共查询到19条相似文献,搜索用时 546 毫秒
1.
电子原子散射中的S,T,U参数可用来描述散射前后自旋状态的变化,研究精细结构水平上的散射激发振幅之间的关系,进而揭示电子原子碰撞过程中电子自旋-轨道耦合以及电子-电子交换等自旋相关效应.采用扭曲波玻恩近似计算了钠原子受电子散射S→P跃迁中的S,T,U参数,分析了多种入射能(2.2-60 eV)的电子与钠原子激发S→P跃迁过程的S,T,U参数随散射角的分布,其中对10 eV入射能的Sp参数与已报道实验数据符合一致.结果表明,较低能电子入射下的S,T,U参数随散射角的分布幅度和起伏都比较明显,入射能大于40 eV的电子入射,S,T,U参数的散射角分布变化很小. 相似文献
2.
基于微分的思想,结合经典的双原子分子跃迁谱线表达式,提出了预言双原子分子P线系高激发振-转跃迁谱线的新解析物理公式.对于某分子电子体系的某一P支跃迁带,利用实验上获得的一组(15条)精确的跃迁谱线和该跃迁带对应的上下振动态的转动常数(Bυ',Bυ″)的精确数据,该公式不仅可以精确地重复已知的实验跃迁谱线,而且还能预测出实验上难以获得的更高激发态的跃迁谱线数据.利用该公式,研究了CO分子电子基态的(2,0)振-转跃迁带的<
关键词:
双原子分子
发射光谱
P线系')" href="#">P线系
CO 相似文献
3.
本文在孙卫国等建立的预测双原子分子高转动激发态的 振转跃迁能谱的解析物理公式的基础上, 增加了该公式推导时被省略的高阶转动项Hv对能级的贡献, 获得了包含此高阶小项的预测双核体系高转动激发态的振转跃迁谱线的新表达式. 使用该新公式对AuO分子P支发射跃迁光谱的研究表明: 加入高阶转动常数Hv后的新公式所预言的振转跃迁 谱线的精度比不包含Hv 的公式给出的结果提高了约一个数量级. 因此, 更加有力地表明了使用多重差分法建立的这类物理公式在预言实 验未给出的物理数据方面的正确性和有效性.
关键词:
AuO
Hv')" href="#">转动常数Hv
P支谱线')" href="#">P支谱线
多重差分法 相似文献
4.
基于第一性原理全势线性缀加平面波方法和局域密度近似(LDA),对ReSi1.75的基态晶格属性进行了研究. 结构优化的结果表明,ReSi1.75的基态平衡晶格常数比实验值小约0.6%. 在LDA计算基础上,考虑局域的Re的d电子库仑作用,用LDA+U方法计算了ReSi1.75的电子结构,发现当Ueff=U-J=4.4eV时,能带结构呈半导体性质. 具有0.12eV
关键词:
1.75')" href="#">ReSi1.75
局域密度近似
自相互修正作用
电子结构 相似文献
5.
聚集速率是评估胶体体系特性及稳定性的关键参数, 静态光散射和动态光散射则是测量聚集速率的两个重要方法. 然而, 用静态光散射和动态光散射测量聚集速率时, 需要知道有关单粒子和双粒子聚集体光散射特性的数据. 为此, 通常需要把动、静两种方法结合, 才能消去这个数据. 以前各种近似理论曾用来解决这个问题, 但因粒子尺寸和形状的限制, 结果并不理想. 而T矩阵方法可以不受粒子大小和形状的限制计算其光散射特性. 本工作用T矩阵方法直接计算静态光散射和动态光散射所必须的粒子散射特性, 并将该法得到的聚集速率与动静态光散射结合法得到的聚集速率进行了比较, 两者结果很接近. 本工作为简化静态光散射和动态光散射测量聚集速率, 扩展其应用范围开辟了新途径.
关键词:
T矩阵')" href="#">T矩阵
光散射法
聚集速率 相似文献
6.
7.
8.
