50 research outputs found

    Rational approximation rate for the MĂŒntz system {xλn} with λn↘0

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    AbstractThe present paper establishes, by employing some new ideas, a nontrivial result of quantitative rational approximation rate for the MĂŒntz system {xλ n} in case λn↘0 as n → ∞

    Nonequilibrium Evolution of Correlation Functions: A Canonical Approach

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    We study nonequilibrium evolution in a self-interacting quantum field theory invariant under space translation only by using a canonical approach based on the recently developed Liouville-von Neumann formalism. The method is first used to obtain the correlation functions both in and beyond the Hartree approximation, for the quantum mechanical analog of the ϕ4\phi^{4} model. The technique involves representing the Hamiltonian in a Fock basis of annihilation and creation operators. By separating it into a solvable Gaussian part involving quadratic terms and a perturbation of quartic terms, it is possible to find the improved vacuum state to any desired order. The correlation functions for the field theory are then investigated in the Hartree approximation and those beyond the Hartree approximation are obtained by finding the improved vacuum state corrected up to O(λ2){\cal O}(\lambda^2). These correlation functions take into account next-to-leading and next-to-next-to-leading order effects in the coupling constant. We also use the Heisenberg formalism to obtain the time evolution equations for the equal-time, connected correlation functions beyond the leading order. These equations are derived by including the connected 4-point functions in the hierarchy. The resulting coupled set of equations form a part of infinite hierarchy of coupled equations relating the various connected n-point functions. The connection with other approaches based on the path integral formalism is established and the physical implications of the set of equations are discussed with particular emphasis on thermalization.Comment: Revtex, 32 pages; substantial new material dealing with non-equilibrium evolution beyond Hartree approx. based on the LvN formalism, has been adde

