9,179 research outputs found

    Euler solution of multiblade rotor flow

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    A numerical method for solving the Euler equations for multiblade rotors has been developed and some preliminary results reported. The numerical scheme is a combination of several recent methods and algorithm improvements, adapted to the particular requirements of rotor-body interactions. A cylindrical basic grid has been used to study conventional multiblade helicopter rotors. Test calculations have been made for two- and six-blade rotors in hover and for a two-blade rotor in forward flight, under transonic tip conditions but without lift. The results show good agreement with experimental data

    Quantum phase diagram of an exactly solved mixed spin ladder

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    We investigate the quantum phase diagram of the exactly solved mixed spin-(1/2,1) ladder via the thermodynamic Bethe ansatz (TBA). In the absence of a magnetic field the model exhibits three quantum phases associated with su(2), su(4) and su(6) symmetries. In the presence of a strong magnetic field, there is a third and full saturation magnetization plateaux within the strong antiferromagnetic rung coupling regime. Gapless and gapped phases appear in turn as the magnetic field increases. For weak rung coupling, the fractional magnetization plateau vanishs and exhibits new quantum phase transitions. However, in the ferromagnetic coupling regime, the system does not have a third saturation magnetization plat eau. The critical behaviour in the vicinity of the critical points is also derived systematically using the TBA.Comment: 20 pages, 2 figure

    Fully gapped superconducting state in Au2Pb: a natural candidate for topological superconductor

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    We measured the ultra-low-temperature specific heat and thermal conductivity of Au2_2Pb single crystal, a possible three-dimensional Dirac semimetal with a superconducting transition temperature Tc≈T_c \approx 1.05 K. The electronic specific heat can be fitted by a two-band s-wave model, which gives the gap amplitudes Δ1\Delta_1(0)/kBTck_BT_c = 1.38 and Δ2\Delta_2(0)/kBTck_BT_c = 5.25. From the thermal conductivity measurements, a negligible residual linear term κ0/T\kappa_0/T in zero field and a slow field dependence of κ0/T\kappa_0/T at low field are obtained. These results suggest that Au2_2Pb has a fully gapped superconducting state in the bulk, which is a necessary condition for topological superconductor if Au2_2Pb is indeed one.Comment: 6 pages, 4 figure

    Hysteresis in the quantum Hall regimes in electron double quantum well structures

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    We present in this paper experimental results on the transport hysteresis in electron double quantum well structures. Exploring the measurement technique of fixing the magnetic field and sweeping a front gate voltage (Vg), we are able to study the hysteresis by varying the top layer Landau level fillings while maintaining a relatively constant filling factor in the bottom layer, allowing us to tackle the question of the sign of Rxx(up)-Rxx(down), where Rxx(up) is the magnetoresistance when Vg is swept up and Rxx(down) when Vg swept down. Furthermore, we observe that hysteresis is generally stronger in the even integer quantum Hall effect (IQHE) regime than in the odd-IQHE regime. This, we argue, is due to a larger energy gap for an even-IQHE state, determined by the Landau level separation, than that for an odd-IQHE state, determined by the Zeeman splitting

    Phase diagram as a function of doping level and pressure in Eu1−x_{1-x}Lax_xFe2_2As2_2 system

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    We establish the phase diagram of Eu1−x_{1-x}Lax_xFe2_2As2_2 system as a function of doping level x and the pressure by measuring the resistivity and magnetic susceptibility. The pressure can suppress the spin density wave (SDW) and structural transition very efficiently, while enhance the antiferromagnetic (AFM) transition temperature TN_N of Eu2+^{2+}. The superconductivity coexists with SDW order at the low pressure, while always coexists with the Eu2+^{2+} AFM order. The results suggests that Eu2+^{2+} spin dynamics is disentangeld with superconducting (SC) pairing taken place in the two-dimensional \emph{Fe-As} plane, but it can strongly affect superconducting coherence along c-axis
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