用多步激发技术测定锶的(5p3/2ns)1及(5p3/2nd)3自电离谱

用分步激发方法及偏振光技术,测定了锶的(5p_3/2ns)₁(n=13-21)及(5p_3/2 nd)₃(n=13-24)各自电离谱,在低于5p_1/2电离限的(5p_3/2ns)₁态的实电子激发谱中,出现对应于(5p_1/2ns)₁及(5p_1/2nd)₁的畸变峰,畸变峰也出现于(5p_3/2nd)₃的实电子激发谱中。这说明(5p_jns)(5p_jnd)自电离系列间存在相互作用。 关键词：     

Sr(5p1/2nd)3自电离谱的测定

用分步激发技术测得了Sr(5p_1/2nd)₃系列(n=11—24)自电离能级的位置及其有效量子数ν_1/2。对其与(5p_3/2nd)₃,系列间可能存在的组态相互作用,进行了初步探讨。 关键词：     

Ba原子6pnd(J=1, 3)自电离光谱的实验研究

采用三台可调谐激光实施孤立实激发,分三步将处于基态的Ba原子激发到6p_1/2nd(J=1,3)和6p_3/2nd(J=1,3)自电离态上,获得了分别从6snd¹D₂(n=7—15)和6snd³D₂(n=7—12) 激发而得到的6p_1/2nd(J=1,3)和6p_3/2nd (J=1,3)自电离光谱,重点对主量子数n较低的自电离态进行了实验研究. 通过光谱的线形拟合得到了上述能级的位置和宽度等数据,进而获得了量子亏损和约化宽度等信息. 通过对不同系列的自电离光谱的分析和比较,详细讨论了这些自电离态的光谱特征及其复杂光谱结构的成因. 关键词： 孤立实激发 组态相互作用 自电离态     

π凝聚态中的弱过程对中子星振动的阻尼效应

本文主要讨论了中子星内部发生从正常中子物态到π凝聚物态相变所产生的星体振动的阻尼,由弱作用反应u(p₁)→u(p₂)+e^-+v_e和u(p₁)+e^-→u(p₂)+v_e算出振动阻尼时标,并考虑了中子星内部的热演化。 关键词：     

外延Si1-xGex薄层中浅杂质的光热电离光谱

在Si_1-xGe_x合金外延层中利用光热电离光谱方法观察到了Si_0.92Ge_0.08合金中浅施主磷的2p_±及3p_±态的分立谱线，并根据有效质量近似理论估算了Si_0.92Ge_0.08合金中磷施主的电离能为45.51meV．与硅相比，由于合金的无序效应，Si_1-xGe_x合金的分立谱线发生明显展宽 关键词：     

W65+—W71+离子2s1/2—2p3/2电子碰撞激发过程及相应辐射跃迁谱线极化度的理论研究

利用基于多组态Dirac-Fock理论方法的原子结构及性质计算程序GRASP92,详细研究了类氟W⁶⁵⁺到类锂W⁷¹⁺离子的2p_38/2—2s_1/2跃迁性质.计算结果与Podpaly等[Phys.Rev.A 80 052504（2009）]的实验结果符合得非常好.在此基础上,利用全相对论扭曲波方法研究了2s_1/2—2p_1/2的电子碰撞激发总截面和磁子能级碰撞激发截面以及部分谱线的线性极化度,分析了电子碰撞激发截面和谱线线性极化度随碰撞能量的变化规律.     

等离子体屏蔽效应对原子能级和振子强度的影响

利用Debye模型,研究了等离子体屏蔽效应对热等离子体中原子能级和振子强度的影响.通过在MCDF模型中引入等离子体屏蔽效应,计算了MnXXII-BrXXII等11个类Be离子在等离子体环境下2s²—［2s_1/2,2p_1/2］₁和2s²—［2s_1/2,2p_3/2］₁跃迁的能级和振子强度.计算结果表明,等离子体屏蔽效应使得类Be离子2s²—［2s_1/2,2p_1/2］₁跃迁的激发能量增大,从而导致谱线蓝移现象;并且随着屏蔽效应的不断增强,蓝移的程度会逐渐加大.屏蔽效应对于2s²—［2s_1/2,2p_3/2］₁跃迁的振子强度也有类似的影响. 关键词： Debye 等离子体屏蔽 跃迁能级 振子强度     

Sr原子5p_(1/2)ns系列自电离谱的观察和测定

本文报道了用孤立实激发的方法,对Sr的5p_(1/2)ns系列自电离谱的观察。测定了Sr的5p_(1/2)ns系列八个态的能级、量子亏损和线宽。     

机械合金化La0.7Ca0.3MnO3的晶化动力学及磁电阻研究

通过机械合金化方法制备了单相La_0.7Ca_0.3MnO₃化合物.球磨形成的非晶态结构在920K退火时转变为钙钛矿型相结构.根据质量作用定律,讨论了非晶晶化动力学行为,其晶化转变激活能约为265kJ/mol.同时研究了化合物的电阻特性,发现低温下样品的电阻ρ与温度T的关系为ρ∝T²,随退火温度的升高,ρ-T²曲线斜率下降.在远离居里温度处的低温磁电阻可用Δρ/ρ₀=p₁-p₂T^3/2-p₃T描述. 关键词：     

