Evidence for a new resonance Σ^＊ （1380） with J^P=1/2^-＊

A new particle Σ^ ＊ with J ^P = 1/2^-was predicted by unquenched quark models with its mass around the well established Σ ＊ （1385） with J P = 3/2 ＋ .Here we re-examine some old data of the K^-p → Λπ^-π^ ＋ reaction.Firstly we re-fit the data for kaon beam momenta in the range of 1.0 - 1.8 GeV.Secondly we study the reaction at the energies around Λ＊（1520） peak.Both studies show evidence for the existence of Σ＊with J^ P = 1/2^-around 1380 MeV.Higher statistic data on relevant reactions are needed to clarify the situation.     

从ψ’→J/ψπ~+π~-衰变中抽取ππ相移(英文)

ψ’→J/ψπ+π-提供了一个抽取低于0.59GeV的ππS波相移的新途径.基于在树图衰变振幅中忽略D波的近似,给出了从ψ’→J/ψπ+π-的ππ不变质量谱中得到ππS波相移的公式.     

CS2 分子 1 B2(1 Σ+u )态预解离动力学研究

研究了CS2 分子1B2 (1Σ+u )预离解态线形势垒下的g振动能级光解动力学,包括预解离寿命、产物振转布居、平动振动转动能量分配和解离通道分支比.在实验过程中,一束可调谐激光激发超声射流冷却的CS2 分子到1B2 (1Σ+u )电子态,光解产物CS用另一束可调谐激光通过激光诱导荧光(LIF)方法检测.通过拟合光解碎片激发谱的谱峰轮廓,获得了源于不同跃迁初始态的1B2 (1Σ+u )态g振动能级的预解离寿命.通过分析CS的LIF光谱,则获得了不同光解波长下CS碎片的v=0~8振动态布居、v=1、4 ~8振动态的转动布居、能量分配以及两个预解离通道CS(X1Σ+ ) +S(3PJ)和CS(X1Σ+ ) +S(1D2 )的分支比.实验还考察了初始态弯曲振动量子数v2″、振动角动量量子数l对解离动力学的影响.发现v2″的影响不大,而l的影响却是明显的.较大的l(=K)对应于较短的寿命和较小的通道分支比S(3PJ) /S(1D2 ),即大的l(=K)有利于预解离的发生,同时更有利于产生S(1D2 ).     

利用BESⅢ的双层TOF寻找D~0-■混合的研究(英文)

在ψ(3770)处,D0→K-π+是研究D0-■混合的非常理想的衰变道．实验上,良好的K／π识别技术将对寻找D0-■混合过程起着决定性的作用．在BESⅢ实验的物理预研究中,发现利用飞行时间的信息,能够精确测定末态中含有多条带电径迹事例的起始时间,从而可以改善飞行时间计数器的时间分辨率．进一步的研究表明,应用该方法后,BESⅢ双层TOF的时间分辨率从～78ps降到～64ps．按照20fb-1的ψ(3770)数据量进行估算,在95％置信度下,D0-■混合率的上限值可以提高7％左右．     

Parameter analysis for a nuclear magnetic resonance gyroscope based on ~(133)Cs–~(129)Xe/~(131)Xe

We theoretically investigate several parameters for the nuclear magnetic resonance gyroscope based on ~(133)C_(s–)~(129)Xe/~(131)Xe. For a cell containing a mixture of ~(133)Cs at saturated pressure, we investigate the optimal quenching gas(N_2) pressure and the corresponding pump laser intensity to achieve 30% ~(133)Cs polarization at the center of the cell when the static magnetic field B0 is 5 μT with different ~(129)Xe/~(131)Xe pressure. The effective field produced by spin-exchange polarized ~(129)Xe or ~(131)Xe sensed by ~(133)Cs can also be discussed in different~(129)Xe/~(131)Xe pressure conditions. Furthermore,the relationship between the detected signal and the probe laser frequency is researched. We obtain the optimum probe laser detuning from the D2(6~2S_(1/2)→ 6~2P_(3/2)) resonance with different ~(129)Xe/~(131)Xe pressure owing to the pressure broadening.     

Search for exotic state 1~(- ) π_1(1400) at BESⅢ

The J/ψ hadronic decays provide good laboratory to search for the hybrid states with exotic quantum numbers. A full Partial Wave Analysis (PWA) is performed to the generated Monte Carlo J/ψ→ρηπ data, based on the design of BESⅢ detector, to study the sensitivity of searching for a possible exotic state at BESⅢ.     

