一维P S D激光定位反馈指示电路设计

针对某新型激光定位微角位移测试系统, 应用一维P S D接收激光并定位反馈指示, 设计了一维P S D对 中处理电路. 实验证明, 激光光斑小于1 0mm时, 对中精度达1mm     

集体运动态中的辛弱数混合

在由S和D核子关联对构成的原子核集体运动态中,存在由辛弱数混合造成的伪态成份. 给出了计算这种伪态成份的公式,并进行计算和讨论.     

激发态Cs(5D)原子间碰撞能量转移

用激光二步激发Cs原子至8S态,从谱线的波长及强度可以确定Cs原子的辐射及碰撞过程,5D态主要是由8S→7P→5D跃迁布居的.在1016-1017Cs密度范围内,测量了碰撞能量合并5D 5D→nL 6S(nL=9D,11S,7F)速率系数,因5D→6P(3.0-3.6μm)处于红外本实验不能探测,利用一个已经测量过的过程(即6P 5D→6S 7D)作相对测量,对于9D,11S和7F态,其平均速率系数分别为(8.4±4.2)×10-10,(7.3±3.6)×10-10和(9.7±4.8)×10-10cm3s-1.讨论了碰撞转移过程11S 6S 7F 6S对速率系数的影响.     

碰撞能量转移Cs(6P)+Cs(5D)→Cs(6S)+Cs(nL=9S,5F)的截面测量

二步激发Cs原子至8S态,测量了碰撞转移过程Cs(6P)+Cs(5D)→Cs(6S)+Cs(nL=9S,5F)的截面,测量由7D,9S和5F态发射的荧光强度,从荧光强度比和σ(7D)值得到了σ(9S)和σ(5F),而σ(7D)已经进行过绝对测量,截面值σ(9S)和σ(5F)分别为8.7×10-15和1.3×10-14?cm2.讨论了能量转移过程9S+6S5F+6S对σ(9S)和σ(5F)的影响.     

K(6S)+H2→K(4D)+H2的碰撞能量转移

激光双光子激发K原子至6s或4D态,测鼍了K(6S,4D)与H2的碰撞转移截面.池温在413K,H2气压在4～40 Pa范围内,K(6S,4D)-K的碰撞效应可略去.在激发6S态的情况下,记录6S→4P时间分辨荧光信号,从荧光强度的对数描绘出的直线斜率得到6S态的有效寿命,而4D态的布居随H2的增加而增加,因此引起4D→4P跃迁谱线的增强.在激发4D态的情况下,采用类似方法得到4D态的有效寿命,由Stern Volmet方程,测得6S和4D态的辐射寿命分别为(97±15)ns和(300±45)ns.激发态K原子总的碰撞去佰居截面为(1.6±0.3)×10-14cm2(对6S态)和(40±6)×10-16cm2(对4D态).该总截面中包含向K原子激发态的非反应碰撞转移截面以及与H2反应生成KH的反应截面.激发6S态,测量4D→4P的时间积分荧光强度随H2气压的变化,得到6S→4D的碰撞转移截面为(1.4±0.3)×10-14cm2.由此得到结论:K(6S)态主要是通过物理猝灭到K(4D)态,虽然在K(6S)+H2的碰撞中,观察到了由于化学反应生成的KH的存在.     

改进的三维分离变量表象方法计算振动光谱

用改进的三维分离变量表象(DVR3D)方法研究了基态电子态H2S和H2O的振动光谱。哈密顿形式在Jacobi坐标下给出,每个坐标都用一组DVR基函数表示.角度部分的DVR基组选择勒让德多项式形式,而径向坐标采用正弦函数形式.为了降低需要对角化的最终哈密顿矩阵的维数,采用连续对角化截断方法.用H2S和H2O振动能级的计算验证算法的正确性.     

Cs(8S)态的碰撞转移和高位原子态的激发

在Cs蒸气中,二步激发Cs原子至8S态,研究了其碰撞转移和高位原子态的产生过程.在1016～1017 cm-3密度范围内,测量了碰撞激发转移8S 6S→6D 6S的速率系数.由测得的荧光强度随密度的变化关系,得到k6D=(2.4±0.5)×10-10 cm3·s-1.同时研究了碰撞能量合并过程5D 5D→nL 6S(nL=9D,11S,7F),5D态是由8S→7P→5D的辐射跃迁产生的.由以前测量过的6P 5D 6S 7D的转移速率系数以及6P态的原子密度,结合荧光强度比得到碰撞能量合并过程的速率系数,对于9D,11S和7F各态,其平均值分别为(6.4±3.2)×10-10,(1.0±0.5)×10-10和(8.4±4.2)×10-10 cm3·s-1.     

