Glueball Masses from Hamiltonian Lattice QCD

We calculate the masses of the 0⁺⁺, 0^-- and l^+- glueballs from QCD in 3+1 dimensions using an eigenvalue equation method for Hamiltonian lattice QCD developed and described by S.H. GUO et al. The mass ratios become approximately constants in the coupling region 6/g²∈[6.0,6.4], from which we estimate M(0^--)/M(0⁺⁺) = 2.44 ± 0.05 ± 0.20 and M(l^+-)/M(0⁺⁺) = 1.91 ± 0.05 ± 0.12.     

胶子非弹性散射过程对夸克胶子等离子体中双轻子产生的影响

双轻子是研究夸克物质的形成和性质的重要探针.本文基于化学平衡化的黏滞性夸克胶子等离子体演化模型,计算了相对论重离子碰撞能量下金-金对心碰撞形成的夸克胶子等离子体中的双轻子产额.在黏滞性计算中加入了胶子非弹性散射过程对黏滞系数的贡献.相较仅考虑夸克和胶子弹性散射的情况,双轻子的产额有较明显的降低.这表明在黏滞系数中加入胶子非弹性散射的贡献使得系统的演化过程加快,演化时间变短.     

Ultralight glueballs in Quark-Gluon Plasma

We consider the dynamics of the scalar and pseudoscalar glueballs in the Quark-Gluon Plasma (QGP). By using the instanton model for the QCD vacuum we give the arguments that the nonperturbative gluon-gluon interaction is qualitatively different in the confinement and deconfinement phases. Based on this observation it is shown that above T _c the values of the scalar and pseudoscalar glueball masses might be very small. The estimation of the temperature of scale invariance restoration, at which the scalar glueball becomes massless, is given. We also discuss the Bose—Einstein condensation of the glueballs and the superfluidity of the glueball matter in QGP.     

Ω Production and Corresponding Ratio of Antiparticle to Particle in Relativistic Nucleus-Nucleus

We use the event generator LUClAE to analyze the WA85 data of ratio of Ω^- to Ω^- in reaction (200A GeV/c)S + W. The result indicates that the reproduction of WA85 data might be achieved in hadronic rescattering regime of LUCIAE and might need not to rely on the formation of QGP.     

Glueballs as bound states of massive gluons

Recent work in both lattice and continuum QCD shows that the gauge field is massive. We investigate the bound states of massive gluons with a Schrödinger equation and find M(0⁺⁺) ≈ 2.3 m, M(0⁻⁺) ≈ 2.7 m, M(2⁺⁺) ≈ 3.2 m, where m is the gluon mass; we expect from this as well as earlier work that m ≈ 500 MeV. These glueballs have widths typical of allowed hadronic decays.     

Transmission of low-energy (< 10 eV) O ions through Au films on TiO2(110)

In an attempt to identify the fundamental processes that influence ion transport through metallic surface layers, we have studied the transmission of O⁺ ions through discontinuous Au films adsorbed on TiO₂(110). A low energy (< 10 eV) O⁺ ion beam is generated via electron stimulated desorption when an Au-dosed TiO₂(110) substrate is bombarded with a focused 250 eV electron beam. Low energy ion scattering data indicate that Au evaporated under ultrahigh vacuum conditions at 300 K forms three-dimensional clusters on TiO₂(110). As the Au coverage increases, the formation of Au clusters on TiO₂(110) blocks a fraction of the TiO₂ surface and the O⁺ yield is attenuated. However, for high coverages (≥30% Au covered substrate) the O⁺ signal decreases at a faster rate than the TiO₂ open area fraction. We attribute the attenuation of the O⁺ yield for high Au coverages mainly to blocking of O⁺ by Au clusters, to deflection of trajectories by the image force between ions and Au clusters, and to charge transfer between desorbing O⁺ and neighboring Au clusters.     

Ion-size effects on the structure and superconductivity of La-214 compounds at 1/8 doping

A structural transition to a low-temperature tetragonal (TLT) phase occurs below T_d2≈60 K in La_2−xBa_xCuO₄ only around x=0.125, accompanied by sharp suppression of superconductivity. In this study we investigated the effects of partial substitution of smaller divalent cations for Ba²⁺ ions (Ba²⁺ > Sr²⁺ > Ca²⁺) on these anomalous low-temperature properties. The suppression of superconductivity is strongly affected by the appearance of the TLT phase for this carrier concentration. We also show that the variations of T_d2 and T_c are quantitatively scaled by the averaged size of cations at the La site. This dependence can be interpreted as chemical effects acting effectively as applied pressure. We discuss how our observation is related to recent reports which claim that the TLT structure itself does not necessarily destroy the superconductivity.     

