Oscillatory-like expansion of a Fermionic superfluid

We study the expansion behaviors of a Fermionic superfluid in a cigar-shaped optical dipole trap for the whole BEC-BCS crossover and various temperatures.At low...     

双黄连口服液和双黄连片中黄芩甙的含量测定

采用了反相高效液相色谱法测定双黄口服液和双黄连片中黄芩甙的含量.具体方法是采用C18色谱柱,以甲醇:水:冰醋酸=49.5:50:0.5为流动相,流速1.0ml/min,紫外光度检测器于波长277nm测定,实验结果表明黄芩甙浓度在0.05~0.20mg/ml时呈良好的线性关系,r=0.9988,在双黄连片中回收率为86.70%,RSD为2.27,在双黄连口服液中回收率为97.31%,RSD为2.10.采用本法测定双黄口服液和双黄连片中黄芩甙的含量,方法灵敏,快速,简便,准确,结果稳定,重现性好,能起到控制双黄连片和双黄连口服液质量的作用.     

关于费米子玻色化技术的注记

传统根据Jordon和Wigner理论,构造了费米子玻色化方案。文章讨论证明了这种方案只有在k≠k′时才成立,而在k=k′时则不成立,从而说明了费米子的玻色化技术是不完备的     

关于谱对和和谐对的刻画

研究了在谱自仿测度中的重要概念谱对和和谐对的刻画．最近,Dorin．Ervin．Dutkay and P．E．T．Jorgensen在Quasiperiodic spectra and orthogonality for iterated function system measures一文中建立了一个一维中谱对和和谐对的刻画,并且得到这种谱集的谱只有有限多个．本文将这一结论推广到了n维,也得到这种谱集的谱只有有限多个．     

kerr介质中级联三能级原子与光场非共振相互作用过程中原子的动力学特性

本文导出了充满ｋｅｒ介质的高Ｑ腔中级联型三能级原子与双模ＳＵ（１,１）相干态场非共振相互作用系统的态矢量,并以此计算三能级原子布居概率随时间的演化,数值计算显示,ｋｅｒ效应产生与两能级原子不同的Ｒａｂｉ振荡特征,而ｋｅｒ效应与失谐的共同作用导致出现电子绝热跃迁转移现象。     

Observation of the ideal Josephson effect in superfluid 4He

Superfluids and superconductors are the only states of condensed matter that can be described by a single wavefunction, with a coherent quantum phase Phi. The mass flow in a superfluid can be described by classical hydrodynamics for small flow velocity, but above a critical velocity, quantized vortices are created and the classical picture breaks down. This can be observed for a superfluid flowing through a microscopic aperture when the mass flow is measured as a function of the phase difference across the aperture; the curve resembles a hysteretic sawtooth where each jump corresponds to the creation of a vortex. When the aperture is made small enough, the system can enter the so-called 'ideal' Josephson regime, where the superfluid mass flow becomes a continuous function of the phase difference. This regime has been detected in superfluid 3He, but was hitherto believed to be unobservable, owing to fluctuations, in 4He. Here we report the observation of the ideal Josephson effect in 4He. We study the flow of 4He through an array of micro-apertures and observe a transition to the ideal Josephson regime as the temperature is increased towards the superfluid transition temperature, Tlambda.     

单自由度齿轮系统非线性动力学特性分析

建立了综合考虑齿侧间隙、时变啮合刚度、综合啮合误差等因素的直齿轮副的单自由度非线性动力学模型,利用变步长Runge-Kutta法对单自由度运动微分方程进行数值求解.结合系统的分岔图、相图、Poincaré映射图以及FFT频谱图,分析了系统在不同侧隙值下,阻尼比变化时的动力学特性,得到了系统的混沌运动形成过程.     

氢键分子系统中扭结孤子偶的辐射及其核化特性

运用一个新的氢键系统的二分量弧子模型,讨论了氢键系统在外场作用下弧子偶的运动,研究了弧子偶对电磁波的散射和核化特性,得到了弧子偶对电磁波的散射截面和平均核化率的表达式。     

用重整化群流方程研究重费密子系统的重整杂化带模型

重整化群流方程方法是一种非常有用的理论研究工具,它可以用于各种物理系统中,求取系统的能谱和期望值,由此获得系统的一些属性.用该方法研究重费密子系统推广后的重整杂化带模型,求得相应的两支准粒子能带,这些结果与用常规的格林函数方法求得的结果完全一致.     

Quantum phase transition from a superfluid to a Mott insulator in a gas of ultracold atoms.

For a system at a temperature of absolute zero, all thermal fluctuations are frozen out, while quantum fluctuations prevail. These microscopic quantum fluctuations can induce a macroscopic phase transition in the ground state of a many-body system when the relative strength of two competing energy terms is varied across a critical value. Here we observe such a quantum phase transition in a Bose-Einstein condensate with repulsive interactions, held in a three-dimensional optical lattice potential. As the potential depth of the lattice is increased, a transition is observed from a superfluid to a Mott insulator phase. In the superfluid phase, each atom is spread out over the entire lattice, with long-range phase coherence. But in the insulating phase, exact numbers of atoms are localized at individual lattice sites, with no phase coherence across the lattice; this phase is characterized by a gap in the excitation spectrum. We can induce reversible changes between the two ground states of the system.     

