Ground-state magnetic moment of the T=1 nucleus 32Cl using on-line β-NMR spectroscopy

2000 ◽  
Vol 62 (4) ◽  
Author(s):  
W. Rogers ◽  
G. Georgiev ◽  
G. Neyens ◽  
D. Borremans ◽  
N. Coulier ◽  
...  
1999 ◽  
Vol 451 (1-2) ◽  
pp. 11-18 ◽  
Author(s):  
H. Ogawa ◽  
K. Asahi ◽  
K. Sakai ◽  
A. Yoshimi ◽  
M. Tsuda ◽  
...  

1992 ◽  
Vol 30 (4) ◽  
pp. 347-358 ◽  
Author(s):  
Werner Offermann ◽  
Evi Fiedler ◽  
Corinna Helmle-Kolb ◽  
Werner Hofer ◽  
Harald Kugel ◽  
...  

2020 ◽  
Vol 2020 ◽  
pp. 1-20
Author(s):  
Jinghui Zhang ◽  
Guoqiang Zeng ◽  
Shifeng Zhang

This paper presents a novel nonlinear sliding mode control scheme that combines on-line model modification, a nonlinear sliding mode controller, and a disturbance observer to solve the essential problems in spacecraft electromagnetic docking control, such as model uncertainties, unknown external disturbances, and inherent strong nonlinearity and coupling. An improved far-field model of electromagnetic force which is much more accurate than the widely used far-field model is proposed to enable the model parameters to be on-line self-adjusting. Then, the relationship between magnetic moment allocation and energy consumption is derived, and the optimal direction of the magnetic moment vector is obtained. Based on the proposed improved far-field model and the research results of magnetic moment allocation law, a fast-nonsingular terminal mode controller driven by a disturbance observer is designed in the presence of model uncertainties and external disturbances. The proposed control method is guaranteed to be chattering-free and to possess superior properties such as finite-time convergence, high-precision tracking, and strong robustness. Two simulation scenarios are conducted to illustrate the necessity of modifying the far-field model and the effectiveness of the proposed control scheme. The simulation results indicate the realization of electromagnetic soft docking and validate the merits of the proposed control scheme. In the end of this paper, some conclusions are drawn.


2002 ◽  
Vol 74 (16) ◽  
pp. 4191-4197 ◽  
Author(s):  
Andrew M. Wolters ◽  
Dimuthu A. Jayawickrama ◽  
Cynthia K. Larive ◽  
Jonathan V. Sweedler
Keyword(s):  

2004 ◽  
Vol 82 (9) ◽  
pp. 717-729 ◽  
Author(s):  
L M García-Cruz ◽  
A Rubio-Ponce ◽  
A E García ◽  
R Baquero

We study the magnetic behavior of a 4d transition-metal Ru monolayer (ML) on different substrates and orientations. In the ground state, an ideal Ru-ML is expected to be ferromagnetic on Ag(001) and Au(001) with a magnetic moment, µ, around 1.7 µB (Bohr magnetons) in both cases. On Cu(001), a Ru-ML is not magnetic. In this paper, we study the magnetic behavior of a Ru-ML at other orientations, i.e., (110) and (111), and analyze the phenomenon as a whole. We find magnetism on Au(111), and Ag(111) (µ ≈ 1 µB for both) but no magnetic activity on a Cu substrate in any orientation. This gives the first impression that the lattice parameter of the substrate is the one that governs the switching on of magnetism in the Ru-ML. But then, we find that on both Ag(110) and Au(110), an ideal Ru-ML is not magnetic. For that reason, we have tried to find another geometric parameter that would correlate better with the magnetic moment. We find that neither the total number of first nearest neighbors for each orientation, nor the number of them on the ML, or the number of them in the substrate, or the area per atom on the ML, correlate. We find a correlation with a parameter, Ω0, that represents the volume per atom in the monolayer–substrate interface region. But this parameter seems to have the wrong trend according to intuition. Further analysis shows that the details of the interaction are important, and that the physics underlying the switching on of magnetism in a Ru-ML on noble metal substrates, is determined by an intraband transfer of d-electronic states, from lower and higher energies to the Fermi level, that enhances the density of states at that energy, in an important way. This depends on specificities of the interaction between the ML and the substrate that are hardly taken into account by a single parameter that is merely geometric. PACS Nos.: 75.10–b, 75.30–m, 75.70.Ak, 73.20.At


In a previous paper (referred to hereafter as Part I) a method for measuring the gyromagnetic ratio for paramagnetic substances was described. Owing to the smallness of the angular moment produced by a change in the magnetic moment of a paramagnetic substance, a low frequency resonance method was employed to build up the amplitude to a measurable magnitude. An account of the method of measurement and elimination of errors was given in detail. The results of experiments on one paramagnetic substance, Dy +++ in dysprosium oxide (Dy 2 O 3 ), showed the Landé splitting factor for this ion to be 1·28, which indicates that the magnetic moment arises from both orbital and spin contributions. This agrees well with the theoretical value 1·33, corresponding to the state 6 H 15/2 deduced by Hund as the most probable ground state of this ion. The present contribution deals with results on salts of the iron group. The magnetic susceptibilities range from 10 -5 to 10 -4 compared with 2·4 × 10 -4 in the case of the Dy 2 O 3 previously used. This necessitates a greater sensi­tivity than that used in Part I, and the means employed to achieve this are described below.


2005 ◽  
Vol 94 (2) ◽  
Author(s):  
G. Neyens ◽  
M. Kowalska ◽  
D. Yordanov ◽  
K. Blaum ◽  
P. Himpe ◽  
...  
Keyword(s):  

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