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RN552

更新时间: 2024-11-20 22:23:43
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描述
THIN FILM AMORPHOUS SILICON POSITION SENSITIVE DETECTORS

RN552 数据手册

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Thin-Film Amorphous Silicon  
Position-Sensitive Detectors  
By Jasmine Henry* and John Livingstone  
Optical position-sensitive detectors are a useful class of sensor with a wide range of  
applications in machine control systems, industrial alignment and robotic vision. They  
have distinct advantages over most arrayed discrete optical devices in that they can  
produce continuous optical signals, and versions based on thin-film amorphous sili-  
con are not restricted by crystal growth limits and so have the potential to be fabri-  
cated in large area format. Sputter-deposited hydrogenated a-Si also has features such  
as excellent adhesion to glass substrates, precise film thickness, and hydrogen content control, which are of some  
interest in device design and fabrication.  
gap of the absorbing material so that a typical silicon-based  
single-crystal device has a maximum response in the region of  
1. Introduction  
1000 nm. Our a-Si devices appear to have an optimal response  
to white light (peakwavelength 690 nm), which corresponds  
to an effective energy gap in the region of 1.8 eV. Light inten-  
sity does not appear to affect the linearity of device output,  
however, the magnitude of the response is directly related to  
the input power while operating below optical saturation. The  
devices, however, appear to lose linearity close to the contacts  
and this is attributed to edge effects related to electric field  
distributions.[4]  
Typical light saturation for silicon-based PSDs is around  
3 W/cm2 and above this figure the photocurrent has a magni-  
tude such that the voltage drop across the sheet resistance is  
so large that it equals reasonable values of reverse bias across  
the device in photodiode mode. At this point the p±n junction  
will be forward biased and hence the PSD no longer functions  
in this mode. Our devices have shown the best linearities in  
photovoltaic mode, with no advantage being gained in photo-  
diode mode implying that we are approaching saturation with  
some of our optical sources. In a photodiode, saturation  
means that the production of photocurrent is saturated and  
can no longer increase with increasing light intensity. This  
leads to an accumulation of charge in the diode which slows it  
down. To remove these charges after the light is turned off, a  
recovery time is required.[5]  
Position-sensitive detectors, or PSDs, comprise an impor-  
tant class of optical sensor, producing an electrical output,  
either voltage or current, which utilizes the lateral photo-  
voltaic effect to give a linear relation between the output and  
the location of a spot of light impinging on a semiconductor  
surface. This phenomenon was first described by Schottky in  
1930[1] and rediscovered by Wallmarkin 1957. [2]  
PSDs are used for a variety of optical applications, such as  
machine tool alignment, medical instrumentation, remote  
optical alignment, robotic vision, and other applications  
requiring precision measurements. Other interesting applica-  
tions include telephone information systems,[3] surface profil-  
ing, angle measurement, rotation monitoring, guidance sys-  
tems, and roles where precise automated control is necessary.  
PSDs are different to photodiode and other device arrays,  
e.g., those formed using charge coupled devices (CCDs), in  
that they can provide continuous information with no internal  
discontinuities.[4] The other advantages of PSDs over CCDs  
are that PSDs have better sampling frequencies (10 MHz to  
10 kHz compared to 2 kHz) and they are cheaper. CCDs have  
the advantage that they are more effective at eliminating the  
effects of stray light.[5]  
The wavelength sensitivity of these devices is, like all semi-  
conductor optical devices, dependent upon the optical energy  
2. Mechanisms of Position-Sensitive Detector  
Operation  
[*] Dr. J. Henry, Dr. J. Livingstone  
Department of Electrical and Electronic Engineering  
University of Western Australia  
35 Stirling Highway, Crawley, W.A. 6009 (Australia)  
E-mail: jasmine@ee.uwa.edu.au  
The simplest model of a PSD is that of a crystal-based  
device with a highly conducting top layer on a lower conduc-  
tivity substrate, with appropriately placed contacts. They can  
Adv. Mater. 2001, 13, No. 12±13, Julyl 4  
Ó WILEY-VCH Verlag GmbH, D-69469 Weinheim, 2001 0935-9648/01/12±1307-01 $ 17.50+.50/0  
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