量子系综对的量子关联性

研究一对量子系综{ε,η}的量子关联性。在量子信息论中,通过量子测量只能知道量子系统的状态ρ以一定的概率pi处于某个状态ρi,从而得到一系列的量子态ρ1,ρ2,…,ρn以及它们出现的相应概率p1,p2,…,pn;进而得到一个量子系综ε={pi,ρi}ni=1。构造一个四体量子态ρε,η,利用量子相对熵,定义了反映量子系综对所含量子关联的度量函数,揭示了这个度量函数的一些性质。     

Universal spin transport in a strongly interacting Fermi gas

Transport of fermions, particles with half-integer spin, is central to many fields of physics. Electron transport runs modern technology, defining states of matter such as superconductors and insulators, and electron spin is being explored as a new carrier of information. Neutrino transport energizes supernova explosions following the collapse of a dying star, and hydrodynamic transport of the quark-gluon plasma governed the expansion of the early Universe. However, our understanding of non-equilibrium dynamics in such strongly interacting fermionic matter is still limited. Ultracold gases of fermionic atoms realize a pristine model for such systems and can be studied in real time with the precision of atomic physics. Even above the superfluid transition, such gases flow as an almost perfect fluid with very low viscosity when interactions are tuned to a scattering resonance. In this hydrodynamic regime, collective density excitations are weakly damped. Here we experimentally investigate spin excitations in a Fermi gas of (6)Li atoms, finding that, in contrast, they are maximally damped. A spin current is induced by spatially separating two spin components and observing their evolution in an external trapping potential. We demonstrate that interactions can be strong enough to reverse spin currents, with components of opposite spin reflecting off each other. Near equilibrium, we obtain the spin drag coefficient, the spin diffusivity and the spin susceptibility as a function of temperature on resonance and show that they obey universal laws at high temperatures. In the degenerate regime, the spin diffusivity approaches a value set by [planck]/m, the quantum limit of diffusion, where [planck]/m is Planck's constant divided by 2π and m the atomic mass. For repulsive interactions, our measurements seem to exclude a metastable ferromagnetic state.     

Vortices and superfluidity in a strongly interacting Fermi gas

Quantum degenerate Fermi gases provide a remarkable opportunity to study strongly interacting fermions. In contrast to other Fermi systems, such as superconductors, neutron stars or the quark-gluon plasma of the early Universe, these gases have low densities and their interactions can be precisely controlled over an enormous range. Previous experiments with Fermi gases have revealed condensation of fermion pairs. Although these and other studies were consistent with predictions assuming superfluidity, proof of superfluid behaviour has been elusive. Here we report observations of vortex lattices in a strongly interacting, rotating Fermi gas that provide definitive evidence for superfluidity. The interaction and therefore the pairing strength between two 6Li fermions near a Feshbach resonance can be controlled by an external magnetic field. This allows us to explore the crossover from a Bose-Einstein condensate of molecules to a Bardeen-Cooper-Schrieffer superfluid of loosely bound pairs. The crossover is associated with a new form of superfluidity that may provide insights into high-transition-temperature superconductors.     

一类超流体膜方程解的存在性

主要研究一类超流体膜方程的非平凡解的存在性。首先,我们主要利用变分法把偏微分方程解的问题化为相应的能量泛函的临界点问题,再利用山路引理证明方程能量泛函的临界点的存在性。     

两相邻Said-Ball曲线的近似合并

利用Said-Ball基函数和Bernste in基函数之间的关系,结合两相邻Béz ier曲线的近似合并方法,给出两相邻Said-Ball曲线的近似合并方法。该法有以下特点:(1)可直接得到合并曲线的控制顶点,(2)不论待合并的两相邻曲线的次数是否相同,均可直接合并,(3)不需对原曲线进行升阶变换,直接提高合并曲线的次数,就可以得到更高阶的合并曲线。在合并过程中,考虑了合并曲线在左右端点处与原曲线达到高阶插值的合并。最后给出数值例子。     

Binary Sequences from a Pair of Elliptic Curves

A family of binary sequences were constructed by using an elliptic curve and its twisted curves over finite fields. It was shown that these sequences possess ＂good＂ cryptographie properties of 0-1 distribution, long period and large linear complexity. The results indicate that such se quences provide strong potential applications in cryptography.     

Hidden magnetism and quantum criticality in the heavy fermion superconductor CeRhIn5

With only a few exceptions that are well understood, conventional superconductivity does not coexist with long-range magnetic order (for example, ref. 1). Unconventional superconductivity, on the other hand, develops near a phase boundary separating magnetically ordered and magnetically disordered phases. A maximum in the superconducting transition temperature T(c) develops where this boundary extrapolates to zero Kelvin, suggesting that fluctuations associated with this magnetic quantum-critical point are essential for unconventional superconductivity. Invariably, though, unconventional superconductivity masks the magnetic phase boundary when T < T(c), preventing proof of a magnetic quantum-critical point. Here we report specific-heat measurements of the pressure-tuned unconventional superconductor CeRhIn5 in which we find a line of quantum-phase transitions induced inside the superconducting state by an applied magnetic field. This quantum-critical line separates a phase of coexisting antiferromagnetism and superconductivity from a purely unconventional superconducting phase, and terminates at a quantum tetracritical point where the magnetic field completely suppresses superconductivity. The T --> 0 K magnetic field-pressure phase diagram of CeRhIn5 is well described with a theoretical model developed to explain field-induced magnetism in the high-T(c) copper oxides, but in which a clear delineation of quantum-phase boundaries has not been possible. These experiments establish a common relationship among hidden magnetism, quantum criticality and unconventional superconductivity in copper oxides and heavy-electron systems such as CeRhIn5.     

相对论磁化等离子体二体关联动力方程的格林函数

应用二体关联动力方程的格林函数方法，算出了相对论磁化等离子体中点源粒子产生的诱发电场和扰动分布函数。