采用完全对角化方法,以尖晶石结构的ZnAl2O4:Cr3+,ZnGa2O4:Cr3+和MgAl2O4:Cr3+系列晶体为例,联系晶格局域结构,对三角对称下3d3离子2E态g因子性质进行了研究.研究中考虑了包括自旋与自旋相互作用、自旋与另一轨
关键词:
2E态g因子')" href="#">2E态g因子
3离子')" href="#">3d3离子
尖晶石结构
磁相互作用 相似文献
9.
用HFR波函数对低密度类氢Ni27+等离子体与电子相互作用的KLn和KMn共振激发的双电子复合过程进行了细致的理论计算研究.根据可能的重要辐射衰变通道,分析了Ni27+等离子体Kα 型和Kβ 型辐射衰变的双电子复合速率系数随旁观电子主量子数n和轨道角动量量子数l与电子温度的变化行为,计算了Ni27+等离子体双电子复合过程的总速率系数.研究结果表明,在低密度条件下,Kα 型和Kβ型辐射衰变的分支双电子复合速率系数与旁观电子主量子数n和轨道角动量量子数l有重要关系,前者的分支速率系数远大于后者.
关键词:
27+离子')" href="#">Ni27+离子
Kα型和Kβ型辐射衰变')" href="#">Kα型和Kβ型辐射衰变
双电子复合
速率系数 相似文献
10.
采用密度泛函理论中的广义梯度近似(GGA)对CoBen(n=1—12)团簇的几何构型进行优化,并对能量、频率和磁性进行了计算,同时考虑了电子的自旋多重度.得到了CoBen(n=1—12)团簇最低能量结构的自旋多重度是2和4.在CoBen(n=1—12)团簇中,Co原子的磁矩出现了奇偶振荡,当n=6时,Co原子的4s,3d和Be原子的2s,2p较强杂化、Co-Be键长的减小以及对称性的降低导致Co原子的磁矩最小.通过对CoBen(n=1—12)团簇电子性质的分析,得出了掺杂可以增强团簇稳定性和有利于增加合金化学活性的结论.n=5,10是团簇的幻数.
关键词:
n团簇')" href="#">CoBen团簇
自旋多重度
磁矩
电子性质 相似文献
11.
Precise measurement of magnetic moment of short-lived β-emitting nuclei12B ( I π=1+, T 1/2=20.18 ms)
Zhou Dongmei Zheng Yongnan Du Enpeng Xu Yongjun Zhu Jiazheng Yuan Daqing Wang Zhiqiang Luo Hailong Zuo Yi Ma Ruigang Duan Xiao M. Mihara M. Fukuda K. Matsuta T. Minamisono Zhu Shengyun 《中国科学G辑(英文版)》2004,47(5):531-539
The spin polarized β-emitting nuclei12B (I
π=1+,T
1/2=20.18 ms) were produced by the nuclear reaction11B(d, p)12B and by the selection technique of the incident deuteron energy and the12B recoil angle following the nuclear reaction. The nuclear magnetic moment of the short-lived nuclei12B was measured by β-NMR with the β-NMR and β-NQR setup established for the first time in China. The nuclear magnetic moment
of12B was determined to be μ=0.99993±0.00048 nm org=0.99993±0.00048 after the precise correction of the Knight shift. 相似文献
12.
T. Tamae T. Hino H. Kawahara M. Nomura M. Sugawara A. Tanaka T. Tanaka H. Tsubota T. Yokokawa T. K. Yoshida 《Nuclear Physics A》2001,690(4):789
Proton energy spectra of the 197Au(e,p) reaction were measured in the region between 17 and 30 MeV at three angles: 40°, 90° and 140°. Two prominent bumps were observed in the (γ,p) spectra converted using virtual photon theory. The higher-energy bump shifts with photon energies and the lower-energy one stays at 10.5 MeV. The higher-energy bump is much larger at 40° than at 140°; on the contrary the angular dependence of the lower-energy bump is small. Neither bump can be described by a statistical calculation. A calculation of a microscopic shell model shows that the lower-energy bump is attributed to the decay of proton-particle–neutron-hole pairs in the T> states, leaving a neutron hole around the Fermi surface. The higher-energy bump can be ascribed to the direct–semidirect mechanism. This paper gives the solution to a part of the long-standing question about the origin of photo-proton emission in heavy nuclei. 相似文献
13.
