C12（d,p）C13反应中存在一个中间结构的可能性

在氘核能量为0.5-2.5MeV能区,测量了C¹²（d,d）C¹²,C¹²（d,p₀）C_8.3.¹³,C¹²（d,p₁）C_13t¹³,C¹²（d,p₂）C_2nd¹³和C¹²（d,p₃）C_3rd¹³反应在几个角度上的激发函数,及在一些能量点上的角分布。围绕E_d=1.73MeV附近,在角分布和激发函数中出现有规律变化趋势,讨论了不同反应机制之间相干,并探讨了孤立“门态”存在的可能性。     

低重复率的Ti:Al2O3飞秒激光放大器研究

本文报道了重复频率为10Hz的Ti:Al₂O₃飞秒激光放大器的研究.基于脉冲啁啾放大技术和采用再生/多通放大装置,得到了能量为8mJ的放大光脉冲,在该放大系统中,激光脉冲获M净增益约8×10⁷.     

31.2MeV α粒子在B核上的(α,t)、(α,d)和(α,p)反应的研究

我们用粒子鉴别系统测量了31.2MeV的α粒子在^11,10B核上的(α,t)、(α,d)和(α,p)反应的角分布; 由出射粒子的能谱, 我们分别得到了剩余核处于基态和不同激发态的十个角分布. 从角分布的形状看, 在¹¹B(α,t₀)¹²C_g﹒s, ¹¹B(α,d₀)¹³C_g﹒s, ¹⁰B(α,d₀)¹²C_g﹒s, ¹⁰B(α,d₁)¹²C_1st, ¹¹B(α,p₀)¹⁴C_g﹒s等反应中均有不同程度的后角上翘; 并且(α,t₀)和(α,p₀)的后角上翘的同位素效应似乎与(α, α)的反常散射的同位素效应相反.     

12C（d,d）12C及12C（d,p）13C反应机制的研究

本文用S矩阵理论给出:研究直接过程与复合共振过程相干机制的方法及计算公式;并用它分析了1.63MeVd<2.05MeV能区¹²C（d,d）¹²C、¹²C（d,p₁）¹³C^*及¹²C（d,p₂）¹³C^*反应的机制.结果表明:在此能区内,两种反应机制相干是存在的;并给出了他们之间的定量关系.同时还定出各种直接过程和复合共振过程参数,特别是确定了E_d=1.726,1.767,1.792及1.86MeV 4个共振态的参数.     

LD泵浦Nd:GdVO4晶体Cr4+:YAG被动调Q激光特性研究

考虑腔内光子数密度的空间高斯分布以及晶体热效应的影响,给出了LD泵浦Nd:GdVO₄ 晶体Cr⁴⁺:YAG被动调Q 1.06 μm激光的耦合速率方程组.数值求解该方程组获得了输出激光的脉冲宽度、重复率、峰值功率以及单脉冲能量随泵浦功率的变化特性,其理论值与实验结果相符.     

Searches for the technicolor signatures via gg → W±πt± at the Large Hadron Collider

In this paper, we calculate the production of a charged top pion in association with a W boson via gg fusion at CERN's Large Hadron Collider in the context of the topcolor assisted technicolor model. We find that the total cross section of pp → gg → W^±π_t is several dozen femtobarns with reasonable values of the parameters, and the total cross section of pp → W^±π_t can reach a few hundred femtobarns when we consider the sum of the contributions of these two parton subprocesses, gg → W^±π_t and bb → W^±π_t.     

Single top production associated with a neutral scalar at LHC in topcolor-assisted technicolor

The topcolor-assisted technicolor (TC2) model predicts a number of neutral scalars like the top-pion (π⁰_t) and the top-Higgs (h⁰_t). These scalars have flavor-changing neutral-current (FCNC) top quark couplings, among which the top-charm transition couplings may be sizable. Such FCNC couplings induce single top productions associated with a neutral scalar at the CERN Large Hadron Collider (LHC) through the parton processes cg→t π⁰_t and cg→t h⁰_t. In this paper we examine these productions and find their production rates can exceed the 3σ sensitivity of the LHC in a large part of parameter space. Since in the Standard Model and the minimal supersymmetric model such rare productions have unobservably small production rates at the LHC, these rare processes will serve as a good probe for the TC2 model.     

掺铒碲钨酸盐玻璃光谱性质的研究

合成了不同浓度Er³⁺掺杂的TeO₂-WO₃-Li₂O体系玻璃（TW glasses）,详细研究了掺杂浓度对这种碲钨酸盐玻璃光学特性的影响。计算了Judd Ofelt(J-O)强度参数,研究了掺杂浓度对15 μm发射带宽的影响,及不同掺杂浓度下Er³⁺的⁴I_11/2-⁴I_13/2和⁴I_13/2-⁴I_15/2无辐射跃迁过程。实验得到了在TW 玻璃中Er³⁺的⁴I_13/2-⁴I_15/2跃迁的浓度猝灭速率约为跃迁的浓度猝灭速率约为0.8×10^-18cm³·s^-1,这对寻求Er³⁺在碲钨酸盐玻璃中的合理掺杂浓度有一定的参考意义,这对寻求Er³⁺在碲钨酸盐玻璃中的合理掺杂浓度有一定的参考意义。实验发现Er³⁺的⁴I_11/2-⁴I_13/2无辐射弛豫速率在这种玻璃体系中约是不含WO₃的碲酸盐玻璃中的2倍,说明含WO₃的掺铒碲钨酸盐玻璃更有利于在980 nm激光泵浦下实现15 μm光放大。     

