Abstract

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.

Highlights

  • Since Schnabl’s construction [1] of an analytic solution for tachyon condensation in cubic open string field theory (CSFT), there have appeared lots of studies on the analytic construction of solutions representing multiple D25-branes within the framework of the KBc algebra [2].1 Among them, the construction presented in [4] by using the boundary condition changing operators, in addition to the elements of the KBc algebra, may be a satisfactory one

  • In [8], we proposed that the 3-brane solution with N = 2 and T = 0 can be constructed in the form (1.2) by making use of the singularities both at K = 0 and K = ∞, and taking, for example, G(K) = (1 + K)2/K

  • We have presented an analytic expression of the multi-brane solutions of CSFT for arbitrary brane numbers

Read more

Summary

Introduction

In this Appendix, we derive eq (3.28) for Sm1,m2,m3 (3.24) by using the (s, z)-integration formula for the Bcccc-correlators [5, 7]. For hQ (E.5), calculating the sum of residues at z = −1 and −1 ± (2πi/s) by using the formula (C.11) and carrying out the s-integration, we obtain. This leads to the expression of hQ given by (4.12) and (4.13). (±) θ(Q ≤ −2) 1F1(2 + Q, 3; ±z) − θ(Q ≥ 1) 1F1(1 − Q, 3; ±z)

Assumptions on the solution
Convenient notation
The most generic unitary U
Γ2 I12
Assumptions on Γa and Fab
N in terms of Γa and Fab
Kεn1 c
Summary and discussions
Full Text
Paper version not known

Talk to us

Join us for a 30 min session where you can share your feedback and ask us any queries you have

Schedule a call

Disclaimer: All third-party content on this website/platform is and will remain the property of their respective owners and is provided on "as is" basis without any warranties, express or implied. Use of third-party content does not indicate any affiliation, sponsorship with or endorsement by them. Any references to third-party content is to identify the corresponding services and shall be considered fair use under The CopyrightLaw.