54,496,324 research outputs found

    High-contrast dark resonance on the D2 - line of 87Rb in a vapor cell with different directions of the pump - probe waves

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    We propose a novel method enabling to create a high-contrast dark resonance in the 87Rb vapor D2-line. The method is based on an optical pumping of atoms into the working states by a two-frequency, linearly-polarized laser radiation propagating perpendicularly to the probe field. This new scheme is compared to the traditional scheme involving the circularly-polarized probe beam only, and significant improvement of the dark resonance parameters is found. Qualitative considerations are confirmed by numerical calculations.Comment: 7 pages, 4 figure

    Transport of a quantum degenerate heteronuclear Bose-Fermi mixture in a harmonic trap

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    We report on the transport of mixed quantum degenerate gases of bosonic 87Rb and fermionic 40K in a harmonic potential provided by a modified QUIC trap. The samples are transported over a distance of 6 mm to the geometric center of the anti-Helmholtz coils of the QUIC trap. This transport mechanism was implemented by a small modification of the QUIC trap and is free of losses and heating. It allows all experiments using QUIC traps to use the highly homogeneous magnetic fields that can be created in the center of a QUIC trap and improves the optical access to the atoms, e.g., for experiments with optical lattices. This mechanism may be cascaded to cover even larger distances for applications with quantum degenerate samples.Comment: 7 pages, 8 figure

    Summing Radiative Corrections to the Effective Potential

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    When one uses the Coleman-Weinberg renormalization condition, the effective potential VV in the massless ϕ44\phi_4^4 theory with O(N) symmetry is completely determined by the renormalization group functions. It has been shown how the (p+1)(p+1) order renormalization group function determine the sum of all the N^{\mbox{\scriptsize p}}LL order contribution to VV to all orders in the loop expansion. We discuss here how, in addition to fixing the N^{\mbox{\scriptsize p}}LL contribution to VV, the (p+1)(p+1) order renormalization group functions also can be used to determine portions of the N^{\mbox{\scriptsize p+n}}LL contributions to VV. When these contributions are summed to all orders, the singularity structure of \mcv is altered. An alternate rearrangement of the contributions to VV in powers of lnϕ\ln \phi, when the extremum condition V(ϕ=v)=0V^\prime (\phi = v) = 0 is combined with the renormalization group equation, show that either v=0v = 0 or VV is independent of ϕ\phi. This conclusion is supported by showing the LL, \cdots, N4^4LL contributions to VV become progressively less dependent on ϕ\phi.Comment: 16 pages; added 2 figures and 2 tables; references revise

    A Method to Identify and Analyze Biological Programs through Automated Reasoning.

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    Predictive biology is elusive because rigorous, data-constrained, mechanistic models of complex biological systems are difficult to derive and validate. Current approaches tend to construct and examine static interaction network models, which are descriptively rich but often lack explanatory and predictive power, or dynamic models that can be simulated to reproduce known behavior. However, in such approaches implicit assumptions are introduced as typically only one mechanism is considered, and exhaustively investigating all scenarios is impractical using simulation. To address these limitations, we present a methodology based on automated formal reasoning, which permits the synthesis and analysis of the complete set of logical models consistent with experimental observations. We test hypotheses against all candidate models, and remove the need for simulation by characterizing and simultaneously analyzing all mechanistic explanations of observed behavior. Our methodology transforms knowledge of complex biological processes from sets of possible interactions and experimental observations to precise, predictive biological programs governing cell function

    Traveling waves in one-dimensional nonlinear models of strain-limiting viscoelasticity

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    In this article we investigate traveling wave solutions of a nonlinear differential equation describing the behaviour of one-dimensional viscoelastic medium with implicit constitutive relations. We focus on a subclass of such models known as the strain-limiting models introduced by Rajagopal. To describe the response of viscoelastic solids we assume a nonlinear relationship among the linearized strain, the strain rate and the Cauchy stress. We then concentrate on traveling wave solutions that correspond to the heteroclinic connections between the two constant states. We establish conditions for the existence of such solutions, and find those solutions, explicitly, implicitly or numerically, for various forms of the nonlinear constitutive relation

    Axial Charges of Octet Baryons in Two-flavor Lattice QCD

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    We evaluate the strangeness-conserving NNN N, ΣΣ\Sigma\Sigma, ΞΞ\Xi\Xi, ΛΣ\Lambda\Sigma and the strangeness-changing ΛN\Lambda N, ΣN\Sigma N, ΛΞ\Lambda\Xi, ΣΞ\Sigma\Xi axial charges in lattice QCD with two flavors of dynamical quarks and extend our previous work on pseudoscalar-meson-octet-baryon coupling constants so as to include πΞΞ\pi\Xi\Xi, KΛΞK\Lambda\Xi and KΣΞK\Sigma\Xi coupling constants. We find that the axial charges have rather weak quark-mass dependence and the breaking in SU(3)-flavor symmetry is small at each quark-mass point we consider.Comment: 6 pages, 6 figures. Added discussions and a figure; version to appear in Physics Letters

    Axial Charges of Octet Baryons in Two-flavor Lattice QCD

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    We evaluate the strangeness-conserving NNN N, ΣΣ\Sigma\Sigma, ΞΞ\Xi\Xi, ΛΣ\Lambda\Sigma and the strangeness-changing ΛN\Lambda N, ΣN\Sigma N, ΛΞ\Lambda\Xi, ΣΞ\Sigma\Xi axial charges in lattice QCD with two flavors of dynamical quarks and extend our previous work on pseudoscalar-meson-octet-baryon coupling constants so as to include πΞΞ\pi\Xi\Xi, KΛΞK\Lambda\Xi and KΣΞK\Sigma\Xi coupling constants. We find that the axial charges have rather weak quark-mass dependence and the breaking in SU(3)-flavor symmetry is small at each quark-mass point we consider.Comment: 6 pages, 6 figures. Added discussions and a figure; version to appear in Physics Letters
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