Sol-gel法制备Er3+-Yb3+共掺杂Al2O3粉末光致发光特性

采用异丙醇铝[Al(OC₃H₇)₃]为前驱体,溶胶-凝胶(Sol-gel)法制备Er³⁺-Yb³⁺共掺杂Al₂O₃粉末.实验结果表明:900 ℃烧结的粉末为固溶Er³⁺、Yb³⁺的γ-(Al,Er,Yb)₂O₃相和少量θ-(Al,Er,Yb)₂O₃相的混合物.Er³⁺-Yb³⁺共掺杂Al₂O₃粉末具有中心波长为1.533 μm的光致发光(PL)特性.1 mol % Er³⁺和1 mol% Yb³⁺共掺杂的Al₂O₃粉末的PL强度较1 mol % Er³⁺掺杂提高2倍,半峰宽从53 nm增加到63 nm.随泵浦功率的提高,PL强度呈线性增加后渐呈饱和趋势.     

坡莫合金纳米粉的恒导磁性及其磁导率的压力、频率特性

 用蒸发冷凝法制备了Fe-50wt%Ni和Fe-84wt%Ni坡莫合金的纳米微粉。经透射电镜X光能谱微区成分分析证实：微粉的成分与原材料的一致；微粉的平均粒径分别为16 nm（Fe-50Ni）和19 nm（Fe-84Ni）。在室温和36个不同的流体静压力（0.000 1~2.205 GPa）下原位测量了它们的磁化和起始磁化曲线。结果表明：（1）Fe-50wt%Ni和Fe-84wt%Ni合金纳米微粉均具有恒导滋特性；（2）这两种纳米粉的起始磁导率随静水压的变化分别为μ_i=8.16+18.2p-24.7p²+18.1p³-6.55p⁴+0.908p⁵（Fe-50Ni合金）和μ_i=5.38-0.169p+0.232p²-0.0786p³（Fe-84Ni合金）；（3）纳米粉的起始磁导率μ_i在频率高于10 MHz才降低，而Fe-50Ni合金片的μ_i在频率高于1 MHz，Fe-84Ni高于100 kHz时就开始下降，故纳米压粉磁芯可应用的频率范围可以比相应组分合金片的大1~2个数量级。     

Searching for a neutral top-Higgs in association with top-quark pairs at an e~+e~- collider in the TC2 model

We investigate the associated production of the neutral top-Higgs h_t⁰ with a pair of top-quarks in the context of the topcolor-assisted technicolor (TC2) model at the future e⁺e^- Linear Colliders (LC) i.e. e⁺e^- → tt h_t⁰. We calculate the production rate and present the distributions of the transverse momenta of top-Higgs and top-quarks. The results show that the total cross section is typically of the order of 1.0-7.5 fb in the energy range between 1000 GeV and 2000 GeV of the LC for the whole top-Higgs mass region of interest. It should be distinctly possible that hundreds or even thousands of h_t⁰ signals can be produced per year at the LC given the luminosity L=500 fb^-1.     

Signature splitting in 129Ce

The high spin states of ¹²⁹Ce have been populated via heavy-ion fusion evaporation reaction ⁹⁶Mo (³⁷Cl, 1p3n) ¹²⁹Ce. The γ-γ coincidence and intensity balance used to measure the B(M1; I→I-1)/B(E2; I→I-2) (the probability ratio of the dipole and quadrupole transition) in ν7/2[523] rotational band of ¹²⁹Ce. And the energy splitting (Δe′) has been got through the experimental Routhians. The lifetimes and quadrupole moments Q_t have been extracted from the lineshape analyses using DSAM. The deformation of the ν7/2[523] rotational band of ¹²⁹Ce was extracted from the Q_t and moment of inertia J_RR.     

因瓦合金纳米微粉的恒磁导率及其压力、频率特性和压力相变

 以Fe-30wt%Ni合金片为母合金，用蒸发冷凝法制备了三种粗细不同的纳米微粒。经透射电镜和X光衍射物相分析，微粒成分与母合金一致。5T、5H和3K粉的平均粒度分别为13.6、27和40 mm。在室温和43~28个不同的流体静压力（0.000 1~2.205 GPa）下测量了它们的磁化曲线、磁导率曲线和起始磁化曲线。结果表明：（1）在H＝(20－132)(1000/4π)A/m范围内Fe-30Ni合金三种纳米粉均具有恒磁导率。（2）三种纳米粉恒磁导率随静水压的变化规律如下：μ_r＝3.83+0.253p-0.022 1p²-0.007 22p³（5T粉）；μ_r＝3.93+1.20p-1.97p²+1.52p³-0.510p⁴+0.059 9p⁵（5H粉）；μ_r＝5.96-0.276p+0.107p²-0.045 9p³（3K粉）。前两者随压力增加而升高。后者随压力增加而下降。（3）γ-α马氏体相变明显存在于5T、5H粉中，而3K粉中未见到。（4）Fe-30Ni合金片的μ_i从200kHz至2 MHz已下降一个数量级，而其纳米粉μ_i的频率范围高于300 MHz，增大两个数量级以上。     

