2,864 research outputs found

    Light-Cone Quantization of the Liouville Model

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    We present the quantization of the Liouville model defined in light-cone coordinates in (1,1) signature space. We take advantage of the representation of the Liouville field by the free field of the Backl\"{u}nd transformation and adapt the approch by Braaten, Curtright and Thorn. Quantum operators of the Liouville field ∂+ϕ\partial_{+}\phi, ∂−ϕ\partial_{-}\phi, egϕe^{g\phi}, e2gϕe^{2g\phi} are constructed consistently in terms of the free field. The Liouville model field theory space is found to be restricted to the sector with field momentum P+=−P−P_{+}=-P_{-}, P+>0P_{+}> 0 , which is a closed subspace for the Liouville theory operator algebra.Comment: 16 p, EFI-92-6

    Lotka--Volterra Type Equations and their Explicit Integration

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    In the present note we give an explicit integration of some two--dimensionalised Lotka--Volterra type equations associated with simple Lie algebras, other than the familiar AnA_n case, possessing a representation without branching. This allows us, in particular, to treat the first fundamental representations of ArA_r, BrB_r, CrC_r, and G2G_2 on the same footing.Comment: 3 pages LATEX fil

    Scattering Mechanism in Modulation-Doped Shallow Two-Dimensional Electron Gases

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    We report on a systematic investigation of the dominant scattering mechanism in shallow two-dimensional electron gases (2DEGs) formed in modulation-doped GaAs/Al_{x}Ga_{1-x}As heterostructures. The power-law exponent of the electron mobility versus density, mu \propto n^{alpha}, is extracted as a function of the 2DEG's depth. When shallower than 130 nm from the surface, the power-law exponent of the 2DEG, as well as the mobility, drops from alpha \simeq 1.65 (130 nm deep) to alpha \simeq 1.3 (60 nm deep). Our results for shallow 2DEGs are consistent with theoretical expectations for scattering by remote dopants, in contrast to the mobility-limiting background charged impurities of deeper heterostructures.Comment: 4 pages, 3 figures, modified version as accepted in AP

    Soliton quantization and internal symmetry

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    We apply the method of collective coordinate quantization to a model of solitons in two spacetime dimensions with a global U(1)U(1) symmetry. In particular we consider the dynamics of the charged states associated with rotational excitations of the soliton in the internal space and their interactions with the quanta of the background field (mesons). By solving a system of coupled saddle-point equations we effectively sum all tree-graphs contributing to the one-point Green's function of the meson field in the background of a rotating soliton. We find that the resulting one-point function evaluated between soliton states of definite U(1)U(1) charge exhibits a pole on the meson mass shell and we extract the corresponding S-matrix element for the decay of an excited state via the emission of a single meson using the standard LSZ reduction formula. This S-matrix element has a natural interpretation in terms of an effective Lagrangian for the charged soliton states with an explicit Yukawa coupling to the meson field. We calculate the leading-order semi-classical decay width of the excited soliton states discuss the consequences of these results for the hadronic decay of the Δ\Delta resonance in the Skyrme model.Comment: 23 pages, LA-UR-93-299

    Correlation functions in super Liouville theory

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    We calculate three- and four-point functions in super Liouville theory coupled to super Coulomb gas on world sheets with spherical topology. We first integrate over the zero mode and assume that a parameter takes an integer value. After calculating the amplitudes, we formally continue the parameter to an arbitrary real number. Remarkably the result is completely parallel to the bosonic case, the amplitudes being of the same form as those of the bosonic case.Comment: 11 page

    Photon Production from a Quark-Gluon-Plasma at Finite Baryon Chemical Potential

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    We compute the photon production of a QCD plasma at leading order in the strong coupling with a finite baryon chemical potential. Our approach starts from the real time formalism of finite temperature field theory. We identify the class of diagrams contributing at leading order when a finite chemical potential is added and resum them to perform a full treatment of the LPM effect similar to the one performed by Arnold, Moore, and Yaffe at zero chemical potential. Our results show that the contribution of 2↦32\mapsto 3 and 3↦23\mapsto 2 processes grows as the chemical potential grows.Comment: 28 pages, 14 figure

    Free fields via canonical transformations of matter-coupled 2D dilaton gravity models

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    It is shown that the 1+1-dimensional matter-coupled Jackiw-Teitelboim model and the model with an exponential potential can be converted by means of appropriate canonical transformations into a bosonic string theory propagating on a flat target space with an indefinite signature. This makes it possible to consistently quantize these models in the functional Schroedinger representation thus generalizing recent results on CGHS theory.Comment: 15 pages, Late

    Multi-Component KdV Hierarchy, V-Algebra and Non-Abelian Toda Theory

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    I prove the recently conjectured relation between the 2×22\times 2-matrix differential operator L=∂2−UL=\partial^2-U, and a certain non-linear and non-local Poisson bracket algebra (VV-algebra), containing a Virasoro subalgebra, which appeared in the study of a non-abelian Toda field theory. Here, I show that this VV-algebra is precisely given by the second Gelfand-Dikii bracket associated with LL. The Miura transformation is given which relates the second to the first Gelfand-Dikii bracket. The two Gelfand-Dikii brackets are also obtained from the associated (integro-) differential equation satisfied by fermion bilinears. The asymptotic expansion of the resolvent of (L−ξ)Ψ=0(L-\xi)\Psi=0 is studied and its coefficients RlR_l yield an infinite sequence of hamiltonians with mutually vanishing Poisson brackets. I recall how this leads to a matrix KdV hierarchy which are flow equations for the three component fields T,V+,V−T, V^+, V^- of UU. For V±=0V^\pm=0 they reduce to the ordinary KdV hierarchy. The corresponding matrix mKdV equations are also given, as well as the relation to the pseudo- differential operator approach. Most of the results continue to hold if UU is a hermitian n×nn\times n-matrix. Conjectures are made about n×nn\times n-matrix mthm^{\rm th}-order differential operators LL and associated V(n,m)V_{(n,m)}-algebras.Comment: 20 pages, revised: several references to earlier papers on multi-component KdV equations are adde

    Quantum Hamilton-Jacobi equation

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    The nontrivial transformation of the phase space path integral measure under certain discretized analogues of canonical transformations is computed. This Jacobian is used to derive a quantum analogue of the Hamilton-Jacobi equation for the generating function of a canonical transformation that maps any quantum system to a system with a vanishing Hamiltonian. A formal perturbative solution of the quantum Hamilton-Jacobi equation is given.Comment: 4 pages, RevTe
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