6,535 research outputs found

    Superconductivity-induced Phonon Renormalization on NaFe1−x_{1-x}Cox_{x}As

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    We report a study of the lattice dynamics in superconducting NaFeAs (Tc = 8 K) and doped NaFe0.97Co0.03As (Tc = 20 K) using Raman light scattering. Five of the six phonon modes expected from group theory are observed. In contrast with results obtained on iso-structural and iso-electronic LiFeAs, anomalous broadening of Eg(As) and A1g(Na) modes upon cooling is observed in both samples. In addition, in the Co-doped sample, a superconductivity-induced renormalization of the frequency and linewidth of the B1g(Fe) vibration is observed. This renormalization can not be understood within a single band and simple multi-band approaches. A theoretical model that includes the effects of SDW correlations along with sign-changing s-wave pairing state and interband scattering has been developed to explain the observed behavior of the B1g(Fe) mode.Comment: 10 pages; 6 figure

    Collapse arrest and soliton stabilization in nonlocal nonlinear media

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    We investigate the properties of localized waves in systems governed by nonlocal nonlinear Schrodinger type equations. We prove rigorously by bounding the Hamiltonian that nonlocality of the nonlinearity prevents collapse in, e.g., Bose-Einstein condensates and optical Kerr media in all physical dimensions. The nonlocal nonlinear response must be symmetric, but can be of completely arbitrary shape. We use variational techniques to find the soliton solutions and illustrate the stabilizing effect of nonlocality.Comment: 4 pages with 3 figure

    Chalcogenide-glass polarization-maintaining photonic crystal fiber for mid-infrared supercontinuum generation

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    In this paper, we report the design and fabrication of a highly birefringent polarization-maintaining photonic crystal fiber (PM-PCF) made from chalcogenide glass, and its application to linearly-polarized supercontinuum (SC) generation in the mid-infrared region. The PM fiber was drawn using the casting method from As38Se62 glass which features a transmission window from 2 to 10 ÎŒm\mu m and a high nonlinear index of 1.13.10−17^{-17}m2^{2}W−1^{-1}. It has a zero-dispersion wavelength around 4.5 ÎŒm\mu m and, at this wavelength, a large birefringence of 6.10−4^{-4} and consequently strong polarization maintaining properties are expected. Using this fiber, we experimentally demonstrate supercontinuum generation spanning from 3.1-6.02 ÎŒm\mu m and 3.33-5.78 ÎŒm\mu m using femtosecond pumping at 4 ÎŒm\mu m and 4.53 ÎŒm\mu m, respectively. We further investigate the supercontinuum bandwidth versus the input pump polarization angle and we show very good agreement with numerical simulations of the two-polarization model based on two coupled generalized nonlinear Schr\"odinger equations.Comment: 13 pages, 8 figure

    Interaction-induced localization of anomalously-diffracting nonlinear waves

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    We study experimentally the interactions between normal solitons and tilted beams in glass waveguide arrays. We find that as a tilted beam, traversing away from a normally propagating soliton, coincides with the self-defocusing regime of the array, it can be refocused and routed back into any of the intermediate sites due to the interaction, as a function of the initial phase difference. Numerically, distinct parameter regimes exhibiting this behavior of the interaction are identified.Comment: Physical Review Letters, in pres

    A simpler and more efficient algorithm for the next-to-shortest path problem

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    Given an undirected graph G=(V,E)G=(V,E) with positive edge lengths and two vertices ss and tt, the next-to-shortest path problem is to find an stst-path which length is minimum amongst all stst-paths strictly longer than the shortest path length. In this paper we show that the problem can be solved in linear time if the distances from ss and tt to all other vertices are given. Particularly our new algorithm runs in O(∣V∣log⁥∣V∣+∣E∣)O(|V|\log |V|+|E|) time for general graphs, which improves the previous result of O(∣V∣2)O(|V|^2) time for sparse graphs, and takes only linear time for unweighted graphs, planar graphs, and graphs with positive integer edge lengths.Comment: Partial result appeared in COCOA201

    Ultra-low-noise supercontinuum generation with a flat near-zero normal dispersion fiber

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    A pure silica photonic crystal fiber with a group velocity dispersion (ÎČ2\beta_2) of 4 ps2^2/km at 1.55 ÎŒ\mum and less than 7 ps2^2/km from 1.32 ÎŒ\mum to the zero dispersion wavelength (ZDW) 1.80 ÎŒ\mum was designed and fabricated. The dispersion of the fiber was measured experimentally and found to agree with the fiber design, which also provides low loss below 1.83 ÎŒ\mum due to eight outer rings with increased hole diameter. The fiber was pumped with a 1.55 ÎŒ\mum, 125 fs laser and, at the maximum in-coupled peak power (P0_0) of 9 kW, a 1.34−-1.82 ÎŒ\mum low-noise spectrum with a relative intensity noise below 2.2\% was measured. The numerical modeling agreed very well with the experiments and showed that P0_0 could be increased to 26 kW before noise from solitons above the ZDW started to influence the spectrum by pushing high-noise dispersive waves through the spectrum

    Quasiperiodic Envelope Solitons

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    We analyse nonlinear wave propagation and cascaded self-focusing due to second-harmonic generation in Fibbonacci optical superlattices and introduce a novel concept of nonlinear physics, the quasiperiodic soliton, which describes spatially localized self-trapping of a quasiperiodic wave. We point out a link between the quasiperiodic soliton and partially incoherent spatial solitary waves recently generated experimentally.Comment: Submitted to PRL. 4 pages with 5 figure

    Dynamic Fano Resonance of Quasienergy Excitons in Superlattices

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    The dynamic Fano resonance (DFR) between discrete quasienergy excitons and sidebands of their ionization continua is predicted and investigated in dc- and ac-driven semiconductor superlattices. This DFR, well controlled by the ac field, delocalizes the excitons and opens an intrinsic decay channel in nonlinear four-wave mixing signals.Comment: 4pages, 4figure
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