π-J/ψ correlation and elliptic flow parameter v2 of charmed mesons at RHIC energy

We study the correlation between the trigger π and the associated J/ψ on near and away sides in Au+Au collisions at √s_NN=200 GeV. In the region of trigger momentum p_t>4 GeV/c, the π spectrum is composed of thermal-shower and shower-shower recombinations in the frame work of the recombination model. We consider the azimuthal anisotropy in the quenched hard parton distribution and then calculate the elliptic flow parameter v₂ of charmed mesons (J/ψ, D⁰ and D_s) for different centralities.     

微光高速电影摄影

低照度、低对比下的高速摄影不断增长的需要促进了新型摄影系统的发展,其中在镜头与高速运动胶片之间加入象增强器所构成的微光高速摄影可使摄影的灵敏度有显著的提高。它具有高光增益、高成家质量的优点。同时由于高速电子快门取代了机械快门,使此类摄影系统面目一新。由于高的光增益,使此摄影系统的信息记录能力大大增加,高速摄影的信息量I为: I=PFn²[log₂(1+SN)]g^2/3其中g=t_p/t_e((时间间隔)(曝光时间))当采用微光高速电影摄影时,它的信息量Γ为: Γ=PFn′²[log₂(1+S/N)](Gg)^2/3 I′/I=(n′/n)²G^2/3G通常为5×10到10⁴倍本章讨论了微光高速摄影系统中主要器件和主要技术。介绍了国外此摄影系统的发展水平与动向以及我国的应用前景。     

Triaxial shape in 129Ce

The high spin states of ¹²⁹Ce have been populated via heavy-ion fusion evaporation reaction ⁹⁶Mo (³⁷Cl, 1p3n) ¹²⁹Ce. The comparison between the signature- and B(M1)-staggering defined by Hagemann and Hamamoto have been showed in the negative-parity band of ¹²⁹Ce. The lifetimes and quadrupole moments Q_t of the high spin states of ¹²⁹Ce have been extracted from the line shape analyses using Doppler shift attenuation method (DSAM). The deformation parameters extracted through the solution of equations for quadrupole transition moments Q_t and collective moments of inertia J_RR.     

低密度硅橡胶冲击雨贡纽曲线测量

 采用阻抗匹配法测量了两种低密度（ρ₀＝0.45 g/cm³和ρ₀＝0.47 g/cm³）硅橡胶在2.5~15 GPa压力范围内的冲击雨贡纽参数，p-u_p和u_s-u_p曲线，并采用最小二乘法拟合出C₀，λ′和λ″的值。实验结果与理论预估值符合较好。     

双包层掺Yb3+光纤环形脉冲激光形成研究

对采用环形腔结构,由偏振敏感的光隔离器构成超短脉冲掺Yb³⁺光纤激光器输出的动力学特性进行了数值模拟.模拟表明:在没有进行色散补偿的掺Yb³⁺光纤环形激光器中,采用非线性偏振旋转的附加脉冲锁模技术,通过改变偏振控制器的方向,可以使激光器工作在不同的区域.实验用976 nm的半导体激光器作为泵浦源,通过调整偏振控制器,实验观测到掺Yb³⁺环形激光器工作在稳态和自脉动状态,其脉动的周期由光纤激光器腔长决定.     

First Principles Study of Aluminium Vacancy in Wurtzite Aluminium Nitride

We report that the aluminium vacancy in wurtzite AlN brings about two impurity levels e and a₂ in the band gap, not just one single t₂ level. The aluminium vacancy carries a magnetic moment of 1μ_B in the ground state. The molecule orbit of the aluminium vacancy becomes e^↑↑a₂^↓ rather than e^↑↑a₂^↓. The calculation is carried out by using the CASTEP code. The intrinsic symmetry of wurtzite AlN is the driving force for this spin splitting. Finally the symmetry of wurtzite AlN results in an anti-ferromagnetic coupling between the aluminium vacancies, as is predicted. Our findings are helpful to gain a more through understanding of the structural and spin property of aluminium vacancy in wurtzite AlN.     

核电荷半径的壳(形变)效应

实验证据分析表明: 大变形区的核电荷方均根半径常数r_p无例外地比相邻球形核大一些. 这可以用形变效应来说明. 中子数在下列壳层中1p_3/2(N~3—6), 1d_5/2(N~9—14), 1f_7/2(N~20—28), 1g_9/2(N~40—50), 1h_11/2(N~70—82)的各同位素的电荷半径的变化(随A的增大半径反而变小等)与A^1/3律完全抵触. 在Z^1/3律基础上, 考虑形变效应后可给予较好的说明.