D-Branes and Physical States
arXiv:hep-th/9607113 · doi:10.1016/S0550-3213(96)00475-0
Abstract
States obtained by projecting boundary states, associated with D-branes, to fixed mass-level and momentum generically define non-trivial cohomology classes. For on-shell states the cohomology is the standard one, but when the states are off-shell the relevant cohomology is defined using a BRST operator with ghost zero modes removed. The zero momentum cohomology falls naturally into multiplets of . At the massless level, a simple set of D-brane configurations generates the full set of zero-momentum states of standard ghost number, including the discrete states. We give a general construction of off-shell cohomology classes, which exhibits a non-trivial interaction between left and right movers that is not seen in on-shell cohomology. This includes, at higher mass levels, states obtained from typical D-brane boundary states as well as states with more intricate ghost dependence.
22 pages, harvmac, no figures
References in corpus (15)
- Dirichlet-Branes and Ramond-Ramond Charges
- String Theory Dynamics In Various Dimensions
- Evidence for F-Theory
- Bound States Of Strings And -Branes
- Evidence for Heterotic - Type I String Duality
- The eleven-dimensional supermembrane revisited
- D-brane dynamics
- Combinatorics of Boundaries in String Theory
- Boundary States of D-Branes and Dy-Strings
- D-Brane Boundary State Dynamics
- The Size of p-Branes
- String Dynamics at Strong Coupling
- Point-Like States for Type 2b Superstrings
- D-strings and F-strings from string loops
- Who changes the string coupling ?