11 research outputs found

    Poisson noise induced switching in driven micromechanical resonators

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    We study Poisson-noise induced switching between coexisting vibrational states in driven nonlinear micromechanical resonators. In contrast to Gaussian noise induced switching, the measured logarithm of the switching rate is proportional not to the reciprocal noise intensity, but to its logarithm, for fixed pulse area. We also find that the switching rate logarithm varies as a square root of the distance to the bifurcation point, instead of the conventional scaling with exponent 3/2.Comment: accepted by PR

    Bulk Fermi surface and electronic properties of Cu0.07_{0.07}Bi2_{2}Se3_{3}

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    The electronic properties of Cu0.07_{0.07}Bi2_{2}Se3_{3} have been investigated using Shubnikov-de Haas and optical reflectance measurements. Quantum oscillations reveal a bulk, three-dimensional Fermi surface with anisotropy kFc/kFab≈k^{c}_{F}/k^{ab}_{F}\approx 2 and a modest increase in free-carrier concentration and in scattering rate with respect to the undoped Bi2_{2}Se3_{3}, also confirmed by reflectivity data. The effective mass is almost identical to that of Bi2_{2}Se3_{3}. Optical conductivity reveals a strong enhancement of the bound impurity bands with Cu addition, suggesting that a significant number of Cu atoms enter the interstitial sites between Bi and Se layers or may even substitute for Bi. This conclusion is also supported by X-ray diffraction measurements, where a significant increase of microstrain was found in Cu0.07_{0.07}Bi2_{2}Se3_{3}, compared to Bi2_{2}Se3_{3}.Comment: Accepted to Phys. Rev B (R

    Unusual Shubnikov-de Haas oscillations in BiTeCl

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    We report measurements of Shubnikov-de Haas (SdH) oscillations in single crystals of BiTeCl at magnetic fields up to 31 T and at temperatures as low as 0.4 K. Two oscillation frequencies were resolved at the lowest temperatures, F1=65±4F_{1}=65 \pm 4 Tesla and F2=156±5F_{2}=156 \pm 5 Tesla. We also measured the infrared optical reflectance (R(ω))\left(\cal R(\omega)\right) and Hall effect; we propose that the two frequencies correspond respectively to the inner and outer Fermi sheets of the Rashba spin-split bulk conduction band. The bulk carrier concentration was ne≈1×1019n_{e}\approx1\times10^{19} cm−3^{-3} and the effective masses m1∗=0.20m0m_{1}^{*}=0.20 m_{0} for the inner and m2∗=0.27m0m_{2}^{*}=0.27 m_{0} for the outer sheet. Surprisingly, despite its low effective mass, we found that the amplitude of F2F_{2} is very rapidly suppressed with increasing temperature, being almost undetectable above T≈4T\approx4 K

    Experimental determination of the bulk Rashba parameters in BiTeBr

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    Shubnikov-de Haas (SdH) oscillations, Hall effect, and optical reflectance (R(omega)) measurements have been performed on single crystals of BiTeBr. Under magnetic fields up to 32 tesla and at temperatures as low as 0.4K, the SdH data shows a single oscillation frequency F = 102 +/- 5 tesla. The combined transport and optical studies establish that the SdH effect originates from the Rashba spin-split bulk conduction band, with the chemical potential situated about 13 meV below the crossing (Dirac) point. The bulk carrier concentration was n(e) approximate to 5 x 10(18) cm(-3) and the effective mass m(1)* = 0.16m(0). Combining SdH and optical data, we reliably determine the Rashba parameters for the bulk conduction band of BiTeBr: the Rashba energy E-R = 28meV and the momentum spin-split k(R) = 0.033 angstrom(-1). Hence, the bulk Rashba coupling strength alpha(R) = 2E(R)/k(R) is found to be 1.7 eV angstrom. Copyright (C) EPLA, 201
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