Inferences on the magnetic domain state of leg 37 basalts

1976 ◽  
Vol 81 (23) ◽  
pp. 4199-4206 ◽  
Author(s):  
G. S. Murthy ◽  
E. R. Deutsch ◽  
R. R. Pätzold
Keyword(s):  
1977 ◽  
Author(s):  
G.S. Murthy ◽  
E.R. Deutsch ◽  
R.R. Patzold
Keyword(s):  

Author(s):  
Andrew P. Roberts ◽  
Xiang Zhao ◽  
Pengxiang Hu ◽  
Alexandra Abrajevitch ◽  
Yen‐Hua Chen ◽  
...  

2006 ◽  
Vol 248 (1-2) ◽  
pp. 508-517 ◽  
Author(s):  
Mark J. Dekkers ◽  
Harald N. Böhnel
Keyword(s):  

Science ◽  
2011 ◽  
Vol 333 (6047) ◽  
pp. 1273-1276 ◽  
Author(s):  
H. C. Walker ◽  
F. Fabrizi ◽  
L. Paolasini ◽  
F. de Bergevin ◽  
J. Herrero-Martin ◽  
...  

Magneto-electric multiferroics exemplified by TbMnO3 possess both magnetic and ferroelectric long-range order. The magnetic order is mostly understood, whereas the nature of the ferroelectricity has remained more elusive. Competing models proposed to explain the ferroelectricity are associated respectively with charge transfer and ionic displacements. Exploiting the magneto-electric coupling, we used an electric field to produce a single magnetic domain state, and a magnetic field to induce ionic displacements. Under these conditions, interference between charge and magnetic x-ray scattering arose, encoding the amplitude and phase of the displacements. When combined with a theoretical analysis, our data allow us to resolve the ionic displacements at the femtoscale, and show that such displacements make a substantial contribution to the zero-field ferroelectric moment.


2018 ◽  
Vol 123 (2) ◽  
pp. 998-1017 ◽  
Author(s):  
P. X. Hu ◽  
X. Zhao ◽  
A. P. Roberts ◽  
D. Heslop ◽  
R. A. Viscarra Rossel

2016 ◽  
Vol 40 (11) ◽  
pp. 9275-9284 ◽  
Author(s):  
Satu G. Gawas ◽  
Sher Singh Meena ◽  
Seikh M. Yusuf ◽  
Vidhyadatta M. S. Verenkar

Reluctance and favorable orientation of magnetic domain with the field at RT and blocking temperature (TB), respectively, as an effect of enhanced magnetic anisotropy by virtue of Co substitution.


2017 ◽  
Vol 122 (7) ◽  
pp. 4767-4789 ◽  
Author(s):  
Xiang Zhao ◽  
Andrew P. Roberts ◽  
David Heslop ◽  
Greig A. Paterson ◽  
Yiliang Li ◽  
...  

2018 ◽  
Vol 453 ◽  
pp. 125-131 ◽  
Author(s):  
M. Manjunatha ◽  
Rajeev Kumar ◽  
Balaram Sahoo ◽  
Ramakrishna Damle ◽  
K.P. Ramesh

Author(s):  
J.N. Chapman ◽  
P.E. Batson ◽  
E.M. Waddell ◽  
R.P. Ferrier

By far the most commonly used mode of Lorentz microscopy in the examination of ferromagnetic thin films is the Fresnel or defocus mode. Use of this mode in the conventional transmission electron microscope (CTEM) is straightforward and immediately reveals the existence of all domain walls present. However, if such quantitative information as the domain wall profile is required, the technique suffers from several disadvantages. These include the inability to directly observe fine image detail on the viewing screen because of the stringent illumination coherence requirements, the difficulty of accurately translating part of a photographic plate into quantitative electron intensity data, and, perhaps most severe, the difficulty of interpreting this data. One solution to the first-named problem is to use a CTEM equipped with a field emission gun (FEG) (Inoue, Harada and Yamamoto 1977) whilst a second is to use the equivalent mode of image formation in a scanning transmission electron microscope (STEM) (Chapman, Batson, Waddell, Ferrier and Craven 1977), a technique which largely overcomes the second-named problem as well.


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