bulk anisotropy
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2021 ◽  
Author(s):  
Olaf Eisen ◽  
Steven Franke ◽  
Daniela Jansen ◽  
John Paden ◽  
Reinhard Drews ◽  
...  

<p>Crystal anisotropy of ice causes slight birefringence for electromagnetic waves. At the same time, the mechanical anisotropy amounts to several orders of magnitude, thus making fabric properties highly-relevant for internal deformation. To date, bulk anisotropy of glaciers and ice sheets can be determined by geophysical methods, such as polarimetric radar, or direct sampling from ice cores. A shortcoming has been so far that changes of bulk anisotropy could mainly be inferred at single point observations, but less so as continuous profiles. Here, we exploit the effect of birefringence caused by bulk anisotropy in co-polarized airborne radar data to determine the horizontal anisotropy across the North-East Greenland Ice Stream. We base our analysis on the fact that birefringence causes a second-order effect on radar amplitudes, which leads to a beat frequency in the low and medium frequency range (O(100 kHz)), which is proportional to the horizontal anisotropy. Complementing our radar analysis with direct fabric and dielectric property observations we can constrain the range of all three fabric eigenvalues as a function of space across and along the ice stream. Finally, we assess the effect of the inferred fabric distribution on the overall ice rheology in the context of ice stream dynamics. Our overall approach has the advantage that it can be applied to co-polarized radar systems, as commonly used in profiling surveys, and does not require dedicated cross-polarized radar set-up. This provides the opportunity to revisit older data, especially from Greenland and Antarctica, to map fabric anisotropy in ice-dynamically interesting regions.</p>


Nanoscale ◽  
2020 ◽  
Vol 12 (11) ◽  
pp. 6378-6384 ◽  
Author(s):  
S. Lequeux ◽  
N. Perrissin ◽  
G. Grégoire ◽  
L. Tillie ◽  
A. Chavent ◽  
...  

Perpendicular Shape Anisotropy based storage layer offers a bulk anisotropy much more robust against thermal fluctuations than the interfacial anisotropy, allowing to reduce the temperature dependence of the coercivity of sub-20 nm MTJ cells.


2007 ◽  
Vol 204 (12) ◽  
pp. 4009-4012 ◽  
Author(s):  
Peili Niu ◽  
Ming Yue ◽  
Yongli Li ◽  
Wei Huang ◽  
Jiuxing Zhang

2005 ◽  
Vol 97 (6) ◽  
pp. 063704 ◽  
Author(s):  
A. Zakharova ◽  
S. T. Yen ◽  
K. Nilsson ◽  
K. A. Chao

Author(s):  
N. Klopĉar ◽  
I. Drevenŝek-olenik ◽  
M. Ĉopiĉ ◽  
M. W. Kim ◽  
A. Rastegar ◽  
...  

2000 ◽  
Vol 62 (19) ◽  
pp. 13048-13052 ◽  
Author(s):  
K. Hingerl ◽  
R. E. Balderas-Navarro ◽  
W. Hilber ◽  
A. Bonanni ◽  
D. Stifter

1996 ◽  
Vol 53 (16) ◽  
pp. R10548-R10551 ◽  
Author(s):  
B. Hillebrands ◽  
J. Fassbender ◽  
R. Jungblut ◽  
G. Güntherodt ◽  
D. J. Roberts ◽  
...  
Keyword(s):  

1996 ◽  
Vol 459 ◽  
Author(s):  
C. Favieres ◽  
C. Caroca ◽  
E. López ◽  
M. C. Sánchez ◽  
P. Sánchez ◽  
...  

ABSTRACTElectrolytic cylindrical amorphous CoP multilayers, grown on copper wires, with controlled continuos variation of the magnetic anisotropy, in both, direction and magnitude, have been produced. The inner zone of the samples has been grown to exhibit radial anisotropy and the overlayer has been obtained with planar longitudinal anisotropy. Our studies have revealed that the magnetization at the surface of the samples is strongly coupled with the bulk anisotropy for thickness of the overlayer of ≈ 1.5 μm. Furthermore, it has been found that an angular deformation applied to the samples, when the copper wire is subjected to a torsion, modifies the direction of the longitudinal anisotropy to the helical direction. Also, a large spontaneous Matteucci effect is induced by means of this angular deformation.


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