类锂离子双电子复合过程中辐射光子角分布和极化特性的理论研究

基于多组态Dirac-Fock 方法和密度矩阵理论,本文详细计算了高电荷态类锂离子（26 ≤ Z ≤ 92）KLL 双电子复合过程中,自由电子被共振俘获到中间双激发态1s2s²2p_3/2J = 1 的磁子能级截面以及该双激发态的取向参数,进而得到了此激发态向基态电偶极辐射跃迁1s2s²2p_3/2J = 1→1s²2s²J = 0 所发出光子的角分布和极化度,重点讨论了Breit 相互作用对相关物理量的影响. 研究表明,Breit 相互作用极大地改变了中间双激发态1s2s²2p_3/2J = 1 不同磁子能级的截面,从而导致了随后退激发放出光子的角分布和极化特性的显著变化. 关键词： 角分布和极化特性 多组态Dirac-Fock方法 密度矩阵理论     

Nuclear ground state spins of short-lived strontium isotopes

Nuclear ground state spins of the odd-mass strontium isotopes between A=79 and 97 were determined by measurements of the hyperfine structure in the ionic transition 5s²S_1/2?5p²P_3/2. The spins of⁹³Sr and⁹⁷Sr are revised to I=5/2 and I=1/2, respectively, while assignments for the remaining isotopes are confirmed.     

Hyperfine interactions in the alkaline-earth Sr ions by collinear fast beam laser spectroscopy

The magnetic dipole hyperfine structure constants of the⁸⁷SrII 5s²S_1/2 ground state and the 5p²P_1/2 excited state, and the isotope shifts of the ionic 5s²S_1/2 → 5p²P_1/2 resonance transition for all stable Sr isotopes, measured by collinear fast beam laser spectroscopy, are reported.     

Discovery of a very low-lying 0+ state in 98Sr and shape coexistence implication in 98Sr

Using the on-line mass separator OSTIS for studies of short-lived fission products, we found two modes for the β-decay of ⁹⁸Rb with respective half-lives of 96 and 114 ms. The latter decay populates a 0⁺ state in ⁹⁸Sr at the unusually low energy of 215.5 keV, which is by far the lowest 0⁺ excited state observed in even-even nuclei. The half-lives of the 0⁺ and the 2₁⁺ states in ⁹⁸Sr were found to be respectively 25 ns and 4 ns. The transition probabilities, the reduced E0 matrix element and the observed level structure suggest shape coexistence for ⁹⁸Sr: the spheroidal 0₁⁺ ground state shows a rotational band with the 2⁺, 4⁺, (6⁺) levels, whereas the presumably spherical 0₂⁺ excited state may be connected with the 2⁺ level of a vibrational band. A simple model is proposed.     

Lifetime measurements in99Sr and100Zr

The lifetime of the first excited state in⁹⁹Sr has been determined by the delayed γ-γ coincidence method. The value of t_/2=0.58(9) ns corresponds to a deformation parameter ß=0.38(4). The deduced z> value confirms the previously proposed ν[411]3/2 Nilsson assignment for the⁹⁹Sr ground state. In addition, lifetime values for the 2⁺ (t_1/2=0.40(8) ns) and 0⁺ (t_1/2=5.36(23) ns) states in¹⁰⁰Zr are obtained, which deviate from older measurements and indicate a larger deformation of ß=0.39(4).     

Radiative lifetimes and collisional quenching cross sections of selectively excited vibrational states of the B 2p1Σu+ state of H2

Radiative lifetimes between 0.54 ns and 0.69 ns have been measured for the vibrational levels υ′ = 0...4 of the B 2p¹Σ_u⁺ state of H₂ after selective excitation by synchroton radiation. Quenching by collisions with H₂ ground state molecules has been observed with cross sections of 5 × 10^-15 cm².     

Radiative Lifetimes of Some 5d10n2F and 5d10n2P Levels of Hg+

Radiative lifetimes of 8p²P_3/1 (15.3 ns) and nf²F (7f²F_5/2 - 24.7 m. 7f²F_7/2 - 5.5 ns, 8f²F_7/2 - 48.5 ns, 8f²F_5/2 - 47.0 ns) levels of Hg⁺ have been measured employing delayed coincidence method. The dependencies of radiative lifetimes vs effective principal quantum number for np²P_3/2 and np²F_7/2 series are non linear.     

Decay properties of the 19/2− isomers in113,117Sb

By means of the generalized centroid-shift method, the following half-lives were determined:T _1/2(3045 keV)=3.7±0.3 ns in¹¹³Sb using the reaction¹⁰⁴Pd(¹²C,p2n) as well asT _1/2 (1322.8 keV)=3.5±0.3 ns,T _1/2(2779.8 keV) =0.50±0.15ns,T _1/2(2874.9 keV)<0.2 ns andT _1/2(3072.9 keV)<0.1 ns in¹¹⁷Sb using the¹¹⁶In(α, 2n) reaction. Three-quasiparticle configurations of the type πd _5/2ν(h_11/2 d _3/2) in^113,117Sb are found to dominate in the wave functions of the 19/2^? states at 3045 and 2780 keV in¹¹³Sb and¹¹⁷Sb, respectively. TheB(E2, 19/2^? → 15/2^?) values in^113–119Sb are discussed.