Measurement of the CP-violation parameter sin2φ1 with a new tagging method at the Υ(5S) resonance

We report a measurement of the CP-violation parameter sin2φ1 at the Υ(5S) resonance using a new tagging method, called "B-π tagging." In Υ(5S) decays containing a neutral B meson, a charged B, and a charged pion, the neutral B is reconstructed in the J/ψK(S)(0) CP-eigenstate decay channel. The initial flavor of the neutral B meson at the moment of the Υ(5S) decay is opposite to that of the charged B and may thus be inferred from the charge of the pion without reconstructing the charged B. From the asymmetry between B-π(+) and B-π(-) tagged J/ψK(S)(0) yields, we determine sin2φ1=0.57±0.58(stat)±0.06(syst). The results are based on 121 fb(-1) of data recorded by the Belle detector at the KEKB e(+)e(-) collider.     

≡BARYONS(S=-2,I=1/2)≡~0=uss,≡~-=dss

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Si(001)-(2*2*1):H表面O2吸附的密度泛函理论研究

建立了一种计算Si(001)-(2×2×1):H表面O2吸附的理论模型．在周期性边界条件下,采用基于密度泛函理论广义梯度近似的超软赝势法对Si(001)-(2×2×1):H表面O2吸附进行了第一性研究．通过占位能的计算,得到了Si(001)-(2×2×1):H表面O2的最佳吸附位置．计算结果表明吸附后的反应产物应为Si=O和H2O,从理论上支持了D．Kovalev等人提出反应机制．     

钪原子的自电离里德伯能级3d4s(~1D_2)nf~2D_(3/2),3d4s(~1D_2)nf~2F_(5/2)和3d4s(~1D_2)np~2D_(3/2)的理论研究

在多通道量子亏损理论框架下,利用相对论多通道理论,分别在冻结实近似和考虑偶极极化下计算钪原子的Jπ=(3/2)-,(5/2)-的三个收敛于[Ar]3d4s(1D2)的自电离里德伯系列的能级.对3d4s(1D2)np2D3/2和3d4s(1D2)nf2F5/2这两个系列,计算结果表明,考虑偶极极化效应后,理论计算和实验测量的量子数亏损之差普遍小于0.01.而对3d4s(1D2)nf2D3/2系列,考虑偶极极化效应后的结果和仅考虑冻结实的结果比较接近,理论计算和实验测量的量子数亏损之差普遍在0.04左右.     

~(206)At的[лh_(1/2)vi_(13/2)~(-1)]10~-同质异能态研究(英文)

利用能量为６０－８０ＭｅＶ的~(１２)Ｃ束流,通过~１９７Ａｎ（~(１２)Ｃ,３ｎ）~２０６Ａｔ反应研究了~２０６Ａｔ核的高自旋能级结构．用７台ＢＧＯ（ＡＣ）ＨＰＧｅ探测器和一台用于探测低能γ射线的平面型ＨＰＧｅ探测器进行了γ射线的激发函数、γ－γ－ｔ符合及γ射线的角分布测量．基于这些测量,首次建立了包括２５条γ跃迁的~２０６Ａｔ高自旋能级纲图．确定了一个半寿命为（９０８±４００）ｎｓ、自旋和宇称为１０的同质异能态．基于较重的双奇核~(２０８,２１０ )Ａｔ能级结构的系统性,对~(２０６)Ａｔ的１０~－同质异能态进行了讨论．     

NaK(61Σ+)与H2碰撞传能中的H2的振转态分布

光学-光学双共振激发NaK至61Σ+高位电子态,研究了NaK(61Σ+)与H₂的电子-振转能量转移。利用相干反斯托克斯拉曼散射(CARS)光谱技术检测H₂的振转态分布。扫描CARS谱表明H₂在(1,1),(2,1),(2,2),(2,3),(3,1),(3,2),(3,3)和(3,5)振转能级上有布居。对于(3,1), (3,2), (3,3)和(3,5)能级,扫描CARS谱峰值直接给出布居数之比。对于(1,1), (2,1), (2,2)和(2,3)能级,扫描CARS谱峰值给出二个可能的布居数之比,利用一个速率方程组,由时间分辨CARS轮廓可以得到真实的比值。用n₁～n₈分别表示H₂的(3,1), (2,1), (1,1), (3,3), (2,3), (2,2), (3,2)和(3,5)能级上布居密度,得到n₂/n₁～n₈/n₁分别为0.51,0.97,0.45,0.18,0.10,0.26和0.31。利用Stern-Volmer公式,得到61Σ+态的总退布速率系数为(2.1±0.4)×10-10 cm3s-1, 由H₂各振转能级布居数之比,得到61Σ+-(1,1), (2,1), (2,2), (2,3), (3,1), (3,2), (3,3)和(3,5)转移速率系数(10-11 cm3·s-1单位)分别为5.4±1.6,2.8±0.8,0.6±0.2,1.0±0.3,5.6±1.7,1.4±0.4,2.5±0.8和1.7±0.5。     

气体分子运动速度=2~(1/2)v关系式的简易推导方法

对 u =2 v式给出了适合工科普通物理教学的简易推导方法     

Theoretical prediction of the optimal conditions for observing the stereodynamical vector properties of the C(~3P) + OH(X~2Π) → CO(X~1 Σ~+) + H(~2S) reaction

