Ground state hyperfine structure of95Mo and97Mo

The hyperfine structure of the ground state 4d ⁵ 5s ⁷ S ₃ of⁹⁵Mo and⁹⁷Mo has been measured by the atomic beam magnetic resonance technique with the following results:⁹⁵Mo:A=?208.582060(10)MHz,B=37.050 (100) kHzC=?30 (10) Hz,D=?3 (3) Hz⁹⁷Mo:A=? 212.980930 (10) MHz,B?69.990(140)kHzC=?5 (10) Hz,D=0 (3) Hz. After application of corrections calculated according to second order perturbation theory, the hyperfine structure constants became:⁹⁵Mo: A_c=?208.582560(290)MHz,B _c =16.920(4300)kHzC _c=?30(270) Hz,D _c =? 3 (50) Hz⁹⁷Mo: A_c=212.981450(300) MHz,B _c =?90.780(4400)kHzC _c=?6(270) Hz,D _c =0 (50) Hz. With the known ratio ofg _I(⁹⁵Mo)/g _I(⁹⁷Mo) [1] a calculation of the hyperfine anomaly yields:₉₅ Δ ₉₇=?0.01009(17)%. The ratio of the uncorrectedB factors isB(⁹⁷Mo)/B(⁹⁵Mo)=?1.8890(47). Because of the relatively large effects of second order hyperfine structure, the ratio of the correctedBfactors differs considerably from the ratio of the uncorrectedB factors. From the correctedB factors the electric quadrupole moments may be evaluated by means of calculated radial integrals [2]. The results are:Q (⁹⁵Mo)=?0.019(12)barns,Q(⁹⁷Mo)=0.102(39)barns.     

94Mo高自旋态能级纲图

通过重离子融合蒸发反应^16O(^82Se 4n)^94Mo布局了^94Mo核的高自旋态．利用多探头探测器阵列GASP进行了在束γ测量，从而重新研究了^94Mo核的高自旋态能级结构．基于新发现的一些重要的连接跃迁，对^94Mo核的高自旋态能级纲图做了重要修改．将新的能级结构与壳模型计算进行了比较和讨论．结果表明要正确的描述^94Mo核的高自旋态(自旋值大于14)能级结构，应考虑价中子在d5／2，g7／2和h11/2轨道上的激发．     

Level structure of78Rb

The excited states of⁷⁸Rb have been investigated by means of in-beam andβ-γ spectroscopy. The production of⁷⁸Rb and theβ radioactivity of⁷⁸Sr have been made through the⁵⁴Fe(²⁸Si,3pn) and⁵⁴Fe(²⁸Si,2p2n) reactions, respectively. Four rotational bands have been observed in the high-spin band structure. The signature splitting is large in the two bands, while the other two bands have small splitting. A detailed low-lying level scheme of⁷⁸Rb has been constructed for the first time via theβ decay of⁷⁸Sr in order to search for a linking transition between the high-spin band head and low lying states.     

Level structure of 76As

The energy-level structure of ⁷⁶As has been studied by the ⁷⁵As(d, p) reaction with 12.0 MeV incident deuterons. Eighty-seven excited energy levels up to 2.5 MeV have been identified. The angular distributions for thirty-nine of the observed transitions are compared with distorted-wave Born approximation calculations. Angular momentum transfers are determined and spectroscopic strengths are deduced from the data. The results are compared with shell-model sum rules and with (d, p) results on N = 42 isotones. Possible spin values are assigned for some of the levels based on the present results, (n, γ), (p, n) and (p, nγ) studies.     

Level structure of 159Lu

The high-spin states of 159Lu were populated by fusion-evaporation reaction 144Sm (19F, 4n) with beam energy 106 MeV. A new level scheme was established, which consists of the yrast band with negative parity, the octupole vibration band based on the states and quasipartical band with positive parity. The high spin states of 159Lu were discussed by systemic characteristics.     

Level structure of 146Tb

The level structure of the doubly odd nucleus ¹⁴⁶Tb has been studied via the ¹¹⁸Sn(³²S, 1p3n) reaction using techniques of in-beam -ray spectroscopy. Measurements of -ray anisotropies, X- and - -t coincidences were performed with 12 BGO(AC)HPGe detectors. Based on the measured results, the level scheme of ¹⁴⁶Tb has been revised significantly and extended up to an excitation energy of 8.39 MeV. The level structure has been interpreted qualitatively by coupling an h _11/2 proton-particle and an h _11/2 neutron-hole to the excited states in the ¹⁴⁶Gd core.Received: 3 July 2003, Published online: 26 November 2003PACS: 23.20.Lv transitions and level energies - 27.60. + j      

Proton-neutron structure of collective excitations in 94Mo

Due to the recent development of radioactive beam production, various direct reaction studies in reversed kinematics have been made to investigate the behavior of the N = 20 shell closure in the neutron-rich region. Coulomb excitation, proton inelastic scattering, and fragmentation of unstable nuclei have been studied with γ-ray detection. Received: 21 March 2002 / Accepted: 16 May 2002 / Published online: 31 October 2002 RID="a" ID="a"e-mail: motobaya@rikkyo.ne.jp     

Level structure in 213Bi

By performing α?γ-coincidence measurements, more precise data on the weak ²¹⁷At α-decay to excited levels of ²¹³Bi have been obtained. A new branch of the α-decay (0.005% per decay) to the 758.9 keV ²¹³Bi level is observed. The structure of the proposed ²¹³Bi levels (0.0 keV 9/2^?, 257.9 keV 7/2^?, 593.1 keV (5/2–9/2)^? and 758.9 keV (5/2–13/2)^?) is discussed in the framework of the shell model.     