    The VEPP-5 injection complex modulator revision and operational experience

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    For the VEPP-5 injection complex klystrons (5045, SLAC Lab., USA) power supply the four modulators producing a pulse voltage of 23.5 kV, a current of 6.3 kA, a pulse-top-duration of 3.7 ”s are used. The modulator scheme designed over ten years ago has proved its reliability and let us to find out and study the weak spots of the modulators. The output voltage stability and pulse-to-pulse time jitter improvements are made. The results of the thyratrons TGI1-2500/50 and TGI1-5000/50A long-term exploitation in the VEPP-5 injection complex modulators are presented. The test results of the thyratron TGI1-2500/50 operating in the mode of more then twice pulse current overload at the nominal mode of modulator operation are also presented.Đ”Đ»Ń жОĐČĐ»Đ”ĐœĐœŃ ĐșĐ»Ń–ŃŃ‚Ń€ĐŸĐœŃ–ĐČ 5045 (ĐČĐžŃ€ĐŸĐ±ĐœĐžŃ†Ń‚ĐČĐŸ SLAC) Ń–ĐœĐ¶Đ”ĐșціĐčĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșсу ВЕПП-5 ĐČĐžĐșĐŸŃ€ĐžŃŃ‚ĐŸĐČуються ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Đž, Ń‰ĐŸ Ń„ĐŸŃ€ĐŒŃƒŃŽŃ‚ŃŒ Ń–ĐŒĐżŃƒĐ»ŃŒŃĐž ĐœĐ°ĐżŃ€ŃƒĐłĐŸŃŽ 23,5 ĐșВ, ŃŃ‚Ń€ŃƒĐŒĐŸĐŒ 6,3 ĐșА, троĐČалістю 3,7 ĐŒĐșс у ĐșŃ–Đ»ŃŒĐșĐŸŃŃ‚Ń– 4 штуĐș. ĐšĐŸĐœŃŃ‚Ń€ŃƒĐșція ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Ń–ĐČ, Ń€ĐŸĐ·Ń€ĐŸĐ±Đ»Đ”ĐœĐ° Đ±Đ»ĐžĐ·ŃŒĐșĐŸ 10 Ń€ĐŸĐșіĐČ Ń‚ĐŸĐŒŃƒ, ĐŽĐŸĐČДла сĐČĐŸŃŽ ĐœĐ°ĐŽŃ–ĐčĐœŃ–ŃŃ‚ŃŒ і, Ń€Đ°Đ·ĐŸĐŒ Đ· Ń‚ĐžĐŒ, ĐŽĐŸĐ·ĐČĐŸĐ»ĐžĐ»Đ° ĐČĐžĐČчото і ĐČояĐČото слабĐșі ĐŒŃ–ŃŃ†Ń ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Ń–ĐČ. ĐŸŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐ° Ń€ĐŸĐ±ĐŸŃ‚Đ° Đ· піЮĐČĐžŃ‰Đ”ĐœĐœŃ ŃŃ‚Đ°Đ±Ń–Đ»ŃŒĐœĐŸŃŃ‚Ń– ĐœĐ°ĐżŃ€ŃƒĐłĐž ĐœĐ° ĐșĐ»Ń–ŃŃ‚Ń€ĐŸĐœŃ–, Đ·ĐŒĐ”ĐœŃˆĐ”ĐœĐœŃŽ Ń‡Đ°ŃĐŸĐČĐŸĐłĐŸ Ń€ĐŸĐ·ĐșОЎу ĐČіЮ Ń–ĐŒĐżŃƒĐ»ŃŒŃŃƒ ĐŽĐŸ Ń–ĐŒĐżŃƒĐ»ŃŒŃŃƒ. ПроĐČĐŸĐŽŃŃ‚ŃŒŃŃ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž троĐČĐ°Đ»ĐŸŃ— Đ”ĐșŃĐżĐ»ŃƒĐ°Ń‚Đ°Ń†Ń–Ń— Ń‚ĐžŃ€Đ°Ń‚Ń€ĐŸĐœŃ–ĐČ ĐąĐ“Đ†1-2500/50 і бГІ1-5000/50 у ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Đ°Ń… ĐŽĐ»Ń жОĐČĐ»Đ”ĐœĐœŃ ĐșĐ»Ń–ŃŃ‚Ń€ĐŸĐœŃ–ĐČ 5045. ВоĐșĐ»Đ°ĐŽĐ”ĐœĐŸ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Đž Ń€Đ”ŃŃƒŃ€ŃĐœĐžŃ… іспотіĐČ Ń‚ĐžŃ€Đ°Ń‚Ń€ĐŸĐœĐ° бГІ1-2500/50 про Đ±Ń–Đ»ŃŒŃˆ ĐœŃ–Đ¶ ĐżĐŸĐŽĐČіĐčĐœĐŸĐŒŃƒ пДрДĐČĐ°ĐœŃ‚Đ°Đ¶Đ”ĐœĐœŃŽ ĐżĐŸ Đ°ĐŒĐżĐ»Ń–Ń‚ŃƒĐŽŃ– ŃŃ‚Ń€ŃƒĐŒŃƒ ĐČ ĐœĐŸĐŒŃ–ĐœĐ°Đ»ŃŒĐœĐŸĐŒŃƒ Ń€Đ”Đ¶ĐžĐŒŃ– Ń€ĐŸĐ±ĐŸŃ‚Đž ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Đ°.Đ”Đ»Ń ĐżĐžŃ‚Đ°ĐœĐžŃ ĐșĐ»ĐžŃŃ‚Ń€ĐŸĐœĐŸĐČ 5045 (ĐżŃ€ĐŸĐžĐ·ĐČĐŸĐŽŃŃ‚ĐČĐŸ SLAC) ĐžĐœĐ¶Đ”ĐșŃ†ĐžĐŸĐœĐœĐŸĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșса ВЭПП-5 ĐžŃĐżĐŸĐ»ŃŒĐ·ŃƒŃŽŃ‚ŃŃ ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Ń‹, Ń„ĐŸŃ€ĐŒĐžŃ€ŃƒŃŽŃ‰ĐžĐ” ĐžĐŒĐżŃƒĐ»ŃŒŃŃ‹ ĐœĐ°ĐżŃ€ŃĐ¶Đ”ĐœĐžĐ”ĐŒ 23,5 ĐșВ, Ń‚ĐŸĐșĐŸĐŒ 6,3 ĐșА, ĐŽĐ»ĐžŃ‚Đ”Đ»ŃŒĐœĐŸŃŃ‚ŃŒŃŽ 3,7 ĐŒĐșс ĐČ ĐșĐŸĐ»ĐžŃ‡Đ”ŃŃ‚ĐČĐ” 4 штуĐș. ĐšĐŸĐœŃŃ‚Ń€ŃƒĐșцоя ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€ĐŸĐČ, Ń€Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚Đ°ĐœĐœĐ°Ń ĐŸĐșĐŸĐ»ĐŸ 10 лДт ĐœĐ°Đ·Đ°ĐŽ, ĐŽĐŸĐșазала сĐČĐŸŃŽ ĐœĐ°ĐŽĐ”Đ¶ĐœĐŸŃŃ‚ŃŒ Đž, ĐČĐŒĐ”ŃŃ‚Đ” с Ń‚Đ”ĐŒ, ĐżĐŸĐ·ĐČĐŸĐ»ĐžĐ»Đ° ĐžĐ·ŃƒŃ‡ĐžŃ‚ŃŒ Đž ĐČыяĐČоть слабыД ĐŒĐ”ŃŃ‚Đ° ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€ĐŸĐČ. ĐŸŃ€ĐŸĐČĐ”ĐŽĐ”ĐœĐ° Ń€Đ°Đ±ĐŸŃ‚Đ° ĐżĐŸ ĐżĐŸĐČŃ‹ŃˆĐ”ĐœĐžŃŽ ŃŃ‚Đ°Đ±ĐžĐ»ŃŒĐœĐŸŃŃ‚Đž ĐœĐ°ĐżŃ€ŃĐ¶Đ”ĐœĐžŃ ĐœĐ° ĐșĐ»ĐžŃŃ‚Ń€ĐŸĐœĐ”, ŃƒĐŒĐ”ĐœŃŒŃˆĐ”ĐœĐžŃŽ ĐČŃ€Đ”ĐŒĐ”ĐœĐœĐŸĐłĐŸ Ń€Đ°Đ·Đ±Ń€ĐŸŃĐ° ĐŸŃ‚ ĐžĐŒĐżŃƒĐ»ŃŒŃĐ° Đș ĐžĐŒĐżŃƒĐ»ŃŒŃŃƒ. ПроĐČĐŸĐŽŃŃ‚ŃŃ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ ĐŽĐ»ĐžŃ‚Đ”Đ»ŃŒĐœĐŸĐč эĐșŃĐżĐ»ŃƒĐ°Ń‚Đ°Ń†ĐžĐž Ń‚ĐžŃ€Đ°Ń‚Ń€ĐŸĐœĐŸĐČ ĐąĐ“Đ˜1-2500/50 Đž бГИ1-5000/50 ĐČ ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Đ°Ń… ĐŽĐ»Ń ĐżĐžŃ‚Đ°ĐœĐžŃ ĐșĐ»ĐžŃŃ‚Ń€ĐŸĐœĐŸĐČ 5045. Đ˜Đ·Đ»ĐŸĐ¶Đ”ĐœŃ‹ Ń€Đ”Đ·ŃƒĐ»ŃŒŃ‚Đ°Ń‚Ń‹ Ń€Đ”ŃŃƒŃ€ŃĐœŃ‹Ń… ĐžŃĐżŃ‹Ń‚Đ°ĐœĐžĐč Ń‚ĐžŃ€Đ°Ń‚Ń€ĐŸĐœĐ° бГИ1-2500/50 про Đ±ĐŸĐ»Đ”Đ” Ń‡Đ”ĐŒ ĐŽĐČĐŸĐčĐœĐŸĐč ĐżĐ”Ń€Đ”ĐłŃ€ŃƒĐ·ĐșĐ” ĐżĐŸ Đ°ĐŒĐżĐ»ĐžŃ‚ŃƒĐŽĐ” Ń‚ĐŸĐșĐ° ĐČ ĐœĐŸĐŒĐžĐœĐ°Đ»ŃŒĐœĐŸĐŒ Ń€Đ”Đ¶ĐžĐŒĐ” Ń€Đ°Đ±ĐŸŃ‚Ń‹ ĐŒĐŸĐŽŃƒĐ»ŃŃ‚ĐŸŃ€Đ°

