10,597 research outputs found

    Characteristic Length Scale of Electric Transport Properties of Genomes

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    A tight-binding model together with a novel statistical method are used to investigate the relation between the sequence-dependent electric transport properties and the sequences of protein-coding regions of complete genomes. A correlation parameter Ω\Omega is defined to analyze the relation. For some particular propagation length wmaxw_{max}, the transport behaviors of the coding and non-coding sequences are very different and the correlation reaches its maximal value Ωmax\Omega_{max}. wmaxw_{max} and \omax are characteristic values for each species. The possible reason of the difference between the features of transport properties in the coding and non-coding regions is the mechanism of DNA damage repair processes together with the natural selection.Comment: 4 pages, 4 figure

    The Unpredictability of the Most Energetic Solar Events

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    Observations over the past two solar cycles show a highly irregular pattern of occurrence for major solar flares, gamma-ray events, and solar energetic particle (SEP) fluences. Such phenomena do not appear to follow the direct indices of solar magnetic activity, such as the sunspot number. I show that this results from the non-Poisson occurrence for the most energetic events. This Letter also points out a particularly striking example of this irregularity in a comparison between the declining phases of the recent two solar cycles (1993-1995 and 2004-2006, respectively) and traces it through the radiated energies of the flares, the associated SEP fluences, and the sunspot areas. These factors suggest that processes in the solar interior involved with the supply of magnetic flux up to the surface of the Sun have strong correlations in space and time, leading to a complex occurrence pattern that is presently unpredictable on timescales longer than active region lifetimes (weeks) and not correlated well with the solar cycle itself.Comment: 4 page

    Observation of simultaneous fast and slow light

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    We present a microresonator-based system capable of simultaneously producing time-advanced and time-delayed pulses. The effect is based on the combination of a sharp spectral feature with two orthogonally-polarized propagating waveguide modes. We include an experimental proof-of-concept implementation using a silica microsphere coupled to a tapered optical fiber and use a time-domain picture to interpret the observed delays. We also discuss potential applications for future all-optical networks.Comment: 6 pages, 5 figure

    Kinetic Inductance of Josephson Junction Arrays: Dynamic and Equilibrium Calculations

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    We show analytically that the inverse kinetic inductance L1L^{-1} of an overdamped junction array at low frequencies is proportional to the admittance of an inhomogeneous equivalent impedance network. The ijthij^{th} bond in this equivalent network has an inverse inductance Jijcos(θi0θj0Aij)J_{ij}\cos(\theta_i^0-\theta_j^0-A_{ij}), where JijJ_{ij} is the Josephson coupling energy of the ijthij^{th} bond, θi0\theta_i^0 is the ground-state phase of the grain ii, and AijA_{ij} is the usual magnetic phase factor. We use this theorem to calculate L1L^{-1} for square arrays as large as 180×180180\times 180. The calculated L1L^{-1} is in very good agreement with the low-temperature limit of the helicity modulus γ\gamma calculated by conventional equilibrium Monte Carlo techniques. However, the finite temperature structure of γ\gamma, as a function of magnetic field, is \underline{sharper} than the zero-temperature L1L^{-1}, which shows surprisingly weak structure. In triangular arrays, the equilibrium calculation of γ\gamma yields a series of peaks at frustrations f=12(11/N)f = \frac{1}{2}(1-1/N), where NN is an integer 2\geq 2, consistent with experiment.Comment: 14 pages + 6 postscript figures, 3.0 REVTe

    Global Energetics of Thirty-Eight Large Solar Eruptive Events

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    We have evaluated the energetics of 38 solar eruptive events observed by a variety of spacecraft instruments between February 2002 and December 2006, as accurately as the observations allow. The measured energetic components include: (1) the radiated energy in the GOES 1 - 8 A band; (2) the total energy radiated from the soft X-ray (SXR) emitting plasma; (3) the peak energy in the SXR-emitting plasma; (4) the bolometric radiated energy over the full duration of the event; (5) the energy in flare-accelerated electrons above 20 keV and in flare-accelerated ions above 1 MeV; (6) the kinetic and potential energies of the coronal mass ejection (CME); (7) the energy in solar energetic particles (SEPs) observed in interplanetary space; and (8) the amount of free (nonpotential) magnetic energy estimated to be available in the pertinent active region. Major conclusions include: (1) the energy radiated by the SXR-emitting plasma exceeds, by about half an order of magnitude, the peak energy content of the thermal plasma that produces this radiation; (2) the energy content in flare-accelerated electrons and ions is sufficient to supply the bolometric energy radiated across all wavelengths throughout the event; (3) the energy contents of flare-accelerated electrons and ions are comparable; (4) the energy in SEPs is typically a few percent of the CME kinetic energy (measured in the rest frame of the solar wind); and (5) the available magnetic energy is sufficient to power the CME, the flare-accelerated particles, and the hot thermal plasma

    d-Wave Pairing Correlation in the Two-Dimensional t-J Model

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    The pair-pair correlation function of the two-dimensional t-J model is studied by using the power-Lanczos method and an assumption of monotonic behavior. In comparison with the results of the ideal Fermi gas, we conclude that the 2D t-J model does not have long range d-wave superconducting correlation in the interesting parameter range of J/t0.5J/t \leq 0.5. Implications of this result will also be discussed.Comment: 4 pages, 6 figures, accepted by PR

    Two-photon interference with thermal light

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    The study of entangled states has greatly improved the basic understanding about two-photon interferometry. Two-photon interference is not the interference of two photons but the result of superposition among indistinguishable two-photon amplitudes. The concept of two-photon amplitude, however, has generally been restricted to the case of entangled photons. In this letter we report an experimental study that may extend this concept to the general case of independent photons. The experiment also shows interesting practical applications regarding the possibility of obtaining high resolution interference patterns with thermal sources.Comment: Added reference 1

    Measurement of the Dynamical Structure Factor of a 1D Interacting Fermi Gas

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    We present measurements of the dynamical structure factor S(q,ω)S(q,\omega) of an interacting one-dimensional (1D) Fermi gas for small excitation energies. We use the two lowest hyperfine levels of the 6^6Li atom to form a pseudo-spin-1/2 system whose s-wave interactions are tunable via a Feshbach resonance. The atoms are confined to 1D by a two-dimensional optical lattice. Bragg spectroscopy is used to measure a response of the gas to density ("charge") mode excitations at a momentum qq and frequency ω\omega. The spectrum is obtained by varying ω\omega, while the angle between two laser beams determines qq, which is fixed to be less than the Fermi momentum kFk_\textrm{F}. The measurements agree well with Tomonaga-Luttinger theory

    R-symmetry and Supersymmetry Breaking at Finite Temperature

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    We analyze the spontaneous U(1)RU(1)_R symmetry breaking at finite temperature for the simple O'Raifeartaigh-type model introduced in [1] in connection with spontaneous supersymmetry breaking. We calculate the finite temperature effective potential (free energy) to one loop order and study the thermal evolution of the model. We find that the R-symmetry breaking occurs through a second order phase transition. Its associated meta-stable supersymmetry breaking vacuum is thermodynamically favored at high temperatures and the model remains trapped in this state by a potential barrier, as the temperature lowers all the way until T=0.Comment: 19 pages, 4 figures - Minor revisions, references added. To appear in JHE
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