14.
使用密耦近似(Close-Coupling)方法、采用Tang-Toennies势模型计算了惰性气体原子Ne与H2分子及同位素D2分子在碰撞能量为83.8 meV时的微分散射截面及分波截面, 并与实验值和文献值进行比较.计算得到的微分散射截面值与实验值符合得较好,分波截面值与文献值也相符合.使用同样的方法和模型,文中对Ne-H2(D2,T2)三个体系的微分截面和分波截面进行了系统计算和比较分析,得出对称同位素替代碰撞体系的散射截面规律. 相似文献
15.
The structural degradation of thermal SiO2 on (100)Si under isochronal post oxidation vacuum annealing (POVA) has been probed by electron spin resonance (ESR). The degradation process, studied in the range Tan = 950–1250 °C, is established as intense point defect generation including E′γ, E′δ, EX and the elusive predominant degradation center S. Thermally activated generation is revealed over broad Tan ranges for the two most populous defects, S and E′γ, with a common activation energy ~1.6eV. Depth profiling after heating at 1200°C shows that the S centers predominantly reside near the oxide borders, generally in anticorrelation with the E′γ distribution. The S center susceptibility has been inferred from conventional ESR signal intensity monitoring as well as from revealed anisotropic demagnetisation effects. It is found Curie-Weiss type with critical temperature of ~ 1.3 K. Newly observed weak hyperfine structure may comply with the S center being an E′-like defect. 相似文献
16.
针对NiS2-xSex系统在x=1.00附近发生的反铁磁量子相变,制备了一系列NiS2-xSex(x=0.96, 0.98, 1.00, 1.05, 1.10和1.20)多晶样品,对其结构、磁性质和电阻率进行了系统的观测.结果发现:样品磁化率-温度关系呈现典型的强关联电子系统特征;与铜氧化物超导体相类似,它们的电阻率-温度关系在很宽的温
关键词:
量子相变
反铁磁自旋涨落
2-xSex体系')" href="#">NiS2-xSex体系 相似文献
17.
18.
Y.-Y. Hu K. Schmidt-Rohr 《Journal of magnetic resonance (San Diego, Calif. : 1997)》2009,197(2):193-207
In experiments on S–L heteronuclear spin systems with evolution of the S-spin magnetization under the influence of a quadrupolar nucleus (L-spin), effects of longitudinal quadrupolar (T1Q) relaxation of the L-spin coherence on the sub-millisecond time scale have been documented and explored, and methods for minimizing their effect have been demonstrated. The longitudinal relaxation results in heteronuclear dephasing even in the reference signal S0 of S{L} REDOR, REAPDOR, RIDER, or SPIDER experiments, due to T1Q-relaxation of the transiently generated SyLz coherence, reducing or even eliminating the observable dephasing ΔS. Pulse sequences for measuring an improved reference signal S00 with minimal heteronuclear recoupling but the same number of pulses as for S0 and S have been demonstrated. From the observed intensity ΔS0 = S00 − S0 and the SPIDER signal ΔS/S0, T1Q can be estimated. Accelerated decays analogous to the dipolar S0 curves will occur in T2 measurements for J-coupled S–L spin pairs. Even in the absence of recoupling pulses, fast T1Q relaxation of the unobserved nucleus shortens the transverse relaxation time T2S,MAS of the observed nucleus, in particular at low spinning frequencies, due to unavoidable heteronuclear dipolar evolution during a rotation period. The observed spinning-frequency dependence of T2S,MAS matches the theoretical prediction and may be used to estimate T1Q. The effects are demonstrated on several 13C{14N} spin systems, including an arginine derivative, the natural N-acetylated polysaccharide chitin, and a model peptide, (POG)10. 相似文献