scholarly journals Dependence of Incident Angle of Surface Morphology of Polycrystalline Copper after Helium Ion Irradiation

Shinku ◽  
2004 ◽  
Vol 47 (1) ◽  
pp. 29-32
Author(s):  
Takashi TAGUCHI ◽  
Yuji YAMAUCHI ◽  
Yuko HIROHATA ◽  
Tomoaki HINO ◽  
Ichiro YANAGISAWA ◽  
...  
2010 ◽  
Vol 670 ◽  
pp. 131-134 ◽  
Author(s):  
Tomoaki Hino ◽  
T. Kobayashi ◽  
Y. Yamauchi ◽  
Y. Nobuta ◽  
M. Nishikawa

In order to smooth the uneven surface of polycrystalline copper, argon ion etching at the elevated temperature was conducted. The polycrystalline copper was obliquely irradiated by argon ion beam with ion energy of 1 keV and an incident angle of 70°. The substrate temperatures during argon ion irradiation were room temperature (RT), 473 K and 573 K. Before and after the irradiation, the surface morphology was observed using an atomic force microscope (AFM). After the irradiation at 473 K and 573 K, the surface was significantly smoothed compared with that at RT. In addition, the fluence required to obtain the smooth surface can be very low, compared with the case at RT. The present study shows that the oblique ion etching at elevated temperature is quite useful to obtain the smooth surface.


2003 ◽  
Vol 777 ◽  
Author(s):  
T. Devolder ◽  
M. Belmeguenai ◽  
C. Chappert ◽  
H. Bernas ◽  
Y. Suzuki

AbstractGlobal Helium ion irradiation can tune the magnetic properties of thin films, notably their magneto-crystalline anisotropy. Helium ion irradiation through nanofabricated masks can been used to produce sub-micron planar magnetic nanostructures of various types. Among these, perpendicularly magnetized dots in a matrix of weaker magnetic anisotropy are of special interest because their quasi-static magnetization reversal is nucleation-free and proceeds by a very specific domain wall injection from the magnetically “soft” matrix, which acts as a domain wall reservoir for the “hard” dot. This guarantees a remarkably weak coercivity dispersion. This new type of irradiation-fabricated magnetic device can also be designed to achieve high magnetic switching speeds, typically below 100 ps at a moderate applied field cost. The speed is obtained through the use of a very high effective magnetic field, and high resulting precession frequencies. During magnetization reversal, the effective field incorporates a significant exchange field, storing energy in the form of a domain wall surrounding a high magnetic anisotropy nanostructure's region of interest. The exchange field accelerates the reversal and lowers the cost in reversal field. Promising applications to magnetic storage are anticipated.


1998 ◽  
Vol 80 (21) ◽  
pp. 4713-4716 ◽  
Author(s):  
M. V. Ramana Murty ◽  
T. Curcic ◽  
A. Judy ◽  
B. H. Cooper ◽  
A. R. Woll ◽  
...  

2013 ◽  
Vol 435 (1-3) ◽  
pp. 214-221 ◽  
Author(s):  
Hongyu Fan ◽  
Li Sun ◽  
Deming Yang ◽  
Jinhai Niu ◽  
Liping Guo ◽  
...  

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