Search for Exotic Strange Dibaryon in Relativistic Heavy Ion Collisions

The exotic strange dibaryon particle (ΩΩ)0 with S = -6 can be produced in relativistic heavy ion collisions. The yields of this kind of exotic strange dibaryon particles can increase signitlcantly soon as the formation of QGP does exhibit after the collision. If there is no phase transition after the collision, the upper bound of the production of this diomega can be estimated from the free hadronic gas model for nuclear matter. The relative yield ratio of diomega to deuteron is less than 0.000205, this means that if there is no QGP creation it is difficult to observe the production of diomega in relativistic heavy ion collisions.     

Er3+单掺和Er3+/Yb3+共掺碲酸盐玻璃的光谱性质及能量传递

采用高温熔融法制备了新型Er3+单掺和Er3 +/Yb3+共掺的TeO2-Bi2O3-SiO2-B2O3玻璃,测试并分析了样品的吸收光谱、发射光谱以及Er3 +/Yb3共掺杂样品的发射光谱和荧光寿命.计算出了玻璃的J-O强度系数Ωt(t=2,4,6);系统讨论了Er3+/Yb3+共掺杂样品在808 nm激光激发下,Yb...     

稀土掺杂镝(Ⅲ)乙酰丙酮邻菲咯啉三元配合物的合成和荧光性质

合成了三个系列稀土掺杂镝乙酰丙酮(Hacac)邻菲咯啉(phen)三元配合物RE_xDy_1-x(acac)₃phen(RE=La,Y,Gd;x=0,0.10,0.20,0.30,0.50,0.70,0.90,1.00),通过紫外光谱、红外光谱、X射线粉末衍射对配合物进行了表征。对各系列配合物进行荧光光谱研究,发现La³⁺、Y³⁺、Gd³⁺对Dy³⁺离子均有荧光增敏作用,它们对Dy³⁺离子的荧光增强顺序为I(La³⁺)>I(Y³⁺)≈I(Gd³⁺)。当x=0.10~0.30,所有掺杂配合物的荧光强度都大于未掺杂的配合物Dy(acac)₃phen的荧光强度。     

惰性稀土离子和抗衡离子对2-噻吩乙醛酸-铕配合物荧光性能的影响

研究了惰性稀土离子和抗衡离子对一系列2-噻吩乙醛酸-铕配合物荧光性能的影响。分别在2-噻吩乙醛酸-邻菲罗啉-铕和2-噻吩乙醛酸-三苯基氧化膦-铕两个体系中按不同比例掺入钇和钆,研究了它们的荧光光谱。结果表明,钇的加入对2-噻吩乙醛酸-邻菲罗啉-铕体系的荧光强度有很强的敏化作用,并且随加入量的增加,这种敏化作用逐渐增强。钇的加入对2-噻吩乙醛酸-三苯基氧化膦-铕体系则呈现出弱的敏化作用,且在一定程度上具有猝灭作用,但这两种作用都是很微小的。钆在少量加入时对2-噻吩乙醛酸-三苯基氧化膦-铕体系具有猝灭作用,当大量加入时则呈现出很强的敏化作用。不同的抗衡离子对配合物的影响是明显的。在二元配合物中,氯化物体系的固体荧光强度最大;在三元配合物中,硝酸盐体系的固体荧光强度最大。     

Identification of the phosphorus-doping defect in MgS as a potential qubit

The P_S defect is obtained by replacing one S atom with one P atom in the wide-bandgap semiconductor MgS. Based on first-principles calculations, the formation energy, defect levels, and electronic structure of the P_S defect in different charge states are evaluated. We predict that the neutral P_S⁰ and positively charged P_S⁺¹ are the plausible qubit candidates for the construction of quantum systems, since they maintain the spin conservation during optical excited transition. The zero-phonon lines at the P_S⁰ and P_S⁺¹ defects are 0.43 eV and 0.21 eV, respectively, which fall in the infrared band. In addition, the zero-field splitting parameter D of the P_S⁺¹ with spin-triplet is 2920 MHz, which is in the range of microwave, showing that the P_S⁺¹ defect can be manipulated by microwave. Finally, the principal values of the hyperfine tensor are examined, it is found that they decay exponentially with the distance from the defect site.     

