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Related papers: Star Algebra Projectors

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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…

High Energy Physics - Theory · Physics 2007-05-23 Ehud Fuchs , Michael Kroyter , Alon Marcus

A sliver state is a classical solution of the string field theory of the tachyon vacuum that represents a background with a single D25-brane. We show that the sliver wavefunctional factors into functionals of the left and right halves of…

High Energy Physics - Theory · Physics 2009-11-07 Leonardo Rastelli , Ashoke Sen , Barton Zwiebach

We consider "sliver" states which act as projection operators in the matter star product of Witten's cubic string field theory. These sliver states, which might be associated with Dirichlet p-branes, are not finite norm states in the matter…

High Energy Physics - Theory · Physics 2009-11-07 Gregory Moore , Washington Taylor

We generalize the idea of boundary states to open string channel. They describe the emission and absorption of the open string in the presence of intersecting D-branes. We study the algebra between such states under the star products of…

High Energy Physics - Theory · Physics 2007-05-23 Hiroshi Isono , Yutaka Matsuo

We establish a translation dictionary between open and closed strings, starting from open string field theory. Under this correspondence, (off-shell) level-matched closed string states are represented by star algebra projectors in open…

High Energy Physics - Theory · Physics 2007-05-23 L. Bonora , N. Bouatta , C. Maccaferri

We describe projection operators in the matter sector of Witten's cubic string field theory using modes on the right and left halves of the string. These projection operators represent a step towards an analytic solution of the equations of…

High Energy Physics - Theory · Physics 2010-02-03 David J. Gross , Washington Taylor

In this note we show that abstract planar algebras are algebras over the topological operad of moduli spaces of stable maps with Lagrangian boundary conditions, which in the case of the projective line are described in terms of real…

Quantum Algebra · Mathematics 2014-11-20 Ozgur Ceyhan , Matilde Marcolli

We introduce a new class of finite dimensional gentle algebras, the surface algebras, which are constructed from an unpunctured Riemann surface with boundary and marked points by introducing cuts in internal triangles of an arbitrary…

Representation Theory · Mathematics 2011-04-05 Lucas David-Roesler , Ralf Schiffler

We provide a simple construction of bipartite entangled states that are positive under partial transposition, and hence undistillable. The construction makes use of the properties of the projectors onto the symmetric and antisymmetric…

Quantum Physics · Physics 2018-03-21 Enrico Sindici , Marco Piani

The interaction vertex for a fermionic first order system of weights (1,0) such as the twisted bc-system, the fermionic part of N=2 string field theory and the auxiliary \eta\xi system of N=1 strings is formulated in the Moyal basis. In…

High Energy Physics - Theory · Physics 2009-11-10 Matthias Ihl , Alexander Kling , Sebastian Uhlmann

We examine string field algebra which is generated by star product in Witten's string field theory including ghost part. We perform calculations using oscillator representation consistently. We construct wedge like states in ghost part and…

High Energy Physics - Theory · Physics 2010-02-03 Isao Kishimoto

We study star product algebras of analytic functions for which the power series defining the products converge absolutely. Such algebras arise naturally in deformation quantization theory and in noncommutative quantum field theory. We…

Mathematical Physics · Physics 2013-12-24 Michael A. Soloviev

Recent algebraic structures of string theory, including homotopy Lie algebras, gravity algebras and Batalin-Vilkovisky algebras, are deduced from the topology of the moduli spaces of punctured Riemann spheres. The principal reason for these…

High Energy Physics - Theory · Physics 2009-10-22 T. Kimura , J. Stasheff , A. A. Voronov

We elaborate on the relations between surface states and squeezed states. First, we investigate two different criteria for determining whether a matter sector squeezed state is also a surface state and show that the two criteria are…

High Energy Physics - Theory · Physics 2008-11-26 Ehud Fuchs , Michael Kroyter

In this note we study associative dialgebras proving that the most interesting such structures arise precisely when the algebra is not semiprime. In fact the presence of some "perfection" property (simpleness, primitiveness, primeness or…

Rings and Algebras · Mathematics 2010-12-23 Candido Martin Gonzalez

We construct massive open string states around a classical solution in the oscillator formulation of Vacuum String Field Theory. In order for the correct mass spectrum to be reproduced, the projection operators onto the modes of the left-…

High Energy Physics - Theory · Physics 2009-11-07 Hiroyuki Hata , Hisashi Kogetsu

Let A=k+A_1+A_2.... be a connected graded, noetherian k-algebra that is generated in degree one over an algebraically closed field k. Suppose that the graded quotient ring Q(A) has the form Q(A)=k(Y)[t,t^{-1},sigma], where sigma is an…

Rings and Algebras · Mathematics 2014-02-26 D. Rogalski , J. T. Stafford

In string field theory there is a fundamental object, the algebra of string field states \A, that must be understood better from a mathematical point of view. In particular we are interested in finding, if possible, a C^* structure over it,…

High Energy Physics - Theory · Physics 2007-05-23 A. Parodi

We generalize some aspects of the theory of compact projections relative to a C*-algebra, to the setting of more general algebras. Our main result is that compact projections are the decreasing limits of `peak projections', and in the…

Operator Algebras · Mathematics 2012-03-19 David P. Blecher , Matthew Neal

Given the unital C$^*$-algebra $A$, the unitary orbit of the projector $p_0=\begin{pmatrix}1 & 0 \\ 0 & 0 \end{pmatrix}$ in the C$^*$-algebra $M_2(A)$ of $2\times 2$ matrices with coefficients in $A$ is called in this paper, the Riemann…

Operator Algebras · Mathematics 2025-05-13 Esteban Andruchow , Gustavo Corach , Lázaro Recht , Alejandro Varela
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