115 research outputs found

    Relations Between Low-lying Quantum Wave Functions and Solutions of the Hamilton-Jacobi Equation

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    We discuss a new relation between the low lying Schroedinger wave function of a particle in a one-dimentional potential V and the solution of the corresponding Hamilton-Jacobi equation with -V as its potential. The function V is ≄0\geq 0, and can have several minina (V=0). We assume the problem to be characterized by a small anhamornicity parameter g−1g^{-1} and a much smaller quantum tunneling parameter Ï”\epsilon between these different minima. Expanding either the wave function or its energy as a formal double power series in g−1g^{-1} and Ï”\epsilon, we show how the coefficients of g−mÏ”ng^{-m}\epsilon^n in such an expansion can be expressed in terms of definite integrals, with leading order term determined by the classical solution of the Hamilton-Jacobi equation. A detailed analysis is given for the particular example of quartic potential V=1/2g2(x2−a2)2V={1/2}g^2(x^2-a^2)^2.Comment: LaTex, 48 pages, no figur

    Monopole Spectra in non-Abelian Gauge Theories

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    We study the continuum limit of the length spectrum of magnetic monopole structures found after various Abelian projections of pure gauge SU(2), including the maximally Abelian gauge. We comment on Gribov copies, and measurements of the string tension.Comment: Talk presented at LATTICE96(topology) LaTeX, with 4 LaTeX figure

    Anomalous gauge couplings of the Higgs boson at high energy photon colliders

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    We study the sensitivity of testing the anomalous gauge couplings gHVVg_{HVV}'s of the Higgs boson in the formulation of linearly realized gauge symmetry via the processes γγ→ZZ\gamma\gamma\to ZZ and γγ→WWWW\gamma\gamma\to WWWW at polarized and unpolarized photon colliders based on e+e−e^+e^- linear colliders of c.m.~energies 500 GeV, 1 TeV, and 3 TeV. Signals beyond the standard model (SM) and SM backgrounds are carefully studied. We propose certain kinematic cuts to suppress the standard model backgrounds. For an integrated luminosity of 1 ab−1^{-1}, we show that (a) γγ→ZZ\gamma\gamma\to ZZ can provide a test of gHγγg_{H\gamma\gamma} to the 3σ3\sigma sensitivity of O(10−3−10−2)O(10^{-3}-10^{-2}) TeV−1^{-1} at a 500 GeV ILC, and O(10−3)O(10^{-3}) TeV−1^{-1} at a 1 TeV ILC and a 3 TeV CLIC, and (b) γγ→WWWW\gamma\gamma\to WWWW at a 3 TeV CLIC can test all the anomalous couplings gHVVg_{HVV}'s to the 3σ3\sigma sensitivity of O(10−3−10−2)O(10^{-3}-10^{-2}) TeV−1^{-1}.Comment: 30 pages, 17 figure

    Brane-induced Skyrmion on S^3: baryonic matter in holographic QCD

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    We study baryonic matter in holographic QCD with D4/D8/\bar{D8} multi-D brane system in type IIA superstring theory. The baryon is described as the "brane-induced Skyrmion", which is a topologically non-trivial chiral soliton in the four-dimensional meson effective action induced by holographic QCD. We employ the "truncated-resonance model" approach for the baryon analysis, including pion and \rho meson fields below the ultraviolet cutoff scale M_KK \sim 1GeV, to keep the holographic duality with QCD. We describe the baryonic matter in large N_c as single brane-induced Skyrmion on the three-dimensional closed manifold S^3 with finite radius R. The interactions between baryons are simulated by the curvature of the closed manifold S^3, and the decrease of the size of S^3 represents the increase of the total baryon-number density in the medium in this modeling. We investigate the energy density, the field configuration, the mass and the root-mean-square radius of single baryon on S^3 as the function of its radius R. We find a new picture of "pion dominance" near the critical density in the baryonic matter, where all the (axial) vector meson fields disappear and only the pion field survive. We also find the "swelling" phenomena of the baryons as the precursor of the deconfinement, and propose the mechanism of the swelling in general context of QCD. The properties of the deconfinement and the chiral symmetry restoration in the baryonic matter are examined by taking the proper order parameters. We also compare our truncated-resonance model with another "instanton" description of the baryon in holographic QCD, considering the role of cutoff scale M_KK.Comment: 25 pages, 12 figure

    Introduction to light cone field theory and high energy scattering

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    In this set of four lectures, we provide an elementary introduction to light cone field theory and some of its applications in high energy scattering.Comment: 28 pages, LaTeX, invited lectures at Cape Town summer school in theoretical physic

    SU(N)-Gauge Theories in Polyakov Gauge on the Torus

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    We investigate the Abelian projection with respect to the Polyakov loop operator for SU(N) gauge theories on the four torus. The gauge fixed A0A_0 is time-independent and diagonal. We construct fundamental domains for A0A_0. In sectors with non-vanishing instanton number such gauge fixings are always singular. The singularities define the positions of magnetically charged monopoles, strings or walls. These magnetic defects sit on the Gribov horizon and have quantized magnetic charges. We relate their magnetic charges to the instanton number.Comment: 11 pages, 2 figure

    What is the order of the deconfining phase transition?

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    The techniques are discussed by which the order of the deconfining phase transition is investigated on the lattice. QCD with Nf=2N_f=2 is a special case, which can provide information on the mechanism of confinement.Comment: Talk at QCD 2003, Montpellier, July 2003, to appear in the proceedings. 4 pages, 1 figur

    General massive gauge theory

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    The concept of perturbative gauge invariance formulated exclusively by means of asymptotic fields is used to construct massive gauge theories. We consider the interactions of rr massive and ss massless gauge fields together with (r+s)(r+s) fermionic ghost and anti-ghost fields. First order gauge invariance requires the introduction of unphysical scalars (Goldstone bosons) and fixes their trilinear couplings. At second order additional physical scalars (Higgs fields) are necessary, their coupling is further restricted at third order. In case of one physical scalar all couplings are determined by gauge invariance, including the Higgs potential. For three massive and one massless gauge field the SU(2)×U(1)SU(2)\times U(1) electroweak theory comes out as the unique solution.Comment: 20 pages, latex, no figure

    Time-dependent quantum scattering in 2+1 dimensional gravity

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    The propagation of a localized wave packet in the conical space-time created by a pointlike massive source in 2+1 dimensional gravity is analyzed. The scattering amplitude is determined and shown to be finite along the classical scattering directions due to interference between the scattered and the transmitted wave functions. The analogy with diffraction theory is emphasized.Comment: 15 pages in LaTeX with 3 PostScript figure

    Color confinement and dual superconductivity in unquenched QCD

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    We report on evidence from lattice simulations that confinement is produced by dual superconductivity of the vacuum in full QCD as in quenched QCD. Preliminary information is obtained on the order of the deconfining phase transition.Comment: 4 pages, to appear in the Proceedings of Quark Matter 02 - The XVI International Conference on Ultrarelativistic Nucleus-Nucleus Collision
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