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Superstring dualities and p-brane bound states
High Energy Physics - Theory · Submitted 19 Dec 1996
abstract compiled · 2026-09-23 · no language-model review
The authors' main claim We show that the M-theory/IIA and IIA/IIB superstring dualities together with the diffeomorphism invariance of the underlying theories require the presence of certain p-brane bound states in IIA and IIB superstring theories preserving 1/2 of the spacetime supersymmetry.
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We show that the M-theory/IIA and IIA/IIB superstring dualities together with the diffeomorphism invariance of the underlying theories require the presence of certain p-brane bound states in IIA and IIB superstring theories preserving 1/2 of the spacetime supersymmetry. We then confirm the existence of IIA and IIB supergravity solutions having the appropriate p-brane bound states interpretation.
background contribution method result interpretation main claim
| # | sentence | role | the authors' own work | states the main conclusion | strength |
|---|---|---|---|---|---|
| s0 | We show that the M-theory/IIA and IIA/IIB superstring dualities together with the diffeomorphism invariance of the underlying theories require the presence of certain p-brane bound states in IIA and IIB superstring theories preserving 1/2 of the spacetime supersymmetry. | result 0.76 | 0.93 | 0.88 | asserted 1.00 |
| s1 | We then confirm the existence of IIA and IIB supergravity solutions having the appropriate p-brane bound states interpretation. | result 0.80 | 0.93 | 0.13 | asserted 1.00 |
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The paper
Original abstract
We show that the M-theory/IIA and IIA/IIB superstring dualities together with the diffeomorphism invariance of the underlying theories require the presence of certain p-brane bound states in IIA and IIB superstring theories preserving 1/2 of the spacetime supersymmetry. We then confirm the existence of IIA and IIB supergravity solutions having the appropriate p-brane bound states interpretation.
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References
How the literature uses it
24 arXiv papers cite this in 26 sentences
Papers citing it · 8 sentences without a confident label
Uses its method or tool 3 papers
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The T-duality relations from type IIB to type IIA are given by [ref] g^(A)_ζ'ζ'=1/g^(B)_ζ'ζ' , g^(A)_MN=g^(B)_MN -g^(B)_ζ' Mg^(B)_ζ' N -B^(B)_ζ' MB^(B)_ζ' N/g^(B)_ζ'ζ' , g^(A)_ζ' M=-B^(B)_ζ' M/g^(B)_ζ'ζ' , ^2ϕ_(A)=^2ϕ_(B)/g^(B)_ζ'ζ' , C_M=C_ζ' M+χB_ζ' M^(B) , C_ζ'=-χ , B^(A)_MN=B^(B)_MN +2B^(B)_ζ' [M g^(B)_N]ζ'/g^(B)_ζ'ζ' , B^(A)_ζ' M=-g^(B)_ζ' M/g^(B)_ζ'ζ' , C_ζ' MN=C_MN +2C_ζ' [M g^(B)_N]ζ'/g^(B)_ζ'ζ' , C_MNP=C_MNPζ'+3/2( C_ζ'[M B^(B)_NP] -B^(B)_ζ' [M C_NP] -4B^(B)_ζ' [M C_|ζ'|Ng^(B)_P]ζ'/g^(B)_ζ'ζ') ,
Dynamical angled brane · D4-brane with angle · 0.85
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Application of the Buscher rules [ref] leads to the NS-NS and R-R field profile for the D7-brane background solution [ref] .
Fluxbrane Inflation · Potential from 10d supergravity perspective · 0.99
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The ten-dimensional T-duality map from the type IIB theory to type IIA theory is given by [ref] g^(A)_xx=1/g^(B)_xx , g^(A)_μν=g^(B)_μν -g^(B)_xμg^(B)_xν -B^(B)_xμB^(B)_xν/g^(B)_xx , g^(A)_xμ=-B^(B)_xμ/g^(B)_xx , ^2ϕ_(A)=^2ϕ_(B)/g^(B)_xx , C_μ=C_xμ+C_(0)B_xμ^(B) , C_x=-C_(0) , B^(A)_μν=B^(B)_μν +2B^(B)_x[μ g^(B)_ν]x/g^(B)_xx , B^(A)_xμ=-g^(B)_xμ/g^(B)_xx , C_xμν=C_μν +2C_x[μ g^(B)_ν]x/g^(B)_xx , C_μνρ=C_μνρx+3/2( C_x[μ B^(B)_νρ] -B^(B)_x[μ C_νρ] -4B^(B)_x[μ C_|x|νg^(B)_ρx/g^(B)_xx) ,
Cosmological brane systems in warped spacetime · Dynamical D2-D6-KK monopole solution · 0.89
Compares with it 1 paper
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In this form the solution is actually simpler than the solutions it generalizes, such as the $D3 ∥D1$, $D3 ∥F1$ [ref] , $D3 ∥(F1 ∥D1)$ and $D3 ∥(F1 ⊥D1)$ bound states [ref] .
The Born-Infeld/Gravity Correspondence · Introduction · 0.85
Cites it as background 14 papers
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It is known that a magnetic flux on a Dp brane stands for the presence of a co-dimension 2 D-branes inside the original Dp brane, forming the so-called 1/2 BPS non-threshold bound state (D(p - 2), Dp) [ref] .
Understanding the open string pair production of the Dp/D0 system · The D2/D0 case · 0.82
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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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