The best optimal initial reactant state and collision energy for observing the stereodynamical vector properties of the title reaction in the ground electronic state X2A potential energy surface(PES) [Zanchet et al. 2006 J. Phys. Chem. A 110 12017] are theoretically predicted using the quasi-classical trajectory(QCT) method for the first time. The calculated results reveal that the smallest value of the rotational quantum number j, larger vibrational quantum number v, and the lower strength of collision energy should be selected for offering the most obvious picture about the stereodynamical vector properties. Polarization-dependent differential cross sections and the angular momentum alignment distribution, P(θr) and P(Φr) in the center-of-mass frame, are obtained to gain an insight into the alignment and orientation of the product molecules. The rotational angular momentum vector j of CO is aligned to be perpendicular to reagent relative velocity k. The product polarizations align along the y axis, pointing to the positive direction of the y axis. A new method is developed to investigate massive reactions with various initial states and to further study the vector properties of the fundamental reactions in detail.     

Measurement of astrophysical S-factor for 9Be(d, α0)7Li and 9Be(d, α1)7Li* reactions at low energies

The thick-target yield of the ⁹Be(d,α0)7Li and ⁹Be(d,α1)7Li*reactions has been first directly measured over deuteron energies from 66 to 94 keV.The obtained S(Ei)ofα0 andα1 have similar trends calculated by the thin-target yield,consistent with Yan’s report within the errors.Furthermore,the parametric expression of S(E)was obtained to calculate the theoretical thick target yield,and it roughly agrees with the experimental thick target yield.     

Nuclear magnetic moments for J~π=2_1~+ state of ~(10)Be with ab initio Monte Carlo shell model calculation

The magnetic moment of 2+1 state for 10Be are calculated and investigated in terms of single particle orbits for protons and neutrons under the framework of ab initio Monte Carlo shell model method in an emax = 3 model space. The reduced matrix elements of orbital and spin angular momentum are evaluated. It is found that the orientations of orbital angular momentum in diferent single particle orbits are consistent. Conversely,the orientations of spin in diferent single particle orbits tend to be chaotic. The nuclear magnetic moment of 2+1 state for 10Be is obtained as 1.006N and is discussed in regards to the contribution of orbital and spin angular momentum both for protons and neutrons. The corresponding g-factor is also given.     

关于“=2~(1/2)的一个简易证明”的讨论

普通物理中一些言而不详的问题是普通物理教学中难以处理的问题之一。《大学物理》83年第5期上朱湘桂同志的“关于u=2v的一个简易证明”一文是解决上述问题的一个有意义的尝试.但对其中有些论述我有不同看法,特提出讨论.一、我认为得出u=2v这个结论,正是运用了麦克斯韦速率分布率的结果,避免运用麦克斯韦速率分布率这个前提,是得不出这个结论的.二、相对速率与各个分子速度之间的夹角是有关系的,但只要研究某一时刻所研究的分子与各个分子速度之间的夹角就行了,不必要既求碰撞前的,又求碰撞后的.这有利于节约教学时间.三、证明了各速度之间…     

乙醇-水分子团簇(C2H5OH)nH2O(n=1-4)的稳定结构特性研究

采用密度泛函理论M06-2X方法, 在6-311 ++G(2d,2p)// 6-311 ++G(d,p)基组水平上对乙醇-水分子团簇(C2H5OH)nH2O(n=1-4)进行计算, 得到乙醇-水分子团簇的各种稳定构型, 并对乙醇水分子团簇的结构特点进行了分析, 优化的各种低能结构、结构参数、氢键、结合能、平均氢键参数、NBO电荷分布等．结果表明: 最低能稳定结构都是环状的, 而且这些团簇除了形成O―H…O型主氢键外, 还有另一种作用方式C―H…O, 称之为次氢键．虽然C―H…O氢键远弱于O―H…O氢键, 但是对团簇的某些性质也有一定的影响.     

乙醇-水分子团簇(C2H5OH)nH2O(n=1-4)的稳定结构特性研究

采用密度泛函理论M06-2X方法, 在6-311 ++G(2d,2p)// 6-311 ++G(d,p)基组水平上对乙醇-水分子团簇(C2H5OH)nH2O(n=1-4)进行计算, 得到乙醇-水分子团簇的各种稳定构型, 并对乙醇水分子团簇的结构特点进行了分析, 优化的各种低能结构、结构参数、氢键、结合能、平均氢键参数、NBO电荷分布等．结果表明: 最低能稳定结构都是环状的, 而且这些团簇除了形成O―H…O型主氢键外, 还有另一种作用方式C―H…O, 称之为次氢键．虽然C―H…O氢键远弱于O―H…O氢键, 但是对团簇的某些性质也有一定的影响.