We find a new subalgebra of the star product in the matter sector. Its elements are squeezed states whose matrices commute with (K_1)^2. This subalgebra contains a large set of projectors. The states are represented by their eigenvalues and we find a mapping between the eigenvalues representation and other known representations. The sliver is naturally in this subalgebra. Surprisingly, all the generalized butterfly states are also in this subalgebra, enabling us to analyze their spectrum, and to show the orthogonality of different butterfly states. This means that multi D-brane states can be built of butterfly states
A sliver state is a classical solution of the string field theory of the tachyon vacuum that represe...
We generalize the idea of boundary states to open string channel. They describe the emission and abs...
Following Okawa, we insert operators at the boundary of regulated star algebra projectors to constru...
The interaction vertex for a fermionic first order system of weights (1,0) such as the twisted bc-sy...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We show that a single-mode squeeze operator S(z) being an unitary operator with a purely continuous ...
The spectrum of the infinite dimensional Neumann matrices M^{11}, M^{12} and M^{21} in the oscillato...
The wedge states form an important subalgebra in the string field theory. We review and further inve...
We define a new set of squeezed states using group theoretical methods. The definition is based on t...
The Barut-Girardello coherent states (BG CS) representation is extended to the noncompact algebras u...
The spectrum of the infinite dimensional Neumann matrices M11, M12 and M21 in the oscillator constru...
In the context of the Anti-de Sitter / Conformal Field Theory correspondence we consider the Berenst...
In Chapter 1, we give an introduction to the topic of open string field theory. The concepts present...
A sliver state is a classical solution of the string field theory of the tachyon vacuum that represe...
We generalize the idea of boundary states to open string channel. They describe the emission and abs...
Following Okawa, we insert operators at the boundary of regulated star algebra projectors to constru...
The interaction vertex for a fermionic first order system of weights (1,0) such as the twisted bc-sy...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We elaborate on the relations between surface states and squeezed states. First, we investigate two ...
We show that a single-mode squeeze operator S(z) being an unitary operator with a purely continuous ...
The spectrum of the infinite dimensional Neumann matrices M^{11}, M^{12} and M^{21} in the oscillato...
The wedge states form an important subalgebra in the string field theory. We review and further inve...
We define a new set of squeezed states using group theoretical methods. The definition is based on t...
The Barut-Girardello coherent states (BG CS) representation is extended to the noncompact algebras u...
The spectrum of the infinite dimensional Neumann matrices M11, M12 and M21 in the oscillator constru...
In the context of the Anti-de Sitter / Conformal Field Theory correspondence we consider the Berenst...
In Chapter 1, we give an introduction to the topic of open string field theory. The concepts present...
A sliver state is a classical solution of the string field theory of the tachyon vacuum that represe...
We generalize the idea of boundary states to open string channel. They describe the emission and abs...
Following Okawa, we insert operators at the boundary of regulated star algebra projectors to constru...