Sm~(3+),Sr~(2+)共掺杂对CeO_2基电解质性能影响的密度泛函理论+U计算

Sm~(3+),Sr~(2+)共掺杂CeO_2的离子电导率被证实可高达Sm~(3+)掺杂CeO_2离子电导率的近两倍,然而,共掺杂对CeO_2电导率的作用机理尚不明确.本文利用第一性原理计算的密度泛函理论+U方法,对Sm~(3+)和Sr~(2+)共掺杂的CeO_2进行了系统的研究,对比Sm~(3+)或Sr~(2+)单掺杂的CeO_2体系,计算并分析了共掺杂体系的电子态密度、能带结构、氧空位形成能以及氧空位迁移能等微观属性.计算结果表明,Sm~(3+),Sr~(2+)的共掺杂对CeO_2基电解质性能的提高具有协同效应,二者的共掺杂不仅能协同抑制CeO_2体系的电子电导率,还能在单掺杂CeO_2的基础上进一步降低氧空位形成能,Sm~(3+)的存在还有助于降低Sr~(2+)对氧空位的俘获作用,而Sr~(2+)的加入则能够在Sm~(3+)掺杂CeO_2的基础上进一步降低最低氧空位迁移能,爬坡式弹性能带方法计算表明共掺杂体系的氧空位迁移能最低可达0.314/0.295 eV,低于Sm~(3+)掺杂CeO_2的最低氧空位迁移能.研究揭示了Sm~(3+),Sr~(2+)共掺杂对CeO_2电导率的协同作用机理,对进一步研发其他高性能的共掺杂电解质材料具有重要的指导意义.     

Gelation in Generalized Smoluchovski Equation

We consider a system of substances A_j reacting according to the scheme: A_i + A_j +A_k A_i+j+k, which is described by the generalized Smoluchovski equation. We discuss the existence of global solutions of this kinetic equation, and show that the total number of monomers may decrease as the result of the formation of infinite clustere (gelation) for some special coagulation kernels. We also solve the case R(i, j, κ) = s_is_js_κ with s_κ = Ak + B explicitly, and find that the gelation indeed occurs at t_c = (6A + B)/6A²(A + B)².     

The Three-Pion Decays of the a1(1260)

We investigate the decay of a₁⁺ (1260)→π⁺π⁺π^- with the assumption that the a₁(1260) is dynamically generated from the coupled channel ρπ and KK^* interactions. In addition to the tree level diagrams that proceed via a₁⁺ (1260)→ρ⁰π⁺→π⁺π⁺π^-, we take into account also the final state interactions of ππ→ππ and KK→ππ. We calculate the invariant π⁺π^- mass distribution and also the total decay width of a₁⁺ (1260)→π⁺π⁺π^- as a function of the mass of a₁(1260). The calculated total decay width of a₁(1260) is significantly different from other model calculations and tied to the dynamical nature of the a₁(1260) resonance. The future experimental observations could test of model calculations and would provide vary valuable information on the relevance of the ρπ component in the a₁(1260) wave function.     

HYPERON DECAYS IN THE CNIRAL BAG MODEL

In terms of the chiral bag model and SD(3) Skyrme wave-functions of baruons, we investigate Δ⁺ →Pγ (SU(2)) and Σp⁺ → Pπ⁰ (SU(3) case) hyperon decays. We have found that for Δ⁺ →Pγ the Skyrme contribution is more important whereas in Σp⁺ → Pπ⁰ the quark content transition dominates.     

Ba2+离子掺杂CsPbBr3蓝光量子点合成及其光学性能

近年来,全无机卤素钙钛矿CsPbX3(X=Cl,Br,I)因其荧光带宽窄、带隙可调、合成工艺简单以及荧光量子产率(Photoluminescence quantum yield,PLQY)高等优点而被应用于光电器件领域.但相比于PLQY接近于100％的红光与绿光CsPbX3量子点,PLQY低于10％的蓝光量子点光学性能...     

The Generalized Moment Analysis (GMA) and Spin Analysis for Boson Resonances

Our analyais^[1] has shown that there exist sensitive and insensitive regions to determine the spin (J = 2 or 4) of ξ(2230) in the general helicity formalism. Whereaa it just falls into the insensitive region by using current data of ξ. If the number of events is not sufficient it is difficult to determine the spin of ξ^[2]. In this paper we generalize the moment analysis^[3]. We define the photon angular distribution H_J(θ_τ, LM) for the moment of process e⁺ +R^- → J/ψ → τ + ξ, ξ → p + p and the weighted moment by choosing appropriate weight function. They provide an effective criterion to determine the spin of ξ. We also use the method to discuss LIE puzzle for process e⁺ + e^- → J/ψ → τ + B₁ B → P₁ + P₂ + P₃.     

Thermoluminescence mechanism of Mn, Mg and Sr doped calcite

In this work, the thermoluminescence properties of synthetic crystals of doped calcite were studied. Samples were doped with Mn²⁺, Mg²⁺ or Sr²⁺, either individually or simultaneously with more than one of these impurities. TL glow curves, partial heating measurements, isometric curves, emission spectra and thermal treatment were performed, in order to investigate the role played by the impurities in the TL glow peaks of calcite. We conclude that the crystals doped with Mn²⁺ show five TL peaks with emission spectra due only to the Mn²⁺. The relative intensity of these peaks is closely related to the other divalent dopant added in the solution (Sr²⁺ or Mg²⁺). These results suggest that although Sr²⁺ and Mg²⁺ act as TL activators stabilising slightly different electron traps, they are not directly connected to the Mn²⁺ luminescence centre.