Origin of orbital momentum and magnetic anisotropy in transition metals

1990 ◽  
Vol 67 (9) ◽  
pp. 4555-4557 ◽  
Author(s):  
H. J. F. Jansen
APL Materials ◽  
2020 ◽  
Vol 8 (7) ◽  
pp. 071105
Author(s):  
Jianpei Xing ◽  
Peng Wang ◽  
Zhou Jiang ◽  
Xue Jiang ◽  
Yi Wang ◽  
...  

1993 ◽  
Vol 48 (13) ◽  
pp. 9894-9897 ◽  
Author(s):  
Brad N. Engel ◽  
Michael H. Wiedmann ◽  
Robert A. Van Leeuwen ◽  
Charles M. Falco

1989 ◽  
Vol 130 (1-3) ◽  
pp. 65-87 ◽  
Author(s):  
Michael C. Böhm ◽  
Christian Elsässer ◽  
Manfred Fähnle ◽  
Ernst-Helmut Brandt

2018 ◽  
Vol 54 (72) ◽  
pp. 10084-10087 ◽  
Author(s):  
Yu. V. Manakin ◽  
V. S. Mironov ◽  
T. A. Bazhenova ◽  
K. A. Lyssenko ◽  
I. F. Gilmutdinov ◽  
...  

We demonstrate that a planar pentadentate organic ligand can generate sufficiently strong ligand-field to stabilize the low-spin orbitally-degenerate configuration of Mo(iii) that results in strong Ising-type magnetic anisotropy.


SPIN ◽  
2016 ◽  
Vol 06 (02) ◽  
pp. 1640002 ◽  
Author(s):  
Jacob Torrejon ◽  
Junyeon Kim ◽  
Jaivardhan Sinha ◽  
Masamitsu Hayashi

We study effects originating from the strong spin–orbit coupling in CoFeB/MgO heterostructures with heavy metal (HM) underlayers. The perpendicular magnetic anisotropy at the CoFeB/MgO interface, the spin Hall angle of the heavy metal layer, current induced torques and the Dzyaloshinskii–Moriya interaction at the HM/CoFeB interfaces are studied for films in which the early 5[Formula: see text] transition metals are used as the HM underlayer. We show how the choice of the HM layer influences these intricate spin–orbit effects that emerge within the bulk and at interfaces of the heterostructures.


Author(s):  
R.W. Carpenter

Interest in precipitation processes in silicon appears to be centered on transition metals (for intrinsic and extrinsic gettering), and oxygen and carbon in thermally aged materials, and on oxygen, carbon, and nitrogen in ion implanted materials to form buried dielectric layers. A steadily increasing number of applications of microanalysis to these problems are appearing. but still far less than the number of imaging/diffraction investigations. Microanalysis applications appear to be paced by instrumentation development. The precipitation reaction products are small and the presence of carbon is often an important consideration. Small high current probes are important and cryogenic specimen holders are required for consistent suppression of contamination buildup on specimen areas of interest. Focussed probes useful for microanalysis should be in the range of 0.1 to 1nA, and estimates of spatial resolution to be expected for thin foil specimens can be made from the curves shown in Fig. 1.


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