118 research outputs found

    0++0^{++} Resonances Observed at BES

    Full text link
    In last 10 years, 0++0^{++} resonances have been observed and studied at BES in many processes, such as J/ψ→γπ+π−π+π−J/\psi\to\gamma\pi^+\pi^-\pi^+\pi^-, γπ+π−\gamma\pi^+\pi^-, γπ0π0\gamma\pi^0\pi^0, γK+K−\gamma K^+K^-, γKSKS\gamma K_SK_S, γωϕ\gamma\omega\phi, ωπ+π−\omega\pi^+\pi^-, ωK+K−\omega K^+K^-, ϕπ+π−\phi\pi^+\pi^-, ϕK+K−\phi K^+K^-, ψ(2S)→J/ψπ+π−\psi(2S)\to J/\psi\pi^+\pi^-, χc0→π+π−K+K−\chi_{c0}\to\pi^+\pi^-K^+K^-, π+π−π+π−\pi^+\pi^-\pi^+\pi^- etc.. The results on 0++0^{++} resonances observed at BES are reviewed.Comment: Plenary talk at SCADRON70, Lisbon, Feb. 200

    On (non-Hermitian) Lagrangeans in (particle) physics and their dynamical generation

    Full text link
    On the basis of a new method to derive the effective action the nonperturbative concept of "dynamical generation" is explained. A non-trivial, non-Hermitian and PT-symmetric solution for Wightman's scalar field theory in four dimensions is dynamically generated, rehabilitating Symanzik's precarious phi**4-theory with a negative quartic coupling constant as a candidate for an asymptotically free theory of strong interactions. Finally it is shown making use of dynamically generation that a Symanzik-like field theory with scalar confinement for the theory of strong interactions can be even suggested by experiment.Comment: 12 pages, no figures, accepted for publication in Czech.J.Phys., revised with respect to obvious typo

    D^+ \to K^- \p^+ \p^+ : the low-energy sector

    Full text link
    An effective SU(3)×SU(3)SU(3)\times SU(3) chiral lagrangian, which includes scalar resonances, is used to describe the process D^+ \rar K^- \p^+ \p^+ at low-energies. Our main result is a set of five SS-wave amplitudes, suited to be used in analyses of production data.Comment: Talk given at SCADRON 70 - Workshop on Scalar Mesons and Related Topics - Lisbon - February 200

    Ãœberwachung der Kfz-Emissionen im realen Verkehr, Methoden und Ergebnisse

    Get PDF
    Systematic monitoring of real driving emissions from vehicles started in the 1990’ies with measurements for the Handbook on Emission factors (HBEFA, http://www.hbefa.net/e/index.html). From 2000 to 2005, a European consortium improved the methods for vehicle testing and evaluation in the EU FP7 Project ARTEMIS. Results from this project are e.g. the ARTEMIS driving cycle (CADC), frequently used for real world LDVs chassis dyno tests, and the ERMES data base, where test results from independent European labs are brought together. Based on the ARTEMIS core consortium, the ERMES group was established (http://www.ermes-group.eu/web/). The ERMES group consists of laboratories, funding organisations and researchers dealing with emission testing with PEMS and on the dynamometer, with remote sensing measurement and with corresponding analysis of measures and technologies to reduce emissions and energy consumption of road vehicles and mobile machines. While the ERMES database on real world tests had only a limited number of cars until HBEFA version 3.1 (e.g. 24 different EURO 5 diesel cars measured), the available data significantly increased during the last 3 years (e.g. covering today 101 EURO 5 and 85 EURO 6 diesel cars). Also for HDVs and 2-wheelers the number of measured vehicles increased significantly after the recent discussions on real world NOx emissions from diesel LDVs. Parallel to the conventional vehicle tests also remote sensing has been systematically developed for vehicle emission monitoring. Remote sensing measures the incremental concentration of gases in the exhaust plume of passing vehicles and thus provides mass emissions per mass of CO2. The number plate is used to identify make and model, engine type, year of registration and emission standard. This information is then associated with the measured instantaneous emissions. Since remote sensing measures thousands of vehicles per day, the data is very useful for the analysis of trends, which need a high number of vehicles to be representative. E.g., Remote Sensing can monitor aging and temperature influences and emission levels per EURO class, brand and possibly vehicle model also as basis for the selection of vehicles for more detailed instrumented tests. The paper describes the methods developed for the monitoring and evaluation and shows actual trends in vehicle emissions

    Phenomenology of pp->pp eta reaction close to threshold

    Full text link
    The recent high statistics measurement of the pp -> pp eta reaction at an excess energy Q=15.5 MeV has been analysed by means of partial wave decomposition of the cross section. Guided by the dominance of the final state 1S0 pp interaction (FSI), we keep only terms involving the FSI enhancement factor. The measured p-p and p-eta effective mass spectra can be well reproduced by lifting the standard on-shell approximation in the enhancement factor and by allowing for a linear energy dependence in the leading 3P0->1S0,s partial wave amplitude. Higher partial waves seem to play only a marginal role

