二步过程生成(ΩΩ)0+机制的研究

研究了一个生成（ΩΩ）0^ 的二步过程：第一步过程为N Ω→(NΩ）022 γ，或NΩ→(NΩ)022 π；第二步为Ω （NΩ）022→（ΩΩ）000 N。结果表明这个二步过程的每一步的截面都比较大，有可能是一个生成（ΩΩ）0^ 的重要途径。     

标量介子场对(ΩΩ)(0+)态生成截面的计算

研究了Ω+Ω→(ΩΩ)0++σ(ε)过程生成(ΩΩ)0+双重子态的截面.结果表明这个过程的生成截面比已计算过的其他Ω+Ω→(ΩΩ)0++X(赝标介子或矢量介子)过程的截面要大一至两个量级.因此这可能是一个值得考虑的(ΩΩ)0+生成途径.     

Snn=200GeV下Au-Au中心碰撞中di-omega产额上限的蒙特卡洛模拟

根据现有的关于(ΩΩ)0+的生成截面的理论计算, 利用HIJING事例产生器研究 了s nn=200GeV下Au-Au中心碰撞中(ΩΩ)0+和NΩ022产生过程, 分别对(ΩΩ)0+的电磁作用产生过程和两步产生过程中的第一步过程进行了(ΩΩ)0+产率的计算, 给出了(ΩΩ)0+产额的上限. 对于电磁作用过程, 其产率为(1.097±0.293)×10^-10. 同时我们也对(NΩ)₀₂₂进行了初步的模拟, 初步给出了它的产率为(0.894±0.005)×10^-4.     

(S_(nn))~(1/2)=200GeV下Au-Au中心碰撞中Di-omega产额上限的蒙特卡罗模拟(英文)

根据现有的关于(ΩΩ)0 的生成截面的理论计算,利用HIJING事例产生器研究了(S_(nn))~(1/2)=200GeV下Au- Au中心碰撞中(ΩΩ)0 和(NΩ)022产生过程,分别对(ΩΩ)0 的电磁作用产生过程和两步产生过程中的第一步过程进行了(ΩΩ)0 产率的计算,给出了(ΩΩ)0 产额的上限,对于电磁作用过程,其产率为(1.097±0.293)×10-10 同时我们也对(NΩ)022进行了初步的模拟,初步给出了它的产率为(0.894±0.005)×10-4.     

一个新的双重子态(ΩΩ)Jπ=0+的研究

用手征SU(3)夸克模型对双重子态(ΩΩ)0⁺的结构进行了研究,这个双重子态的结合能约100MeV,2个Ω间均方根距离0.84fm,初步估计其平均寿命约是自由Ω寿命的两倍.由于这些有兴趣的性质以及带有两个负电荷的特性,它有利于在重离子碰撞实验过程中去识别.     

Structures of（ΩΩ）0＋and（[1]Ω）1＋in Extended Chiral SU（3） Quark Model

The structures of (ΩΩ)0 and ([1]Ω)1 are studied in the extended chiral SU(3) quark model in which vector meson exchanges are included. The effect from the vector meson fields is very similar to that from the one-gluon exchange (OGE) interaction. Both in the chiral SU(3) quark model and in the extended chiral SU(3) quark model,di-omega (ΩΩ)0 is always deeply bound, with over one hundred MeV binding energy, and ([1]Ω)1 ‘s binding energy is around 20 MeV. An analysis shows that the quark exchange effect plays a very important role for making di-omega (ΩΩ)0 deeply bound.     

Exotic ΩΩ dibaryon states in a molecular picture

We investigate the exotic ΩΩ dibaryon states with J^P=0⁺and 2⁺in a molecular picture.We construct a tensorΩΩmolecular interpolating current and calculate the two-point correlation function within the method of QCD sum rules.Our calculations indicate that the masses of the scalar and tensor dibaryon states are mΩΩ,0⁺=(3.33±0.51)GeV and mΩΩ,2⁺=(3.15±0.33)GieV,respectively,which are below the 2mΩthreshold.Within error,these results do not negate the existence of loosely bound molecularΩΩdibaryon states.These exotic strangeness S=-6 and doubly-chargedΩΩdibaryons,if they exist,may be identified in heavy-ion collision processes in the fu-ture.     

Structures of (ΩΩ)0 and (([1])Ω)1 in Extended Chiral SU(3) Quark Model

The structures of (ΩΩ)0 and (([1])Ω)1 are studied in the extended chiral SU(3) quark model in whichvector meson exchanges are included. The effect from the vector meson fields is very similar to that from the one-gluonexchange (OGE) interaction. Both in the chiral SU(3) quark model and in the extended chiral SU(3) quark model,di-omega (ΩΩ)0 is always deeply bound, with over one hundred MeV binding energy, and (([1])Ω)1 ‘s binding energyis around 20 MeV. An analysis shows that the quark exchange effect plays a very important role for making di-omega(ΩΩ)0 deeply bound.     

高激发振动态RbH（Х1Σ+,ν″=15～22）与H2,N2的振动-振动碰撞能量转移

脉冲激光激发Rb原子至6 D态,Rb(6 D)与H2反应生成RbH(Х1Σ+,ν″=0～2)振动态。研究了RbH(Х1Σ+)高位振动态与H2,N2间的碰撞弛豫过程,利用泛频泵浦分别激发Х1Σ+(ν″=0)至Х1Σ+(ν″=15～22)各振动态,检测激光激发Х1Σ+(ν″)至A1Σ+(ν′),测量A1Σ+(ν′)的时间分辨激光感应荧光光谱,利用Stern-Volmer方程,得到振动能级ν″的总的弛豫速率系数kν(H2)。在H2和N2的混合气体中,总弛豫速率系数kν(H2+N2)与α(H2的摩尔配比)成直线的关系,其斜率为kν(H2)-kν(N2),而截距为kν(N2)。对于ν″<18主要发生单量子弛豫(Δν=1)过程,kν(H2)和kν(N2)与振动量子数ν″均成线性增加关系。对于ν″≥18,多量子弛豫(Δν≥2)过程及共振振动-振动转移起重要作用。对于RbH(ν″=21)+N2(0),测量ν″=16的布居数时间演化轮廓,在20μs内有一个锐锋,在100～200μs内有一个较低的宽峰,锐锋相应于RbH(ν″=21)+N2(0)→RbH(ν″=16)+N2(1)的共振转移过程,而宽峰是由相继的单量子过程产生的。     

手征SU(3)夸克模型与六夸克态的研究

用手征 SU( 3)夸克模型分析了 ( 0 s) 6组态的六夸克态能量 ,结果表明手征 SU( 3)介子场可以对某些多奇异数的态提供较强的吸引作用 .进一步用共振群方法研究了 ( ΩΩ) 0 + 及 ( ΩΞ) 1+ 等多奇异数系统 ,得到 ( ΩΩ) 0 是一个深度束缚的双重态. An analysis is made for the (0s) 6 six quark cluster states in the chiral SU (3) quark model. The results show that for some multistrangeness states the chiral SU (3) could offer more attraction. Further RGM dynamical calculation of the multistrangeness system (ΩΩ) 0+ and (ΩΞ) 1+ has been done. It shows that (ΩΩ) 0+ is a deeply bound state in the chiral SU (3) quark model.