Two-dimensional implications of a purely reactive model for plasma etching

1991 ◽  
Vol 38 (9) ◽  
pp. 2025-2032 ◽  
Author(s):  
A.F. Gerodolle ◽  
J. Pelletier
Langmuir ◽  
2014 ◽  
Vol 30 (41) ◽  
pp. 12354-12361 ◽  
Author(s):  
Eser M. Akinoglu ◽  
Anthony J. Morfa ◽  
Michael Giersig

2017 ◽  
Vol 110 (13) ◽  
pp. 131901 ◽  
Author(s):  
Yongbeom Kwon ◽  
Geonyeop Lee ◽  
Sooyeoun Oh ◽  
Jihyun Kim ◽  
Stephen J. Pearton ◽  
...  

2007 ◽  
Vol 56 (2) ◽  
pp. 977
Author(s):  
Ma Xiao-Tao ◽  
Zheng Wan-Hua ◽  
Ren Gang ◽  
Fan Zhong-Chao ◽  
Chen Liang-Hui

2004 ◽  
Vol 03 (01n02) ◽  
pp. 81-85
Author(s):  
E. Yu. GAVRILIN ◽  
Yu. B. GORBATOV ◽  
V. V. STARKOV ◽  
A. F. VYATKIN

Photonic crystals are the very promising novel materials for micro- and nanophotonics for visible region. To produce photonic crystals for this region of light, artificial structures with characteristic sizes less than 1 μm have to be manufactured. Electrochemical deep anodic etching and plasma etching techniques is normally used to produce such structures in silicon wafers. However, standard way of deep anodic etching realization is not suitable for sub-micrometer porous silicon formation. In the present work combination of the deep anodic etching and focused ion beam techniques is used to produce ordered structure of macropores in silicon.


2006 ◽  
Vol 3 (4) ◽  
pp. 209-215
Author(s):  
Z.M. Xiao ◽  
B.J. Chen ◽  
H. Fan

The paper describes the fabrication and characterization of two-dimensional resonant micromirror device actuated by sol-gel deposited PZT thin films. The actuation principle is based on the bimorph beam structure, which consists of an oxide layer and a piezoelectric PZT layer. The two-dimensional scanning performance can be achieved by applying AC voltages with phase shifts at resonance to the actuating beams. The devices are fabricated through thin film depositions, lithography, dry plasma etching and the ICP release process. For a micromirror structure with a 300μm ×300μm mirror plate, the first four resonance frequencies are measured to be in the range of 10–30 kHz. To investigate the vibration modes, the deflections on different locations of the mirror plate are measured. The two dimensional scanning angle is determined to be in one direction and 11° at 23.4 kHz in the perpendicular direction.


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