-2)$, D$p$) bound state [ref] , respectively.
A classification of long-range interactions between two stacks of $p$ \& $p'$-branes · The long-range interactions between non-parallel D-branes with flux · 0.88
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