    General Aspects of PT-Symmetric and P-Self-Adjoint Quantum Theory in a Krein Space

    Get PDF
    In our previous work, we proposed a mathematical framework for PT-symmetric quantum theory, and in particular constructed a Krein space in which PT-symmetric operators would naturally act. In this work, we explore and discuss various general consequences and aspects of the theory defined in the Krein space, not only spectral property and PT symmetry breaking but also several issues, crucial for the theory to be physically acceptable, such as time evolution of state vectors, probability interpretation, uncertainty relation, classical-quantum correspondence, completeness, existence of a basis, and so on. In particular, we show that for a given real classical system we can always construct the corresponding PT-symmetric quantum system, which indicates that PT-symmetric theory in the Krein space is another quantization scheme rather than a generalization of the traditional Hermitian one in the Hilbert space. We propose a postulate for an operator to be a physical observable in the framework.Comment: 32 pages, no figures; explanation, discussion and references adde

    Remarks on the f_0(400-1200) scalar meson as the dynamically generated chiral partner of the pion

    Get PDF
    The quark-level linear sigma model is revisited, in particular concerning the identification of the f_0(400-1200) (or \sigma(600)) scalar meson as the chiral partner of the pion. We demonstrate the predictive power of the linear sigma model through the pi-pi and pi-N s-wave scattering lengths, as well as several electromagnetic, weak, and strong decays of pseudoscalar and vector mesons. The ease with which the data for these observables are reproduced in the linear sigma model lends credit to the necessity to include the sigma as a fundamental q\bar{q} degree of freedom, to be contrasted with approaches like chiral perturbation theory or the confining NJL model of Shakin and Wang.Comment: 15 pages, plain LaTeX, 3 EPS figure

    Vacuum Stability of the wrong sign (−ϕ6)(-\phi^{6}) Scalar Field Theory

    Full text link
    We apply the effective potential method to study the vacuum stability of the bounded from above (−ϕ6)(-\phi^{6}) (unstable) quantum field potential. The stability (∂E/∂b=0)\partial E/\partial b=0) and the mass renormalization (∂2E/∂b2=M2)\partial^{2} E/\partial b^{2}=M^{2}) conditions force the effective potential of this theory to be bounded from below (stable). Since bounded from below potentials are always associated with localized wave functions, the algorithm we use replaces the boundary condition applied to the wave functions in the complex contour method by two stability conditions on the effective potential obtained. To test the validity of our calculations, we show that our variational predictions can reproduce exactly the results in the literature for the PT\mathcal{PT}-symmetric ϕ4\phi^{4} theory. We then extend the applications of the algorithm to the unstudied stability problem of the bounded from above (−ϕ6)(-\phi^{6}) scalar field theory where classical analysis prohibits the existence of a stable spectrum. Concerning this, we calculated the effective potential up to first order in the couplings in dd space-time dimensions. We find that a Hermitian effective theory is instable while a non-Hermitian but PT\mathcal{PT}-symmetric effective theory characterized by a pure imaginary vacuum condensate is stable (bounded from below) which is against the classical predictions of the instability of the theory. We assert that the work presented here represents the first calculations that advocates the stability of the (−ϕ6)(-\phi^{6}) scalar potential.Comment: 21pages, 12 figures. In this version, we updated the text and added some figure

    Solvability and PT-symmetry in a double-well model with point interactions

    Full text link
    We show that and how point interactions offer one of the most suitable guides towards a quantitative analysis of properties of certain specific non-Hermitian (usually called PT-symmetric) quantum-mechanical systems. A double-well model is chosen, an easy solvability of which clarifies the mechanisms of the unavoided level crossing and of the spontaneous PT-symmetry breaking. The latter phenomenon takes place at a certain natural boundary of the domain of the "acceptable" parameters of the model. Within this domain the model mediates a nice and compact explicit illustration of the not entirely standard probabilistic interpretation of the physical bound states in the very recently developed (so called PT symmetric or, in an alternative terminology, pseudo-Hermitian) new, fairly exciting and very quickly developing branch of Quantum Mechanics.Comment: 24 p., written for the special journal issue "Singular Interactions in Quantum Mechanics: Solvable Models". Will be also presented to the int. conference "Pseudo-Hermitian Hamiltonians in Quantum Physics III" (Instanbul, Koc University, June 20 - 22, 2005) http://home.ku.edu.tr/~amostafazadeh/workshop/workshop.ht
    • …
    corecore