(Noncommutative) Supersymmetric Peakon Type (original) (raw)

Using Grozman's formalism of invariant differential operators we demonstrate the derivation of N = 2 Camassa-Holm equation from the action of Vect(S 1|2) on the space of pseudo-differential symbols. We also use generalized logarithmic 2-cocycles to derive N = 2 super KdV equations. We show this method is equally effective to derive Camassa-Holm family of equations and these system of equations can also be interpreted as geodesic flows on the Bott-Virasoro group with respect to right invariant H 1-metric. In the second half of the paper we focus on the derivations of the fermionic extension of a new peakon type systems. This new one-parameter family of N = 1 super peakon type equations, known as N = 1 super b-field equations, are derived from the action of Vect(S 1|1) on tensor densities of arbitrary weights. Finally, using the formal Moyal deformed action of Vect(S 1|1) on the space of Pseudo-differential symbols to derive the noncommutative analogues of N = 1 super b-field equations. Keywords Pseudo-differential symbols • Super KdV • Camassa-Holm equation • Geodesic flow • Super b-field equations • Moyal deformation • Noncommutative integrable systems Mathematics Subject Classification (2000) 17B68 • 37K10 • 58J40 1 Prelude to Noncommutative Integrable Systems Noncommutative geometry [5] extends the notions of classical differential geometry from differential manifold to discrete spaces, like finite sets and fractals, and noncommutative spaces which are given by noncommutative associative algebras. It was an idea of Descartes that we can study a space by means of functions on the space, in other words, the algebra

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Virasoro Action on Pseudo-Differential Symbols and (Noncommutative) Supersymmetric Peakon Type Integrable Systems

Acta Applicandae Mathematicae, 2008

Using Grozman's formalism of invariant differential operators we demonstrate the derivation of N = 2 Camassa-Holm equation from the action of Vect(S 1|2) on the space of pseudo-differential symbols. We also use generalized logarithmic 2-cocycles to derive N = 2 super KdV equations. We show this method is equally effective to derive Camassa-Holm family of equations and these system of equations can also be interpreted as geodesic flows on the Bott-Virasoro group with respect to right invariant H 1-metric. In the second half of the paper we focus on the derivations of the fermionic extension of a new peakon type systems. This new one-parameter family of N = 1 super peakon type equations, known as N = 1 super b-field equations, are derived from the action of Vect(S 1|1) on tensor densities of arbitrary weights. Finally, using the formal Moyal deformed action of Vect(S 1|1) on the space of Pseudo-differential symbols to derive the noncommutative analogues of N = 1 super b-field equations. Keywords Pseudo-differential symbols • Super KdV • Camassa-Holm equation • Geodesic flow • Super b-field equations • Moyal deformation • Noncommutative integrable systems Mathematics Subject Classification (2000) 17B68 • 37K10 • 58J40 1 Prelude to Noncommutative Integrable Systems Noncommutative geometry [5] extends the notions of classical differential geometry from differential manifold to discrete spaces, like finite sets and fractals, and noncommutative spaces which are given by noncommutative associative algebras. It was an idea of Descartes that we can study a space by means of functions on the space, in other words, the algebra

Superconformal Algebras and Supersymmetric Integrable Flows

2009

After a comprehensive review of superconformal algebras, super-diffeomorphisms and supervector fields on supercircles S 1|n we study various supersymmetric extensions of the KdV and Camassa-Holm equations. We describe their (super) Hamiltonian structures and their connection to bihamiltonian geometry. These are interpreted as geodesic flows on various superconformal groups. We also give an example of superintegrable systems of Ramond type. The one-parameter family of equations shown by Degasperis, Holm and Hone (DHH) to possess multi-peakon solutions is identified as a geodesic flow equation on a one-parameter deformation of the group of diffeomorphisms of the circle, with respect to a right-invariant Sobolev H 1-metric. A supersymmetrisation of the algebra of deformed vector fields on S 1 yields supersymmetric DHH equations (also known as b-field equations), which include the supersymmetric Camassa-Holm equation as a special case.

V ect ( S 1 ) Action on Pseudodifferential Symbols on S 1 and (Noncommutative) Hydrodynamic Type Systems

Journal of Nonlinear Mathematical Physics, 2006

The standard embedding of the Lie algebra V ect(S 1) of smooth vector fields on the circle V ect(S 1) into the Lie algebra ΨD(S 1) of pseudodifferential symbols on S 1 identifies vector field f (x) ∂ ∂x ∈ V ect(S 1) and its dual as π(f (x) ∂ ∂x) = f (x)ξ π(u(x)dx 2) = u(x)ξ −2. The space of symbols can be viewed as the space of functions on T * S 1. The natural lift of the action of Dif f (S 1) yields Dif f (S 1)-module. In this paper we demonstate this construction to yield several examples of dispersionless integrable systems. Using Ovsienko and Roger method for nontrivial deformation of the standard embedding of V ect(S 1) into ΨD(S 1) we obtain the celebrated Hunter-Saxton equation. Finally, we study the Moyal quantization of all such systems to construct noncommutative systems.

Field Theory on Noncommutative Space-Time and the Deformed Virasoro Algebra

arXiv: High Energy Physics - Theory, 2000

We consider a field theoretical model on the noncommutative cylinder which leads to a discrete-time evolution. Its Euclidean version is shown to be equivalent to a model on the complex qqq-plane. We reveal a direct link between the model on a noncommutative cylinder and the deformed Virasoro algebra constructed earlier on an abstract mathematical background. As it was shown, the deformed Virasoro generators necessarily carry a second index (in addition to the usual one), whose meaning, however, remained unknown. The present field theoretical approach allows one to ascribe a clear meaning to this second index: its origin is related to the noncommutativity of the underlying space-time. The problems with the supersymmetric extension of the model on a noncommutative super-space are briefly discussed.

LTCC Lectures on Noncommutative Differential Geometry

2018

Noncommutative geometry is the idea that when geometry is done in terms of coordinate algebras, one does not really need the algebra to be commutative. We provide an introduction to the relevant mathematics from a constructive ‘differential algebra’ point of view that works over general fields and includes the noncommutative geometry of quantum groups as well as of finite groups. We also mention applications to models of quantum spacetime.

Supersymmetric Kuper Camassa–Holm Equation and Geodesic Flow: A Novel Approach

International Journal of Geometric Methods in Modern Physics, 2008

We use the logarithmic 2-cocycle and the action of V ect (S1) on the space of pseudodifferential symbols to derive one particular type of supersymmetric KdV equation, known as Kuper-KdV equation. This equation was formulated by Kupershmidt and it is different from the Manin–Radul–Mathieu type equation. The two Super KdV equations behave differently under a supersymmetric transformation and Kupershmidt version does not preserve SUSY transformation. In this paper we study the second type of supersymmetric generalization of the Camassa–Holm equation correspoding to Kuper-KdV equation via standard embedding of super vector fields into the Lie algebra of graded pseudodifferential symbols. The natural lift of the action of superconformal group SDiff yields SDiff module. This method is particularly useful to construct Moyal quantized systems.

Supersymmetry in noncommutative superspaces

Journal of High Energy Physics, 2003

Non commutative superspaces can be introduced as the Moyal-Weyl quantization of a Poisson bracket for classical superfields. Different deformations are studied corresponding to constant background fields in string theory. Supersymmetric and non supersymmetric deformations can be defined, depending on the differential operators used to define the Poisson bracket. Some examples of deformed, 4 dimensional lagrangians are given. For extended superspace (N > 1), some new deformations can be defined, with no analogue in the N = 1 case.

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