Search engine for discovering works of Art, research articles, and books related to Art and Culture
ShareThis
Javascript must be enabled to continue!

Analytic construction of multi-brane solutions in cubic string field theory for any brane number

View through CrossRef
Abstract We present an analytic construction of multi-brane solutions with any integer brane number in cubic open string field theory (CSFT) on the basis of the ${K\!Bc}$ algebra. Our solution is given in the pure-gauge form $\Psi=U{Q_\textrm{B}} U^{-1}$ by a unitary string field $U$, which we choose to satisfy two requirements. First, the energy density of the solution should reproduce that of the $(N+1)$-branes. Second, the equations of motion (EOM) of the solution should hold against the solution itself. In spite of the pure-gauge form of $\Psi$, these two conditions are non-trivial ones due to the singularity at $K=0$. For the $(N+1)$-brane solution, our $U$ is specified by $[N/2]$ independent real parameters $\alpha_k$. For the 2-brane ($N=1$), the solution is unique and reproduces the known one. We find that $\alpha_k$ satisfying the two conditions indeed exist as far as we have tested for various integer values of $N\ (=2, 3, 4, 5, \ldots)$. Our multi-brane solutions consisting only of the elements of the ${K\!Bc}$ algebra have the problem that the EOM is not satisfied against the Fock states and therefore are not complete ones. However, our construction should be an important step toward understanding the topological nature of CSFT, which has similarities to the Chern–Simons theory in three dimensions.
Title: Analytic construction of multi-brane solutions in cubic string field theory for any brane number
Description:
Abstract We present an analytic construction of multi-brane solutions with any integer brane number in cubic open string field theory (CSFT) on the basis of the ${K\!Bc}$ algebra.
Our solution is given in the pure-gauge form $\Psi=U{Q_\textrm{B}} U^{-1}$ by a unitary string field $U$, which we choose to satisfy two requirements.
First, the energy density of the solution should reproduce that of the $(N+1)$-branes.
Second, the equations of motion (EOM) of the solution should hold against the solution itself.
In spite of the pure-gauge form of $\Psi$, these two conditions are non-trivial ones due to the singularity at $K=0$.
For the $(N+1)$-brane solution, our $U$ is specified by $[N/2]$ independent real parameters $\alpha_k$.
For the 2-brane ($N=1$), the solution is unique and reproduces the known one.
We find that $\alpha_k$ satisfying the two conditions indeed exist as far as we have tested for various integer values of $N\ (=2, 3, 4, 5, \ldots)$.
Our multi-brane solutions consisting only of the elements of the ${K\!Bc}$ algebra have the problem that the EOM is not satisfied against the Fock states and therefore are not complete ones.
However, our construction should be an important step toward understanding the topological nature of CSFT, which has similarities to the Chern–Simons theory in three dimensions.

Related Results

What is Analytic Philosophy
What is Analytic Philosophy
Special Issue: What is Analytic PhilosophyReferencesHaaparantaG. P. Baker and P. M. S. Hacker. Frege: Logical Excavations. Oxford, Blackwell, 1984.M. Dummett. The Interpretation of...
Brane motion in a compact space: Adiabatic perturbations of brane-bulk coupled fluids
Brane motion in a compact space: Adiabatic perturbations of brane-bulk coupled fluids
When a brane is moving in a compact space, bulk-probing signals originating at the brane can arrive back at the brane outside the lightcone of the emitting event. In this paper, we...
D3-brane loop amplitudes from M5-brane tree amplitudes
D3-brane loop amplitudes from M5-brane tree amplitudes
Abstract We study loop corrections to scattering amplitudes in the world-volume theory of a probe D3-brane, which is described by the supersymmetric Dirac-Born...
String Field Theory
String Field Theory
After more than 50 years from the Veneziano amplitude, the fundamental formulation of string theory (ST) remains elusive. On the one hand, there is the world-sheet formulation that...
Parameterized Strings: Algorithms and Applications
Parameterized Strings: Algorithms and Applications
The parameterized string (p-string), a generalization of the traditional string, is composed of constant and parameter symbols. A parameterized match (p-match) exists between two p...
Cutoff brane vs the Karch-Randall brane: the fluctuating case
Cutoff brane vs the Karch-Randall brane: the fluctuating case
Abstract Recently, certain holographic Weyl transformed CFT2 is proposed to capture the main features of the AdS3/BCFT2 correspondence [1, 2]. In this paper, b...
All-order quartic couplings in highly symmetric D-brane-anti-D-brane systems
All-order quartic couplings in highly symmetric D-brane-anti-D-brane systems
A bstract We compute six-point string amplitudes for the scattering of one closed string Ramond-Ramond...
Perturbative F-theory 10-brane and M-theory 5-brane
Perturbative F-theory 10-brane and M-theory 5-brane
Abstract The exceptional symmetry is realized perturbatively in F-theory which is the manifest U-duality theory. The SO(5) U-duality symmetry acts on both the ...

Back to Top