Dependence of Magnetic Coupling Constant of Ammonia on the Inversion State

1961 ◽  
Vol 16 (11) ◽  
pp. 2283-2287 ◽  
Author(s):  
Koichi Shimoda
Keyword(s):  
Magnetic Coupling ◽  
Coupling Constant ◽  
Inversion State ◽  
Magnetic Coupling Constant

Intra-molecular magnetic exchange interaction in the tripyridinium bis[tetrachloroferrate(iii)] chloride molecular magnet: a broken symmetry-DFT study

2015 ◽  
Vol 17 (29) ◽  
pp. 19119-19125 ◽  
Author(s):  
F. Baniasadi ◽  
M. M. Tehranchi ◽  
M. B. Fathi ◽  
N. Safari ◽  
V. Amani
Keyword(s):  
Magnetic Coupling ◽  
Dft Method ◽  
Broken Symmetry ◽  
Molecular Magnet ◽  
Coupling Constant ◽  
Magnetic Exchange Interaction ◽  
Magnetic Exchange ◽  
Electronic Spin ◽  
Density Maps ◽  
Magnetic Coupling Constant

A superexchange interaction path between Fe–Fe in (FeCl4)2(py·H)3Cl is illustrated making use of electronic spin density maps (ESDM) and the magnetic coupling constant is calculated using the BS-DFT method as JFe–Fe = 13.2062 kJ mol−1.

Highly efficient perturbative + variational strategy based on orthogonal valence bond theory for the evaluation of magnetic coupling constants. Application to the trinuclear Cu(ii) site of multicopper oxidases

2016 ◽  
Vol 18 (27) ◽  
pp. 18365-18380 ◽  
Author(s):  
Lorenzo Tenti ◽  
Daniel Maynau ◽  
Celestino Angeli ◽  
Carmen J. Calzado
Keyword(s):  
Low Cost ◽  
Valence Bond ◽  
Magnetic Coupling ◽  
Coupling Constants ◽  
Coupling Constant ◽  
Multicopper Oxidases ◽  
Valence Bond Theory ◽  
Bond Theory ◽  
Rational Evaluation ◽  
Magnetic Coupling Constant

A new perturbative + variational strategy: a low-cost, quantitative and rational evaluation of the magnetic coupling constant in complex systems.

Change in torque transmitted by a standard magnetic coupling with the same overall dimensions, depending on the grade of permanent magnet and its dimensions

2021 ◽  
pp. 30-34
Author(s):  
Keyword(s):  
Permanent Magnet ◽  
Permanent Magnets ◽  
Magnetic Coupling ◽  
Coupling Constant ◽  
Air Gaps ◽  
Neodymium Iron Boron ◽  
Magnetic Couplings ◽  
Magnetic Coupling Constant

The possibility of changing the torque transmitted by a cylindrical magnetic coupling, depending on the brand of a high-coercive permanent magnet — neodymium— iron—boron, samarium—cobalt is considered. Using the example of standard magnetic couplings with a diameter of 133 mm for magnets and air gaps between the half couplings for magnets of 5 and 7 mm, the change in the torque transmitted by the magnetic coupling without changing its overall dimensions is shown. Varying the torque of the magnetic coupling is possible by changing the shape, size and grade of permanent magnets while keeping the same number of magnets in each of the half-couplings of the magnetic coupling constant. Keywords; magnetic coupling, permanent magnet, number of magnets. [email protected]

scholarly journals Temperature dependent magnetization of the two band model for diluted magnetic semiconductors

2014 ◽  
Vol 24 (2) ◽  
pp. 141
Author(s):  
Vu Kim Thai ◽  
Hoang Anh Tuan
Keyword(s):  
Diluted Magnetic Semiconductors ◽  
Magnetic Semiconductors ◽  
Magnetic Coupling ◽  
Band Model ◽  
Coupling Constant ◽  
Temperature Dependent ◽  
Impurity Bands ◽  
Diluted Magnetic ◽  
Two Band Model ◽  
Temperature Dependent Magnetization

The temperature dependent magnetization of a two band model for diluted magnetic semiconductors as a function of magnetic coupling constant, hopping parameters and carrier densities is calculated by using the coherent potential approximation.  It is shown that the degree of overlapping of the impurity bands  and carrier density are crucial parameters determining the magnetization behavior of the system.

Grain separation enhanced magnetic coercivity in Pt/Co multilayers.

1993 ◽  
Vol 51 ◽  
pp. 1038-1039 ◽  
Author(s):  
G.A. Bertero ◽  
R. Sinclair
Keyword(s):  
Remanent Magnetization ◽  
Strong Influence ◽  
Uniaxial Anisotropy ◽  
Magnetic Coupling ◽  
Recording Media ◽  
Magnetic Media ◽  
Signal To Noise ◽  
Out Of Plane ◽  
Longitudinal Recording ◽  
The Relationship

Pt/Co multilayers displaying perpendicular (out-of-plane) magnetic anisotropy and 100% perpendicular remanent magnetization are strong candidates as magnetic media for the next generation of magneto-optic recording devices. The magnetic coercivity, Hc, and uniaxial anisotropy energy, Ku, are two important materials parameters, among others, in the quest to achieving higher recording densities with acceptable signal to noise ratios (SNR). The relationship between Ku and Hc in these films is not a simple one since features such as grain boundaries, for example, can have a strong influence on Hc but affect Ku only in a secondary manner. In this regard grain boundary separation provides a way to minimize the grain-to-grain magnetic coupling which is known to result in larger coercivities and improved SNR as has been discussed extensively in the literature for conventional longitudinal recording media.We present here results from the deposition of two Pt/Co/Tb multilayers (A and B) which show significant differences in their coercive fields.

Imaging magnetic microstructure with SEMPA

1993 ◽  
Vol 51 ◽  
pp. 1032-1033
Author(s):  
M. H. Kelley ◽  
J. Unguris ◽  
R. J. Celotta ◽  
D. T. Pierce
Keyword(s):  
Electron Microscopy ◽  
Thin Films ◽  
Scanning Electron Microscopy ◽  
Sandwich Structure ◽  
Magnetic Coupling ◽  
Polarization Analysis ◽  
Secondary Electrons ◽  
Magnetic Microstructure ◽  
Escape Depth ◽  
Scanning Electron

By measuring the spin polarization of secondary electrons generated in a scanning electron microscope, scanning electron microscopy with polarization analysis (SEMPA) can directly image the magnitude and direction of a material’s magnetization. Because the escape depth of the secondaries is only on the order of 1 nm, SEMPA is especially well-suited for investigating the magnetization of ultra-thin films and surfaces. We have exploited this feature of SEMPA to study the magnetic microstrcture and magnetic coupling in ferromagnetic multilayers where the layers may only be a few atomic layers thick. For example, we have measured the magnetic coupling in Fe/Cr/Fe(100) and Fe/Ag/Fe(100) trilayers and have found that the coupling oscillates between ferromagnetic and antiferromagnetic as a function of the Cr or Ag spacer thickness.The SEMPA apparatus has been described in detail elsewhere. The sample consisted of a magnetic sandwich structure with a wedge-shaped interlayer as shown in Fig. 1.

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