scholarly journals SWR Studies of Higher-Order Surface Anisotropy Terms in (Ga,Mn)As Thin Films

2018 ◽  
Vol 133 (3) ◽  
pp. 635-638
Author(s):  
H. Puszkarski ◽  
P. Tomczak ◽  
H.T. Diep
1988 ◽  
Vol 49 (C8) ◽  
pp. C8-1695-C8-1696 ◽  
Author(s):  
J. R. Cullen ◽  
K. B. Hathaway

1999 ◽  
Author(s):  
S. Wanis ◽  
A. Sercovich ◽  
N. Komerath
Keyword(s):  

Nano Letters ◽  
2021 ◽  
Author(s):  
Jinkwon Kim ◽  
Junsik Mun ◽  
Carla M. Palomares García ◽  
Bongju Kim ◽  
Robin S. Perry ◽  
...  

Author(s):  
Mohd. Shkir ◽  
Kamlesh V. Chandekar ◽  
Aslam Khan ◽  
El Sayed Yousef ◽  
H. Elhosiny Ali ◽  
...  

Author(s):  
Amgad R. Rezk ◽  
Ofer Manor ◽  
Leslie Y. Yeo ◽  
James R. Friend

Arising from an interplay between capillary, acoustic and intermolecular forces, surface acoustic waves (SAWs) are observed to drive a unique and curious double flow reversal in the spreading of thin films. With a thickness at or less than the submicrometre viscous penetration depth, the film is seen to advance along the SAW propagation direction, and self-similarly over time t 1/4 in the inertial limit. At intermediate film thicknesses, beyond one-fourth the sound wavelength λ ℓ in the liquid, the spreading direction reverses, and the film propagates against the direction of the SAW propagation. The film reverses yet again, once its depth is further increased beyond one SAW wavelength. An unstable thickness region, between λ ℓ /8 and λ ℓ /4, exists from which regions of the film either rapidly grow in thickness to exceed λ ℓ /4 and move against the SAW propagation, consistent with the intermediate thickness films, whereas other regions decrease in thickness below λ ℓ /8 to conserve mass and move along the SAW propagation direction, consistent with the thin submicrometre films.


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