Free-standing GaN substrates fabricated by a combination of substrate fracturing and chemical lift-off

2011 ◽  
Vol 8 (7-8) ◽  
pp. 2123-2126 ◽  
Author(s):  
Hiroki Goto ◽  
Hyun-Jae Lee ◽  
Seogwoo Lee ◽  
Meoung-Whan Cho ◽  
Takafumi Yao
Keyword(s):  
2020 ◽  
Vol 3 (1) ◽  
Author(s):  
Jinyong Ma ◽  
Jiayi Qin ◽  
Geoff T. Campbell ◽  
Giovanni Guccione ◽  
Ruvi Lecamwasam ◽  
...  

Abstract Optical levitation of mechanical oscillators has been suggested as a promising way to decouple the environmental noise and increase the mechanical quality factor. Here, we investigate the dynamics of a free-standing mirror acting as the top reflector of a vertical optical cavity, designed as a testbed for a tripod cavity optical levitation setup. To reach the regime of levitation for a milligram-scale mirror, the optical intensity of the intracavity optical field approaches 3 MW cm−2. We identify three distinct optomechanical effects: excitation of acoustic vibrations, expansion due to photothermal absorption, and partial lift-off of the mirror due to radiation pressure force. These effects are intercoupled via the intracavity optical field and induce complex system dynamics inclusive of high-order sideband generation, optical bistability, parametric amplification, and the optical spring effect. We modify the response of the mirror with active feedback control to improve the overall stability of the system.


2001 ◽  
Vol 680 ◽  
Author(s):  
U. Karrer ◽  
C.R. Miskys ◽  
O. Ambacher ◽  
M. Stutzmann

ABSTRACTThick GaN films, grown by hydride vapor phase epitaxy (HVPE), were separated from their sapphire substrate with a laser-induced lift-off process. After cleaning and polishing, these films offer the most direct way to investigate and compare the influence of crystal polarity on the electronic properties of Ga-face and N-face surfaces, respectively. Different barrier heights for Pt Schottky diodes evaporated onto Ga- and N-face GaN are determined from the dependence of the effective barrier height versus ideality factor by I-V measurements to 1.15 eV and 0.80 eV, respectively. The charge neutrality condition at the surface is modified by the spontaneous polarization due to the polarization induced bound sheet charge. This effect has to be included in the electronegativity concept of metal induced gap states (MIGS) and can also be illustrated by different band bending of the conduction and valence band, inferred from the self-consistent solution of the Schrödinger-Poisson equation. Furthermore, temperature dependent I-V characteristics are compared to simulated behavior of Schottky diodes, exhibiting excellent agreement in forward direction, but showing deviations in the reverse current.


2006 ◽  
Vol 3 (6) ◽  
pp. 1475-1478 ◽  
Author(s):  
T. Paskova ◽  
V. Darakchieva ◽  
P. P. Paskov ◽  
B. Monemar ◽  
M. Bukowski ◽  
...  
Keyword(s):  

2014 ◽  
Vol 104 (25) ◽  
pp. 252109 ◽  
Author(s):  
Yoshiaki Mokuno ◽  
Yukako Kato ◽  
Nobuteru Tsubouchi ◽  
Akiyoshi Chayahara ◽  
Hideaki Yamada ◽  
...  

2019 ◽  
Vol 22 (2) ◽  
pp. 1901192 ◽  
Author(s):  
Steffen Bornemann ◽  
Nursidik Yulianto ◽  
Hendrik Spende ◽  
Yuliati Herbani ◽  
Joan Daniel Prades ◽  
...  

1995 ◽  
Vol 10 (5) ◽  
pp. 1321-1326 ◽  
Author(s):  
Jaecheol Bang ◽  
Guo-Quan Lu

The kinetics of constrained-film sintering were studied in a borosilicate glass (BSG) + silica system because of their applications in microelectronic packaging technologies. Samples with a silica content by 20% by volume were prepared from slurries of powder mixtures in a commercial polyvinyl butyral (PVB) binder solution. Constrained films about 0.2 mm thick were formed by doctor-blade casting the slurries on silicon wafers. Free-standing films about 0.6 mm thick were also produced by casting the slurries on a treated mylar sheet for easy lift-off. Sintering experiments were carried out in a hot stage at temperatures between 715 °C and 775 °C. Shrinkage profiles of the free and constrained (shrinkage in thickness only) films were determined in situ using a custom-designed optical system. The densification rates measured in the constrained films were slower than those in the free films. However, the substrate constraint had no effect on the activation energy of densification which was found equal to 385 ± 10 kJ/mol, the same for both free and constrained films. A relation between the constrained-film and free-film densification profiles was derived using the viscous analogy for the constitutive equations of a porous sintering body.


2013 ◽  
Vol 38 ◽  
pp. 919-925 ◽  
Author(s):  
Sarah Kajari-Schröder ◽  
Jörg Käsewieter ◽  
Jan Hensen ◽  
Rolf Brendel

2019 ◽  
Vol 16 (150) ◽  
pp. 20180626 ◽  
Author(s):  
Nikolay V. Ryzhkov ◽  
Natalya A. Mamchik ◽  
Ekaterina V. Skorb

In situ studies of transmembrane channels often require a model bioinspired artificial lipid bilayer (LB) decoupled from its underlaying support. Obtaining free-standing lipid membranes is still a challenge. In this study, we suggest an electrochemical approach for LB separation from its solid support via hydroquinone oxidation. Layer-by-layer deposition of polyethylenimine (PEI) and polystyrene sulfonate (PSS) on the gold electrode was performed to obtain a polymeric nanocushion of [PEI/PSS] 3 /PEI. The LB was deposited on top of an underlaying polymer support from the dispersion of small unilamellar vesicles due to their electrostatic attraction to the polymer support. Since lipid zwitterions demonstrate pH-dependent charge shifting, the separation distance between the polyelectrolyte support and LB can be adjusted by changing the environmental pH, leading to lipid molecules recharge. The proton generation associated with hydroquinone oxidation was studied using scanning vibrating electrode and scanning ion-selective electrode techniques. Electrochemical impedance spectroscopy is suggested to be a powerful instrument for the in situ observation of processes associated with the LB–solid support interface. Electrochemical spectroscopy highlighted the reversible disappearance of the LB impact on impedance in acidic conditions set by dilute acid addition as well as by electrochemical proton release on the gold electrode due to hydroquinone oxidation.


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