200 research outputs found

    On the nature of the Virasoro algebra

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    The multiplication in the Virasoro algebra [ep,eq]=(pq)ep+q+θ(p3p)δp+q,p,qZ, [e_p, e_q] = (p - q) e_{p+q} + \theta \left(p^3 - p\right) \delta_{p + q}, \qquad p, q \in {\mathbf Z}, [θ,ep]=0, [\theta, e_p] = 0, comes from the commutator [ep,eq]=epeqeqep[e_p, e_q] = e_p * e_q - e_q * e_p in a quasiassociative algebra with the multiplication \renewcommand{\theequation}{*} \be \ba{l} \ds e_p * e_q = - {q (1 + \epsilon q) \over 1 + \epsilon (p + q)} e_{p+q} + {1 \over 2} \theta \left[p^3 - p + \left(\epsilon - \epsilon^{-1} \right) p^2 \right] \delta^0_{p+q}, \vspace{3mm}\\ \ds e_p * \theta = \theta* e_p = 0. \ea \ee The multiplication in a quasiassociative algebra R{\cal R} satisfies the property \renewcommand{\theequation}{**} \be a * (b * c) - (a * b) * c = b * (a * c) - (b * a) * c, \qquad a, b, c \in {\cal R}. \ee This property is necessary and sufficient for the Lie algebra {\it Lie}(R)({\cal R}) to have a phase space. The above formulae are put into a cohomological framework, with the relevant complex being different from the Hochschild one even when the relevant quasiassociative algebra R{\cal R} becomes associative. Formula ()(*) above also has a differential-variational counterpart

    Coadjoint Poisson actions of Poisson-Lie groups

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    A Poisson-Lie group acting by the coadjoint action on the dual of its Lie algebra induces on it a non-trivial class of quadratic Poisson structures extending the linear Poisson bracket on the coadjoint orbits

    Quadratic Poisson brackets compatible with an algebra structure

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    Quadratic Poisson brackets on a vector space equipped with a bilinear multiplication are studied. A notion of a bracket compatible with the multiplication is introduced and an effective criterion of such compatibility is given. Among compatible brackets, a subclass of coboundary brackets is described, and such brackets are enumerated in a number of examples.Comment: 6 page

    r-matrices for relativistic deformations of integrable systems

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    We include the relativistic lattice KP hierarchy, introduced by Gibbons and Kupershmidt, into the rr-matrix framework. An rr-matrix account of the nonrelativistic lattice KP hierarchy is also provided for the reader's convenience. All relativistic constructions are regular one-parameter perturbations of the nonrelativistic ones. We derive in a simple way the linear Hamiltonian structure of the relativistic lattice KP, and find for the first time its quadratic Hamiltonian structure. Amasingly, the latter turns out to coincide with its nonrelativistic counterpart (a phenomenon, known previously only for the simplest case of the relativistic Toda lattice)

    On the Miura map between the dispersionless KP and dispersionless modified KP hierarchies

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    We investigate the Miura map between the dispersionless KP and dispersionless modified KP hierarchies. We show that the Miura map is canonical with respect to their bi-Hamiltonian structures. Moreover, inspired by the works of Takasaki and Takebe, the twistor construction of solution structure for the dispersionless modified KP hierarchy is given.Comment: 19 pages, Latex, no figure

    2D Quantum Gravity and The Miura Map

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    We study the sL(3,C) mKDV string theories. We obtain the flows and the string equations. Using the generalized Miura map, we show that we have an unification of these models with the [P,Q]=Q sL(3,C) KDV ones in the framework of open-closed string theories in minimal models backgrounds.Comment: 12 pages, phyzz

    On the B\"acklund Transformation for the Moyal Korteweg-de Vries Hierarchy

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    We study the B\"acklund symmetry for the Moyal Korteweg-de Vries (KdV) hierarchy based on the Kuperschmidt-Wilson Theorem associated with second Gelfand-Dickey structure with respect to the Moyal bracket, which generalizes the result of Adler for the ordinary KdV.Comment: 9 pages, Revte

    Dispersionful analogues of Benney's equations and NN-wave systems

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    We recall Krichever's construction of additional flows to Benney's hierarchy, attached to poles at finite distance of the Lax operator. Then we construct a ``dispersionful'' analogue of this hierarchy, in which the role of poles at finite distance is played by Miura fields. We connect this hierarchy with NN-wave systems, and prove several facts about the latter (Lax representation, Chern-Simons-type Lagrangian, connection with Liouville equation, τ\tau-functions).Comment: 12 pages, latex, no figure

    Nonstandard Drinfeld-Sokolov reduction

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    Subject to some conditions, the input data for the Drinfeld-Sokolov construction of KdV type hierarchies is a quadruplet (\A,\Lambda, d_1, d_0), where the did_i are Z\Z-gradations of a loop algebra \A and \Lambda\in \A is a semisimple element of nonzero d1d_1-grade. A new sufficient condition on the quadruplet under which the construction works is proposed and examples are presented. The proposal relies on splitting the d1d_1-grade zero part of \A into a vector space direct sum of two subalgebras. This permits one to interpret certain Gelfand-Dickey type systems associated with a nonstandard splitting of the algebra of pseudo-differential operators in the Drinfeld-Sokolov framework.Comment: 19 pages, LaTeX fil

    Conformal Covariantization of Moyal-Lax Operators

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    A covariant approach to the conformal property associated with Moyal-Lax operators is given. By identifying the conformal covariance with the second Gelfand-Dickey flow, we covariantize Moyal-Lax operators to construct the primary fields of one-parameter deformation of classical WW-algebras.Comment: 13 pages, Revtex, no figures, v.2: typos corrected, references added and conclusion modifie
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