氢化物发生—原子荧光法测定不同产地绞股蓝及其根际土壤中As,Hg,Se

通过优化了的氢化物发生—原子荧光法测定了7个省产绞股蓝及其根际土壤中As,Hg,Se三种元素的含量,研究结果表明:7个省产绞股蓝中As,Hg,Se的含量存在较大差异,但As和Hg两种重金属元素含量均低于《药用植物及制剂进出口绿色行业标准》中As和Hg的限量标准。Se元素含量同根际土壤中Se元素含量显示极显著相关性,故湖北恩施富硒区产绞股蓝中Se含量明显高于其他6省产绞股蓝。研究结果可以初步判定,绞股蓝中Se元素主要来源于土壤,而As和Hg元素的积累则不同于Se元素,还可能受到大气气溶胶的干、湿沉降等因素的影响。     

Geometric phases in qubit-oscillator system beyond conventional rotating-wave approximation

In this work we investigated the geometric phases of a qubit-oscillator system beyond the conventional rotating- wave approximation. We find that in the limiting of weak coupling the results coincide with that obtained under rotating-wave approximation while there exists an increasing difference with the increase of coupling constant. It was shown that the geometric phase is symmetric with respect to the sign of the detuning of the quantized field from the one-photon resonance under the conventional rotating-wave approximation while a red-blue detuning asymmetry occurs beyond the conventional rotating-wave approximation.     

基于滑移网格与RNG湍流模型计算泵内的动静干扰

本文利用三维Navier-Stockes方程和RNG湍流模型,在转动与静止部件间采用滑移网格技术建立交互界面,对泵内动静干扰引起的三维非定常湍流进行了计算,得到了旋转叶轮与固定导叶间流体的湍流特征。从计算结果可知,静叶与动叶间各点的压力脉动频率成分一致,且幅值沿周向呈正弦变化规律。这说明利用滑移网格技术及RNG湍流模型,可以模拟三维非定常动静干扰流动问题。     

短波碲镉汞光伏器件的低频噪声研究

对所研制的短波光伏碲镉汞器件进行了变温电流-电压特性和低频噪声研究，测试温度范围255—293K.实验结果表明随着温度的下降，器件的优值因子R₀A从45×10³Ωcm²增加到7×10⁴Ωcm².器件在低频区的主要噪 声成分是1/f噪声和产生-复合噪声，在高频区主要是散粒噪声.在测试的偏压内，器件的1/f噪声功率谱密度与流过器件的电流的平方成正比，器件的Hooge系数为3×10^-4—7×10^-4.从噪声 功率谱密度曲线分析中得到产生-复合噪声的特征时间常数τ，通过τ的温度特性得到了器件的深能级. 关键词： 碲镉汞 优值因子 低频噪声 深能级     

Delocalized fermions in underdoped cuprate superconductors

Low-temperature heat transport was used to investigate the ground state of high-purity single crystals of the lightly doped cuprate YBa2Cu3O6.33. Samples were measured with doping concentrations on either side of the superconducting phase boundary. We report the observation of delocalized fermionic excitations at zero energy in the nonsuperconducting state, which shows that the ground state of underdoped cuprates is a thermal metal. Its low-energy spectrum appears to be similar to that of the d-wave superconductor, i.e., nodal. The insulating ground state observed in underdoped La2-xSrxCuO4 is attributed to the competing spin-density-wave order.     

Critical point and the nature of the pseudogap of single-layered copper-oxide Bi2Sr2-xLaxCuO6+delta superconductors

We apply strong magnetic fields of H=28.5 to 43 T to suppress superconductivity (SC) in the cuprates Bi2Sr2-xLaxCuO6+delta (x=0.65, 0.40, 0.25, 0.15, and 0), and investigate the low temperature (T) normal state by 63Cu nuclear spin-lattice relaxation rate (1/T1) measurements. We find that the pseudogap (PG) phase persists deep inside the overdoped region but terminates at x approximately 0.05, which corresponds to the hole doping concentration of approximately 0.21. Beyond this critical point, the normal state is a Fermi liquid that persists as the ground state when superconductivity is removed by the magnetic field. A comparison of the superconducting state with the H-induced normal state in the x=0.40 (Tc=32 K) sample indicates that there remains substantial part of the Fermi surface even in the fully developed PG state, which suggests that the PG and SC are coexisting matters.     

Globally polarized quark-gluon plasma in noncentral A + A collisions

Produced partons have a large local relative orbital angular momentum along the direction opposite to the reaction plane in the early stage of noncentral heavy-ion collisions. Parton scattering is shown to polarize quarks along the same direction due to spin-orbital coupling. Such global quark polarization will lead to many observable consequences, such as left-right asymmetry of hadron spectra and global transverse polarization of thermal photons, dileptons, and hadrons. Hadrons from the decay of polarized resonances will have an azimuthal asymmetry similar to the elliptic flow. Global hyperon polarization is studied within different hadronization scenarios and can be easily tested.     

Subpeaks in the Brillouin loss spectra of distributed fiber-optic sensors

Subpeaks in the Brillouin loss spectra of distributed fiber-optic sensors were observed for what is believed to be the first time and studied. We discovered that the Fourier spectrum of the pulsed signal and the off-resonance oscillation both contributed to subpeaks. The off-resonance oscillation at frequency /v - vB/ is the oscillation in the Brillouin time domain when beat frequency v of the two counterpropagating laser beams does not match local Brillouin frequency vB. This study is important in differentiating the subpeaks from actual strain-temperature peaks.     

Simple method to identify the spatial location better than the pulse length with high strain accuracy

The second-order partial derivative of the Stokes signal with respect to frequency and position shows a maximum or minimum at the boundary between two different strained sections. This idea is used to locate the boundary of different stress regions. Knowing the boundaries, we then fit the Brillouin spectrum at the middle between them to get the strain value. This allows a location accuracy of between 5 and 10 cm, which is shorter than the pulse length of 20 cm used in the experiment. The lowest detectable Brillouin frequency difference between two strain sections is 1.2 MHz.     

不同氮源制备CNx纳米管薄膜及其低场致电子发射性能

采用高温热解法,分别以氯化铵(NH4Cl)和乙二胺(C2H8N2)为氮源在洁净的硅片上沉积生长CNx纳米管薄膜.利用扫描电子显微镜、高分辨率透射电子显微镜和拉曼光谱对CNx纳米管进行形貌观察和表征.结果显示不同氮源制备出的CNx纳米管薄膜的洁净度、有序度以及纳米管的结构明显不同.热解乙二胺(C2H8N2)/二茂铁(C10H10Fe)制备出的结晶度较低的"竹节状"结构CNx纳米管平行基底表面有序生长,而且低场致电子发射性能优越,开启电场1.0V/μm,外加电场达到2.89V/μm时发射电流密度为860μA/cm2.