1,326 research outputs found

    Nonperturbative Matching for Field Theories with Heavy Fermions

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    We examine a paradox, suggested by Banks and Dabholkar, concerning nonperturbative effects in an effective field theory which is obtained by integrating out a generation of heavy fermions, where the heavy fermion masses arise from Yukawa couplings. They argue that light fermions in the effective theory appear to decay via instanton processes, whereas their decay is forbidden in the full theory. We resolve this paradox by showing that such processes in fact do not occur in the effective theory, due to matching corrections which cause the relevant light field configurations to have infinite action.Comment: 10 pages, no figures, uses harvmac, Harvard University Preprint HUTP-93/A03

    De Sitter Waves and the Zero Curvature Limit

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    We show that a particular set of global modes for the massive de Sitter scalar field (the de Sitter waves) allows to manage the group representations and the Fourier transform in the flat (Minkowskian) limit. This is in opposition to the usual acceptance based on a previous result, suggesting the appearance of negative energy in the limit process. This method also confirms that the Euclidean vacuum, in de Sitter spacetime, has to be preferred as far as one wishes to recover ordinary QFT in the flat limit.Comment: 9 pages, latex no figure, to appear in Phys. Rev.

    Vacuum Ambiguity in de Sitter Space at Strong Coupling

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    It is well known that in the weak coupling regime, quantum field theories in de Sitter space do not have a unique vacuum, but a class of vacua parametrized by a complex parameter α\alpha, i.e., the so-called α\alpha-vacua. In this article, using gauge/gravity duality, we calculate the symmetric two-point function of strongly coupled N=4{\cal N}=4 supersymmetric Yang-Mills theory on dS3dS_3. We find that there is a class of de Sitter invariant vacua, parametrized by a set of complex parameters {αν}\{\alpha_{\nu}\}.Comment: 17 pages in JHEP style, references adde

    Color-Octet Charmonium Production in Top Quark Decays

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    We calculate the direct production rate of J/ψJ/\psi in top quark decays. The color-octet J/ψJ/\psi production via tW+bJ/ψt\rightarrow W^+ b J/\psi is shown to have a large branching ratio of order 1.5×1041.5\times 10^{-4}, which is over an order of magnitude higher than that of the color-singlet J/ψJ/\psi production via tW+bJ/ψ g gt\rightarrow W^+ b J/\psi~g~g or tW+b χcJ gt\rightarrow W^+ b~\chi_{cJ}~g followed by χcJJ/ψ γ\chi_{cJ}\rightarrow J/\psi~\gamma. This result can be used as a powerful tool to test the importance of the color-octet mechanism in heavy quarkonium production.Comment: 10 pages LaTex (2 figures in PS-file

    Boson--fermion bound states in two dimensional QCD

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    We derive the boson--fermion bound state equation in a two dimensional gauge theory in the large--\nc limit. We analyze the properties of this equation and in particular, find that the mass trajectory is linear with respect to the bound state level for the higher mass states.Comment: 5pp, 2 figs (as a separate file), TIT/HEP-23

    On Thermalization in de Sitter Space

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    We discuss thermalization in de Sitter space and argue, from two different points of view, that the typical time needed for thermalization is of order R3/lpl2R^{3}/l_{pl}^{2}, where RR is the radius of the de Sitter space in question. This time scale gives plenty of room for non-thermal deviations to survive during long periods of inflation. We also speculate in more general terms on the meaning of the time scale for finite quantum systems inside isolated boxes, and comment on the relation to the Poincar\'{e} recurrence time.Comment: 14 pages, 2 figures, latex, references added. Improved discussion in section 3 adde

    CP violation in gauge theories

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    We define the CP transformation properties of scalars, fermions and vectors in a gauge theory and show that only three types of interactions can lead to CP violation: scalar interactions, fermion-scalar interactions and FF~ F \tilde F associated with the strong CP problem and which involve only the gauge fields. For technicolor theories this implies the absence of CP violation within perturbation theory.Comment: 5 pages, 1 figure, revtex and epsf require

    Production of neutral scalar Higgs bosons at eγe\gamma colliders

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    We study the production of neutral scalar (CP even) Higgs bosons in the process eγehe\gamma\to e h by including supersymmetric corrections to the dominant tt-channel photon exchange amplitude. In addition to the standard model W±W^{\pm} and fermion loops, there are substantial contributions from chargino loops. For some cases, these contributions can exceed those of the WW's and ordinary fermions. The cross sections in this channel are generally one or two orders of magnitude larger than those in the related channel eeˉγhe\bar{e}\to\gamma h.Comment: 12 pages RevTeX, 5 postscript figures included, uses epsf.st

    On the consistency of de Sitter vacua

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    In this paper the consistency of the de Sitter invariant α\alpha -vacua, which have been introduced as simple tools to study the effects of transplanckian physics, is investigated. In particular possible non renormalization problems are discussed, as well as non standard properties of Greens functions. We also discuss the non thermal properties of the α\alpha -vacua and the necessity of α\alpha to change. The conclusion is that non of these problems necessarily exclude an application of the α\alpha -vacua to inflation.Comment: 12 pages, v2: minor clarifications and corrections to reference

    Topological Excitations in Compact Maxwell-Chern-Simons Theory

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    We construct a lattice model of compact (2+1)-dimensional Maxwell-Chern- Simons theory, starting from its formulation in terms of gauge invariant quantities proposed by Deser and Jackiw. We thereby identify the topological excitations and their interactions. These consist of monopolo- antimonopole pairs bounded by strings carrying both magnetic flux and electric charge. The electric charge renders the Dirac strings observable and endows them with a finite energy per unit length, which results in a linearly confining string tension. Additionally, the strings interact via an imaginary, topological term measuring the (self-) linking number of closed strings.Comment: harvmac, CERN-TH. 6906/93, DFUPG 80/9
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