原子核的配对壳模型数值计算(Ⅱ)

在配对壳模型内做SD子空间截断,选BCS对为S对,D对通过D=[S,Q]获得. 通过计算Z,Nε[50,82]区域的几个核,研究了单粒子能量和反常宇称态对于低能集体态的影响.     

核子配对壳模型计算中的多体效应

截断到S ,D子空间的核子配对壳模型用于原子核1 2 8- 1 34 Xe和1 30 - 1 36 Ba的计算。为考虑多体效应 ,S ,D对分别用变分法和Tamm Dancoff近似给定。用一个含有三个参数的哈密顿量系统地描述了Xe和Ba同位素的能谱 ,本征态和电磁跃迁的强度。所得结果和实验结果符合得较好 ,并且在一定程度上改善了用表面δ相互作用决定的S ,D对所得结果中的不足之处。     

Operat orized Bogoliubov Transformat ion and Seniority Mixing in Collective States of Nuclei

The operatorized Bogoliubov transformation (OBT) to deal with the seniority mixing problem in the cojlective states composed of S and D nucleon pairs is introduced. The spurious components of such states due to seniority mixing are disdussed and evaluated by using OBT.     

A conservative scheme for the relativistic Vlasov–Maxwell system

A new scheme for numerical integration of the 1D2V relativistic Vlasov–Maxwell system is proposed. Assuming that all particles in a cell of the phase space move with the same velocity as that of the particle located at the center of the cell at the beginning of each time step, we successfully integrate the system with no artificial loss of particles. Furthermore, splitting the equations into advection and interaction parts, the method conserves the sum of the kinetic energy of particles and the electromagnetic energy. Three test problems, the gyration of particles, the Weibel instability, and the wakefield acceleration, are solved by using our scheme. We confirm that our scheme can reproduce analytical results of the problems. Though we deal with the 1D2V relativistic Vlasov–Maxwell system, our method can be applied to the 2D3V and 3D3V cases.     

Probabilistic Teleportation of a Four-Particle Entangled State

A Scheme for teleporting an unknown four-particle entangled state is proposed via entangled swapping. In this scheme, four pairs of entangled particles are used as quantum channel. It is shown that, if the four pairs of particles are nonmaximally entangled, the teleportation can be successfully realized with certain probability if a receiver adopts some appropriate unitary transformations.     

Seniority in quantum many-body systems. I. Identical particles in a single shell

A discussion of the seniority quantum number in many-body systems is presented. The analysis is carried out for bosons and fermions simultaneously but is restricted to identical particles occupying a single shell. The emphasis of the paper is on the possibility of partial conservation of seniority which turns out to be a peculiar property of spin-9/2 fermions but prevalent in systems of interacting bosons of any spin. Partial conservation of seniority is at the basis of the existence of seniority isomers, frequently observed in semi-magic nuclei, and also gives rise to peculiar selection rules in one-nucleon transfer reactions.     

Coherent-state theory for the proton-neutron quasispin group

An extended coherent-state theory ^{1, 2}) is used to give a simple construction for the matrix elements of the proton-neutron sp(4) quasispin algebra. A very simple analytical expression is given for the matrix elements of the sp(4) generators valid for all cases where initial and final states are multiplicity-free with respect to the U(1) × SU(2) n, T subalgebra. In the more general case, involving multiplicity, the most natural orthonormal basis constructed by the coherent-state method leads to many-nucleon states in the seniority scheme which are approximately labelled by T_p, the isospin of the p nucleon pairs coupled to J = 0, T = 1.     

Shell structure and pairing for interacting fermions in a trap

The shell structures for weakly interacting fermions in harmonic oscillator traps at zero temperature undergo several transitions depending on the number of particles in the trap and their interaction strength. Calculations of the one and two-particle spectra give the pairing gaps, and the many particle state is constructed by the seniority scheme. For sufficiently few particles, N less than or similar to 10(4), the pairing field exceeds the mean-field splitting of single particle levels at the Fermi surface and the greater number of almost degenerate states due to the SU(3) symmetry in the harmonic oscillator shell lead to supergaps. Deformation and rotation are also discussed.     

Probabilistic Teleportation of a Three-Particle State

A scheme for teleporting a three-particle state is proposed when three pairs of entangled particles are used as quantum channels. Quantum teleportation can be successfully realized with a certain probability if the receiver adopts an appropriate unitary-reduction strategy. The probability of successful teleportation is determined by the smaller coetficients of the three entangled pairs.     

Probabilistic Teleportation of a Three-Particle State

A scheme for teleporting a three-particle state is proposed when three pairs of entangled particles are used as quantum channels. Quantum teleportation can be successfully realized with a certain probability if the receiver adopts an appropriate unitary-reduction strategy. The probability of successful teleportation is determined by the smaller coefficients of the three entangled pairs.