scholarly journals Magnetostriction in Amorphous Co66Fe34 Microcantilevers Fabricated with Hydrogenated Amorphous Silicon

2020 ◽  
Vol 233 ◽  
pp. 05003
Author(s):  
B.M. Silveira ◽  
J.H. Belo ◽  
R. Pinto ◽  
J.A. Silva ◽  
T.D. Ferreira ◽  
...  

To study the magnetostriction of Co66Fe34 thin films, amorphous silicon microcantilevers were prepared by surface micromachining, and the 136 nm-thick magnetostrictive film was deposited by electron beam physical vapor deposition and patterned on top of the microcantilever structure. The magnetostriction of the Co66Fe34 films was confirmed by measuring the deflection of the cantilevers under a varying magnetic field, reaching displacements up to 8 nm. The configuration was simulated using COMSOL software, yielding a similar deflection behavior as a function of the magnetic field, with a film with a magneto strictive coefficient of λ S ~ 55 p.p.m. The experimental configuration uses a laser and a position sensitive detector to measure the displacement, based on an optical lever configuration, and a piezoelectric stage to calibrate the system.

2015 ◽  
Vol 656-657 ◽  
pp. 92-100
Author(s):  
Li Cheng Hu ◽  
Yong Shiang Li ◽  
Chien Chieh Lee ◽  
Jeng Yang Cheng ◽  
I Chen Chen ◽  
...  

The uniformity improvement of high deposition rate in hydrogenated amorphous silicon (a-Si:H) film deposited by electron cyclotron resonance chemical vapor deposition (ECR-CVD) is very essential for a large substrate in PV solar industry. In order to improve the uniformity in depositing thin film in large area, the auxiliary magnetic coils were designed and installed in ECR-CVD to modify the distribution of magnetic field. In addition, the dependence of the other ECR-CVD processing parameters such as resonance position, microwave power, working pressure, and substrate temperature were investigated. The results indicated that more uniform a-Si:H film could be obtained when working pressure was decreased. By using finite element analysis, it was found that location of turbo pump would impact gas flow field and this effect would become more significant at high pressure. Increasing microwave power, increasing horizontal gradient of the magnetic field to the substrate, and forming Cusp magnetic field could enhance ECR-CVD deposition uniformity greatly. However, the plasma location and substrate temperature were not major factors affecting a-Si:H film uniformity in ECR-CVD process. Finally, the optimal and the best 3.8% in uniformity could be achieved in 150mm diameter when the ratio of magnetic field strength at wafer edge to wafer center is 215%, working pressure is 1.5 mtorr, microwave power density is 4W/cm2, and substrate temperature is 180°C.


1987 ◽  
Vol 58 (2) ◽  
pp. 202-206 ◽  
Author(s):  
V. A. Chumak ◽  
M. Bertolotti ◽  
A. Ferrari ◽  
F. Bartoloni ◽  
F. Evangelisti

1978 ◽  
Vol 21 (11-12) ◽  
pp. 1461-1463 ◽  
Author(s):  
Robert A. Street ◽  
David K. Biegelsen ◽  
John C. Knights ◽  
Ching Tsang ◽  
Robert M. White

1985 ◽  
Vol 57 (10) ◽  
pp. 4778-4782 ◽  
Author(s):  
Satoshi Arimoto ◽  
Hidekazu Yamamoto ◽  
Hideo Ohno ◽  
Hideki Hasegawa

2001 ◽  
Vol 664 ◽  
Author(s):  
H. ǵuas ◽  
P. Nunes ◽  
E. Fortunato ◽  
R. Silva ◽  
V. Silva ◽  
...  

ABSTRACTIn this work a new structure is proposed for position sensitive detectors consisting of glass/Cr/a-Si:H(n+)/a-Si:H(i)/ZnO, where the ZnO forms an heterojunction with the a-Si:H(i). The results show that this structure works with success in the fabrication of linear position sensitive detectors. The devices present a good nonlinearity of ͌ 2% and a good sensitivity tothe light intensity. The main advantages of this structure over the classical p-i-n are an easier to built topology and a higher yield due to a better immunity to the a-Si:H pinholes, since the ZnO does not diffuse so easily into a-Si:H as the metal does, which are the cause of frequent failure in the p-i-n devices due to short-circuits caused by the deposition of the metal over the a-Si:H. In this structure the illumination is made directly on the ZnO, so a transparent substrate is not needed and a larger range of substrates can be used.


1967 ◽  
Vol 31 ◽  
pp. 375-380
Author(s):  
H. C. van de Hulst

Various methods of observing the galactic magnetic field are reviewed, and their results summarized. There is fair agreement about the direction of the magnetic field in the solar neighbourhood:l= 50° to 80°; the strength of the field in the disk is of the order of 10-5gauss.


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