J. Cent. South Univ. Technol. (2011) 18: 744−748
DOI: 10.1007/s11771−011−0757−8
Analysis and simulation of lateral PIN photodiode gated by
transparent electrode fabricated on fully-depleted SOI film
XIE Hai-qing(谢海情), ZENG Yun(曾云), ZENG Jian-ping(曾健平), WANG Tai-hong(王太宏)
School of Physics and Microelectronics Science, Hunan University, Changsha 410082, China
© Central South University Press and Springer-Verlag Berlin Heidelberg 2011
Abstract: A novel device, lateral PIN photodiode gated by transparent electrode (LPIN PD-GTE) fabricated on fully-depleted SOI
film was proposed. ITO film was adopted in the device as gate electrode to reduce the light absorption. Thin Si film was fully
depleted under gate voltage to achieve low dark current and high photo-to-dark current ratio. The model of gate voltage was obtained
and the numerical simulations were presented by ATLAS. Current−voltage characteristics of LPIN PD-GTE obtained in dark (dark
current) and under 570 nm illumination (photo current) were studied to achieve the greatest photo-to-dark current ratio for active
channel length from 2 to 12 µm. The results show that the photo-to-dark current ratio is 2.0×10
7
, with dark current of around
5×10
−4
pA under V
GK
=0.6 V, P
IN
=5 mW/cm
2
, for a total area of 10 µm×10 µm in fully depleted SOI technology. Thus, the LPIN
PD-GTE can be suitable for high-grade photoelectric systems such as blue DVD.
Key words: lateral PIN photodiode; transparent electrode; physical model; photo-to-dark current ratio; silicon-on-insulator
1 Introduction
Nowadays, short distance optical communications
and optical storage (OS) systems such as blue DVD
require fast (gigahertz to tens of gigahertz bandwidth)
and responsive photodetectors with high photo-to-dark
current ratio increasingly [1−2]. Bulk silicon detectors,
however, hardly cope with these specifications, mainly in
regards to bandwidth, and nonintegrated detectors are
usually used due to high dark currents of photodiode and
low sensitivity of MOS structure (due to only one kind of
carrier and light-absorption of gate) in CMOS process
less than 0.25 µm [3−6]. The ultimate performances of
optical receiver circuits are limited because of high
bonding capacitor, cost and area, which is a limitation for
the employment in local-area networks, inter-chip/
intra-chip interconnects, and Ethernet [7−8].
Lateral PIN photodiode on SOI has been the focus
for extensive research over the past decade due to its
high responsivity and quantum efficiency [9−10].
However, high reverse bias needs to be used in this PIN
photodiode to achieve a low capacitance and high
sensitivity. In addition, it is not propitious to integration
for the small input resistance [11]. In the modern
microelectronic integration industry, MOS is the
fundamental ingredient since it has large input resistance,
low noise and wide spectrum range [12−13].
In order to achieve low dark current and high photo
current under low reverse voltage, lateral PIN
photodiode gated by transparent electrode (LPIN
PD-GTE) based on partially depleted (PD) SOI film
compatible with CMOS process was proposed recently
[14]. The structure of LPIN PD-GTE is very similar to
traditional MOS structure, but only ITO is applied as
gate to reduce the light absorption. In the previous work,
a physical model was presented based on standard
semiconductor equations under partial depletion. The
numerical calculation indicated that LPIN PD-GTE has
high sensitivity and signal to noise ratio (SNR). In this
work, the characteristics of LPIN PD-GTE fabricated on
FD SOI substrate are focused on.
2 Device structure
Thin film SOI LPIN PD-GTE was realized in the
FD SOI CMOS technology with the parameters shown in
Fig.1. The thickness of thin Si film, d
Si
, is equal to
200 nm; the thickness of the front oxide, d
FOX
, is equal to
20 nm; the thickness of the buried oxide (BOX), d
BOX
, is
equal to 380 nm; the thickness of substrate, d
sub
, is equal
to 500 nm. The length of N
+
and P
+
zones, L
PN
, is equal
to 1 μm and different L values, the length of the channel
typically corresponding to a P
−
-doping of 10
15
cm
−3
, of 2,
4, 6, 8, 10 and 12 μm are selected.
The absorption in ITO film is the main loss of
Foundation item: Project(61040061) supported by the National Natural Science Foundation of China; Project supported by Hunan Provincial Innovation
Foundation for Postgraduate Students, China
Received date: 2010−01−31; Accepted date: 2011−01−05
Corresponding author: ZENG Yun, Professor; Tel: +86−731−88822332; E-mail: zengyun@hnu.cn