    Transverse phase-locking in fully frustrated Josephson junction arrays: a new type of fractional giant steps

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    We study, analytically and numerically, phase locking of driven vortex lattices in fully-frustrated Josephson junction arrays at zero temperature. We consider the case when an ac current is applied {\it perpendicular} to a dc current. We observe phase locking, steps in the current-voltage characteristics, with a dependence on external ac-drive amplitude and frequency qualitatively different from the Shapiro steps, observed when the ac and dc currents are applied in parallel. Further, the critical current increases with increasing transverse ac-drive amplitude, while it decreases for longitudinal ac-drive. The critical current and the phase-locked current step width, increase quadratically with (small) amplitudes of the ac-drive. For larger amplitudes of the transverse ac-signal, we find windows where the critical current is hysteretic, and windows where phase locking is suppressed due to dynamical instabilities. We characterize the dynamical states around the phase-locking interference condition in the IVIV curve with voltage noise, Lyapunov exponents and Poincar\'e sections. We find that zero temperature phase-locking behavior in large fully frustrated arrays is well described by an effective four plaquette model.Comment: 12 pages, 11 figure

    Dragon-kings: mechanisms, statistical methods and empirical evidence

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    This introductory article presents the special Discussion and Debate volume "From black swans to dragon-kings, is there life beyond power laws?" published in Eur. Phys. J. Special Topics in May 2012. We summarize and put in perspective the contributions into three main themes: (i) mechanisms for dragon-kings, (ii) detection of dragon-kings and statistical tests and (iii) empirical evidence in a large variety of natural and social systems. Overall, we are pleased to witness significant advances both in the introduction and clarification of underlying mechanisms and in the development of novel efficient tests that demonstrate clear evidence for the presence of dragon-kings in many systems. However, this positive view should be balanced by the fact that this remains a very delicate and difficult field, if only due to the scarcity of data as well as the extraordinary important implications with respect to hazard assessment, risk control and predictability.Comment: 20 page

    Measurement of the azimuthal anisotropy of Y(1S) and Y(2S) mesons in PbPb collisions at √S^{S}NN = 5.02 TeV

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    The second-order Fourier coefficients (υ2_{2}) characterizing the azimuthal distributions of ΄(1S) and ΄(2S) mesons produced in PbPb collisions at sNN\sqrt{s_{NN}} = 5.02 TeV are studied. The ΄mesons are reconstructed in their dimuon decay channel, as measured by the CMS detector. The collected data set corresponds to an integrated luminosity of 1.7 nb−1^{-1}. The scalar product method is used to extract the υ2_{2} coefficients of the azimuthal distributions. Results are reported for the rapidity range |y| < 2.4, in the transverse momentum interval 0 < pT_{T} < 50 GeV/c, and in three centrality ranges of 10–30%, 30–50% and 50–90%. In contrast to the J/ψ mesons, the measured υ2_{2} values for the ΄ mesons are found to be consistent with zero
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