12,950 research outputs found

    NLO-QCD corrections to e+ e- --> hadrons in models of TeV-scale gravity

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    We present results on NLO-QCD corrections to the process e+ e- --> hadrons via photon-, Z- and graviton-exchange in the context of TeV-scale gravity models. The quantitative impact of these QCD corrections for searches of extra dimensions at a Linear Collider is briefly discussed.Comment: 10 pages, LaTeX, using axodraw.st

    Higgs Bosons: Intermediate Mass Range at e+e- Colliders

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    We elaborate on the production of the Standard Model Higgs particle at high-energy e+ee^+e^- colliders through the reaction e+eZHe^+e^- \rightarrow ZH. Particular emphasis is put on the intermediate mass range. In addition to the signal we discuss in detail the background processes. Angular distributions which are sensitive to the spin and parity of the Higgs particle are analyzed.Comment: Standard Latex. 15 pages. 11 figures available by fax or regular mail. MAD/PH/749, DESY 93-064, UdeM-LPN-TH-93-143, NUHEP-TH-93-1

    Perturbative QCD Fragmentation Functions for Production of P-wave Mesons with Charm and Beauty

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    We calculate the leading order QCD fragmentation functions for the production of PP-wave charmed beauty mesons. Long-distance effects are factored into two nonperturbative parameters: the derivative of the radial wavefunction at the origin and a second parameter related to the probability for a (bˉc)(\bar b c) heavy quark pair that is produced in a color-octet SS-wave state to form a color-singlet PP-wave bound state. The four 2P2P states and those 3P3P states which lie below the BDBD flavor threshold eventually all decay into the 1S1S ground state BcB_c through hadronic cascades or by emitting photons. The total fragmentation probabilities for production of the 1S1S ground state BcB_c from the cascades of the 2P2P and 3P3P states are about 1.7×1041.7 \times 10^{-4} and 2.3×1042.3 \times 10^{-4} respectively. Thus the direct production of the PP-wave states via fragmentation may account for a significant fraction of the inclusive production rate of the BcB_c at large transverse momentum in high energy colliders. Our analytic results for the PP-wave fragmentation functions disagree with those obtained earlier in the literature.Comment: 31 pages, Latex file, 1 figure (postscript file appended at the end

    Re-parameterization Invariance in Fractional Flux Periodicity

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    We analyze a common feature of a nontrivial fractional flux periodicity in two-dimensional systems. We demonstrate that an addition of fractional flux can be absorbed into re-parameterization of quantum numbers. For an exact fractional periodicity, all the electronic states undergo the re-parameterization, whereas for an approximate periodicity valid in a large system, only the states near the Fermi level are involved in the re-parameterization.Comment: 4 pages, 1 figure, minor changes, final version to appear in J. Phys. Soc. Jp

    Chandra X-ray Observations of the Two Brightest Unidentified High Galactic Latitude Fermi-LAT gamma-ray Sources

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    We present Chandra ACIS-I X-ray observations of 0FGL J1311.9-3419 and 0FGL J1653.4-0200, the two brightest high Galactic latitude (|b|>10 deg) gamma-ray sources from the 3 month Fermi-LAT bright source list that are still unidentified. Both were also detected previously by EGRET, and despite dedicated multi-wavelength follow-up, they are still not associated with established classes of gamma-ray emitters like pulsars or radio-loud active galactic nuclei. X-ray sources found in the ACIS-I fields of view are catalogued, and their basic properties are determined. These are discussed as candidate counterparts to 0FGL J1311.9-3419 and 0FGL J1653.4-0200, with particular emphasis on the brightest of the 9 and 13 Chandra sources detected within their respective Fermi-LAT 95% confidence regions. Further follow-up studies, including optical photometric and spectroscopic observations are necessary to identify these X-ray candidate counterparts in order to ultimately reveal the nature of these enigmatic gamma-ray objects.Comment: ApJ, accepted. 18 pages, 5 figure

    Hadronic Production of S-wave and P-wave Charmed Beauty Mesons via Heavy Quark Fragmentation

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    At hadron colliders the dominant production mechanism of (bˉc)(\bar bc) mesons with large transverse momentum is due to parton fragmentation. We compute the rates and transverse momentum spectra for production of S-wave and P-wave (bˉc)(\bar b c) mesons at the Tevatron via the direct fragmentation of the bottom antiquark as well as the Altarelli-Parisi induced gluon fragmentation. Since all the radially and orbitally excited (bˉc)(\bar b c) mesons below the BDBD flavor threshold will cascade into the pseudoscalar ground state BcB_c through electromagnetic and/or hadronic transitions, they all contribute to the inclusive production of BcB_c. The contributions of the excited S-wave and P-wave states to the inclusive production of BcB_c are 58 and 23\%, respectively, and hence significant.Comment: Changes are made in the Discussio

    The WW Boson Loop Background to H -> ZZ at Photon-photon Colliders

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    We have performed a complete one-loop calculation of γγZZ\gamma \gamma \rightarrow ZZ in the Standard Model, including both gauge bosons and fermions in the loop. We confirm the large irreducible continuum background from the WW-boson loop found by Jikia. We have included the photon-photon luminosity, and find that the continuum background of transverse ZZ boson pairs prohibits finding a heavy Higgs with mass \gtap 350 GeV in this decay mode.Comment: 16 pages + 4 PS figures included (uuencoded), MAD/PH/77

    Relativistic field theories in a magnetic background as noncommutative field theories

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    We study the connection of the dynamics in relativistic field theories in a strong magnetic field with the dynamics of noncommutative field theories (NCFT). As an example, the Nambu-Jona-Lasinio models in spatial dimensions d2d \geq 2 are considered. We show that this connection is rather sophisticated. In fact, the corresponding NCFT are different from the conventional ones considered in the literature. In particular, the UV/IR mixing is absent in these theories. The reason of that is an inner structure (i.e., dynamical form-factors) of neutral composites which plays an important role in providing consistency of the NCFT. An especially interesting case is that for a magnetic field configuration with the maximal number of independent nonzero tensor components. In that case, we show that the NCFT are finite for even dd and their dynamics is quasi-(1+1)-dimensional for odd dd. For even dd, the NCFT describe a confinement dynamics of charged particles. The difference between the dynamics in strong magnetic backgrounds in field theories and that in string theories is briefly discussed.Comment: 19 pages, REVTeX4, clarifications added, references added, to appear in Phys. Rev.

    The consistency condition for the three-point function in dissipative single-clock inflation

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    We generalize the consistency condition for the three-point function in single field inflation to the case of dissipative, multi-field, single-clock models. We use the recently introduced extension of the effective field theory of inflation that accounts for dissipative effects, to provide an explicit proof to leading (non-trivial) order in the generalized slow roll parameters and mixing with gravity scales. Our results illustrate the conditions necessary for the validity of the consistency relation in situations with many degrees of freedom relevant during inflation, namely that there is a preferred clock. Departures from this condition in forthcoming experiments would rule out not only single field but also a large class of multi-field models.Comment: 26+11 page

    Persistent Currents in Quantum Chaotic Systems

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    The persistent current of ballistic chaotic billiards is considered with the help of the Gutzwiller trace formula. We derive the semiclassical formula of a typical persistent current ItypI^{typ} for a single billiard and an average persistent current for an ensemble of billiards at finite temperature. These formulas are used to show that the persistent current for chaotic billiards is much smaller than that for integrable ones. The persistent currents in the ballistic regime therefore become an experimental tool to search for the quantum signature of classical chaotic and regular dynamics.Comment: 4 pages (RevTex), to appear in Phys. Rev. B, No.59, 12256-12259 (1999
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