An Iron-Porphyrin Complex with Large Easy-Axis Magnetic Anisotropy on Metal Substrate

ACS Nano ◽  
2017 ◽  
Vol 11 (11) ◽  
pp. 11402-11408 ◽  
Author(s):  
Bing Liu ◽  
Huixia Fu ◽  
Jiaqi Guan ◽  
Bin Shao ◽  
Sheng Meng ◽  
...  
2021 ◽  
Vol 60 (6) ◽  
pp. 3843-3850
Author(s):  
Ashwin Chaturvedi ◽  
Caroline K. Williams ◽  
Nilakshi Devi ◽  
Jianbing “Jimmy” Jiang

1999 ◽  
Vol 562 ◽  
Author(s):  
K. Attenborough ◽  
M. Cerisier ◽  
H. Boeve ◽  
J. De Boeck ◽  
G. Borghs ◽  
...  

ABSTRACTWe have studied the magnetic and structural properties of thin electrodeposited Co and Cu layers grown directly onto (100) n-GaAs and have investigated the influence of a buffer layer. A dominant fourfold anisotropy with a uniaxial contribution is observed in 10 nm Co electrodeposited films on GaAs. An easy axis is observed in the [001] GaAs direction with two hard axes of differing coercivities parallel to the [011] and [011] directions. For thicker films the easy axes in the [001] direction becomes less pronounced and the fourfold anisotropy becomes less dominant. Co films of similar thicknesses deposited onto an electrodeposited Cu buffer layer were nearly isotropic. From X-ray diffraction 21 nm Co layers on GaAs were found to be hcp with the c-axis tending to be in the plane of the film. The anisotropy is ascribed to the Co/GaAs interface and is held responsible for the unique spin-valve properties seen recently in electrodeposited Co/Cu films.


2019 ◽  
Vol 9 (1) ◽  
Author(s):  
Oana Ciubotariu ◽  
Anna Semisalova ◽  
Kilian Lenz ◽  
Manfred Albrecht

AbstractIn the attempt of implementing iron garnets with perpendicular magnetic anisotropy (PMA) in spintronics, the attention turned towards strain-grown iron garnets. One candidate is Tm3Fe5O12 (TmIG) which possesses an out-of-plane magnetic easy axis when grown under tensile strain. In this study, the effect of film thickness on the structural and magnetic properties of TmIG films including magnetic anisotropy, saturation magnetization, and Gilbert damping is investigated. TmIG films with thicknesses between 20 and 300 nm are epitaxially grown by pulsed laser deposition on substituted-Gd3Ga5O12(111) substrates. Structural characterization shows that films thinner than 200 nm show in-plane tensile strain, thus exhibiting PMA due to strain-induced magnetoelastic anisotropy. However, with increasing film thickness a relaxation of the unit cell is observed resulting in the rotation of the magnetic easy axis towards the sample plane due to the dominant shape anisotropy. Furthermore, the Gilbert damping parameter is found to be in the range of 0.02 ± 0.005.


2014 ◽  
Vol 20 (44) ◽  
pp. 14262-14269 ◽  
Author(s):  
Itziar Oyarzabal ◽  
José Ruiz ◽  
José Manuel Seco ◽  
Marco Evangelisti ◽  
Agustín Camón ◽  
...  

Nanoscale ◽  
2018 ◽  
Vol 10 (36) ◽  
pp. 17335-17340 ◽  
Author(s):  
Yun Zhang ◽  
Zhao Wei ◽  
Meiguang Zhang ◽  
Xiao Gu ◽  
Li Huang

A huge MAE up to 180 meV is found in a 2D Ir–DCA framework with the easy axis perpendicular to the sheet.


2018 ◽  
Vol 28 (32) ◽  
pp. 1801846 ◽  
Author(s):  
Mauro Perfetti ◽  
Mikkel A. Sørensen ◽  
Ursula B. Hansen ◽  
Heiko Bamberger ◽  
Samuel Lenz ◽  
...  

CrystEngComm ◽  
2020 ◽  
Vol 22 (13) ◽  
pp. 2297-2303 ◽  
Author(s):  
Yuewei Wu ◽  
Jing Xi ◽  
Jinhui Yang ◽  
Weiming Song ◽  
Shuchang Luo ◽  
...  

Coligand effects lead to two mononuclear octahedral Co(ii) complexes exhibiting easy-axis magnetic anisotropies and distinct magnetic properties.


1989 ◽  
Vol 151 ◽  
Author(s):  
F. J. Lamelas ◽  
C. H. Lee ◽  
Hui He ◽  
W. Vavra ◽  
Roy Clarke

ABSTRACTA series of epitaxial Co-Cu superlattices has been grown on GaAs (110) substrates by molecular beam epitaxy. Detailed analysis of x-ray diffuse scattering scans along Co (101ℓ) reveals a crossover from from the bulk hcp phase of Co to metastable fcc stacking. Our measurements indicate a strong correlation between structural symmetry and the magnetic anisotropy in Co - noble metal superlattices. In particular, the perpendicular easy axis of magnetization onsets at Co layer thickness ♣ 19 Å in Cohcp-Au compared to only ˜11 Å in Cofcc-Cu.


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