The structure and magnetic crystallographic anisotropy of PrFe10.5Mo1.5 and PrFe10.5Mo1.5Nx

Neutron powder diffraction studies indicate that PrFe_10.5Mo_1.5N_x retains the ThMn₁₂-type structure, and nitrogen atoms occupy the interstitial 2b sites. According to the structure parameters, the crystal-field coefficients of Pr³⁺ in the PrFe_10.5Mo_1.5 compounds and their nitrides were calculated using the single-ion model. The results show that upon nitrogenation the easy magnetization direction of PrFe_10.5Mo_1.5 changes from easy plane to easy axis. As a preliminary attempt, magnetic powders based on PrFe_10.5Mo_1.5N_x were obtained with a maximum energy product of 16.6 MGOe at room temperature.     

The valence band structure of V−Mo solid solutions

The electronic structure of V _x Mo_1–x (x=0.2; 0.4; 0.6; 0.75) solid solutions was studied by XPS and UPS. The density of states at the Fermi energy,N(E _F), deduced from these measurements, shows a minimum as a function of the alloy concentration on the Mo rich side. This behaviour can be explained by band structure calculations and is in good agreement with previous NMR measurements. The relation between the electronic structure at the Fermi level and the superconducting properties is discussed. The band structure of the Mo rich alloys can be understood in terms of a rigid band model.     

Level structure of doubly odd154Ho

¹⁵⁴Ho was studied via¹⁴¹Pr(¹⁶O,3n) reaction at beam energy of 75 MeV. We found two new rotationally aligned bands made of neutron h_9/2 and f_7/2 orbitals coupled to a proton h_11/2 orbital. As with several new high-spin states, up to I=20, the ground state band with odd parity starts to show anomalous signature splitting at I=13 in this doubly odd¹⁵⁴Ho. The observed rotational bands in¹⁵⁴Ho are quite consistent with the onset of collectivity which appears in general at neutron number of 87 in neutron-deficient rare-earth nuclei.     

Magnetic structure of ErCo10Mo2 and TbCo10Mo2 determined by time-of-flight neutron powder diffraction

The crystal and magnetic structures of tetragonal compounds ErCo₁₀Mo₂ and TbCo₁₀Mo₂ (space group I₄/mmm) have been investigated by time-of-flight neutron powder diffraction at 5 K. The compound ErCo₁₀Mo₂ is planar at 5 K whilst TbCo₁₀Mo₂ remains axial even at low temperatures. The magnetic moments of the three Co sublattices have been determined, with moments of 1.0(0.2)μ _B , 0.8(0.2)μ _B and 0.8(0.2)μ _B for 8i, 8j and 8f sites respectively. The Er and Tb moments are reduced by approximately 7% from their free-ion values by the action of the tetragonal crystal field.     

LEED analysis of the surface structure of Mo(001)

A detailed comparison between theoretical and experimental LEED data for the Mo(001) surface, using the quantitative r-factor method of Zanazzi and Jona, yields a value for the surface layer contraction of 9.5 ± 2.0%, consistent with the 11.5% found previously by Ignatiev et al. Non-structural parameters are also in agreement, although the surface Debye temperature, 230 K, is slightly higher than found before. r-Factors were used to investigate the effects of all the parameters, and show that an energy-dependent inner potential gives better agreement than a fixed value and that the second layer is contracted by about 1% of the bulk layer spacing. The effect of using different ion core potentials is examined and discussed. A superposition potential which models the surface ion environment is found to have a significant effect on the layer displacement concluded.     

高度离化的钼离子细致结构能谱测量

高度离化的中、高z元素激光等离子体辐射的细致结构能谱对惯性约束聚变等离子体诊断和原子结构理论计算等方面非常有用．在“神光Ⅱ”激光装置上，聚焦0．35μm激光束于真空室内的钼（Mo）元素固体靶上，产生Mo激光等离子体，用高分辨椭圆弯晶谱仪测量Mo激光等离子体辐射在0．32-0．58nm范围内的X射线细致结构能谱，并对实测能谱进行辨识和归类．辨识出了n=4—2，3—2系列离子共振跃迁和内壳层跃迁的能谱线，还有类氢、类氦离子共振线及伴线．另外，对谱线的半高全宽度（FWHM）值做了分析．在整个测量范围内，谱线精确波长值的绝对误差小于0．0005nm，与HFR方法得到的理论计算结果值比较，两者符合较好．此工作的结果对积累Mo元素离子谱线数据具有重要的意义．     

Identification and structure of high spin particle-hole states in89Mo

Particle-γ andγ-coincidences of the reaction⁵⁸Ni(³⁶Ar, 4pn)⁸⁹Mo have been used to gain more information about high spin states in⁸⁹Mo and to establish the yrast sequence up to 7.6 MeV excitation energy and probable spin 37/2 ?. Spins and parities were assigned on the basis of DCO-ratios measured with the OSIRIS spectrometer and a large volume Ge detector placed at 162° to the beam. Furthermore, aγ-ray angular distribution experiment was carried out using the reaction⁵⁸Ni(³⁵Cl, 3pn)⁸⁹Mo. As in the neighboring isotopes⁸⁸Mo and⁹⁰Mo, the positive-parity high-spin states can be grouped into shell model multiplets characterized by increasing seniorities of proton particles and neutron holes in the 1g_9/2 shell. The negative-parity states can be explained with one nucleon moving in thep _1/2 orbit. The energies and wave functions of these states have been deduced by means of the shell model code RITSSCHIL. The 2584 keV (21/2⁺) is an isomeric state the mean life of which has been estimated from delayedγγ-coincidences.