scholarly journals Polarization domain walls in optical fibres as topological bits for data transmission

2017 ◽  
Vol 11 (2) ◽  
pp. 102-107 ◽  
Author(s):  
M. Gilles ◽  
P.-Y. Bony ◽  
J. Garnier ◽  
A. Picozzi ◽  
M. Guasoni ◽  
...  
Author(s):  
M. Gilles ◽  
P-Y Bony ◽  
M. Guasoni ◽  
A. Picozzi ◽  
J. Fatome
Keyword(s):  

2015 ◽  
Vol 51 (2) ◽  
pp. 168-170
Author(s):  
R.M. Ribeiro ◽  
V.N.H. Silva ◽  
A.P.L. Barbero ◽  
C.M. Alves ◽  
C.R.L. Rodrigues

1982 ◽  
Vol 4 (4) ◽  
pp. 477-479 ◽  
Author(s):  
P. M. Gray ◽  
M. M. Phillips ◽  
A. J. Turtle ◽  
R. Ellis

Work on the development and use of optical fibres as light guides in astronomical spectroscopy has been underway at the AAO for over a year now. The fibres used are step-index polymer-clad silica with a core size of 200 microns giving an aperture size of 1.3 arcsec at the AAT f/8 focus. They are optimised for data transmission with losses below 5dB/km at a wavelength of 800 nm. The blue transmission is somewhat lower, typically 500dB/km at 300nm and 90dB/km at 400nm but over the short 2m length used these attenuations give transmissions of 79% and 96% respectively.


Author(s):  
M. Gilles ◽  
P-Y. Bony ◽  
J. Garnier ◽  
A. Picozzi ◽  
M. Guasoni ◽  
...  

2017 ◽  
pp. 217-310
Author(s):  
G. Stepniak ◽  
M. Schüppert ◽  
C.-A. Bunge

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.


Author(s):  
Yalcin Belli

Fe-Cr-Co alloys have great technological potential to replace Alnico alloys as hard magnets. The relationship between the microstructures and the magnetic properties has been recently established for some of these alloys. The magnetic hardening has been attributed to the decomposition of the high temperature stable phase (α) into an elongated Fe-rich ferromagnetic phase (α1) and a weakly magnetic or non-magnetic Cr-rich phase (α2). The relationships between magnetic domains and domain walls and these different phases are yet to be understood. The TEM has been used to ascertain the mechanism of magnetic hardening for the first time in these alloys. The present paper describes the magnetic domain structure and the magnetization reversal processes in some of these multiphase materials. Microstructures to change properties resulting from, (i) isothermal aging, (ii) thermomagnetic treatment (TMT) and (iii) TMT + stepaging have been chosen for this investigation. The Jem-7A and Philips EM-301 transmission electron microscopes operating at 100 kV have been used for the Lorentz microscopy study of the magnetic domains and their interactions with the finely dispersed precipitate phases.


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