1192 IEEE JOURNAL OF SOLID-STATE CIRCUITS, VOL. 32, NO. 8, AUGUST 1997
A New Cryogenic CMOS Readout
Structure for Infrared Focal Plane Array
Chih-Cheng Hsieh, Chung-Yu Wu, Senior Member, IEEE, and Tai-Ping Sun
Abstract— A new current readout structure for the infrared
(IR) focal-plane-array (FPA), called the switch-current integra-
tion (SCI) structure, is presented in this paper. By applying
the share-buffered direct-injection (SBDI) biasing technique and
off focal-plane-array (off-FPA) integration capacitor structure,
a high-performance readout interface circuit for the IR FPA is
realized with a pixel size of 50
2
50
m
2
. Moreover, the correlated
double sampling (CDS) stage and dynamic discharging output
stage are utilized to improve noise and speed performance of the
readout structure under low power dissipation. An experimental
SCI readout chip has been designed and fabricated in 0.8-
m
double-poly-double-metal (DPDM) n-well CMOS technology. The
measurement results of the fabricated readout chip at 77 K
with 4 and 8 V supply voltages have successfully verified both
the readout function and the performance improvement. The
fabricated chip has a maximum charge capacity of 1.12
2
10
8
electrons, a maximum transimpedance of 1
2
10
9
, and ae
active power dissipation of 30 mW. The proposed CMOS SCI
structure can be applied to various cryogenic IR FPA’s.
Index Terms—CMOS integrated circuit, cryogenic electronics,
focal plane array, readout circuit.
I. INTRODUCTION
I
N the design of the infrared (IR) focal-plane array (FPA),
high resolution has become a common requirement in many
applications. This leads to large array format and small pixel
size. Due to the small pixel size, it is difficult in the design
of high-resolution large IR FPA’s to implement complex
high-performance readout input circuits (e.g., buffered direct
injection (BDI) [1], [2], capacitive transimpedance amplifier
(CTIA) [3], [4], and chopper-stabilized input circuit (CSI) [5])
with a large enough in-pixel integration capacitor. Usually one
uses a simple readout circuit to maintain a large enough in-
pixel capacitor. Thus, the readout performance (e.g., dynamic
range and signal-to-noise ratio) is degraded. Moreover, the
strict constraint on the unit-cell power dissipation also in-
creases the difficulty to obtain the good readout performance
in a large format IR FPA.
So far, several developed simple current readout schemes
such as the direct injection (DI) [1], [6], [7], the source
follower per detector (SFD) [8], [9], and the gate-modulation
input (GMI) [8], [10], have been developed and have become
commonly used structures in the IR FPA readout chip. In these
Manuscript received August 30, 1996; revised March 6, 1997.
C.-C. Hsieh and C.-Y. Wu are with the Integrated Circuits and Systems
Laboratory, Department of Electronics Engineering and Institute of Electron-
ics, National Chiao Tung University, Hsinchu, Taiwan 300, R.O.C.
T.-P. Sun is with the Chung Shang Institute of Science and Technology,
Lung-Tan, Taiwan, R.O.C.
Publisher Item Identifier S 0018-9200(97)05315-8.
readout schemes, a simple circuit is used to satisfy both pixel
size and power dissipation limitations while sacrificing some
readout performance such as the poor injection efficiency,
the detector bias nonuniformity, and the noise figures. In the
applications of long wavelength infrared (LWIR) detection,
a large integration capacitor is needed because of the large
amount of both background photons and dark currents in the
photodiode. Thus, a large common off-focal-plane integration
capacitor is used in the readout circuit to meet the requirement
while minimizing the chip area [11], [12]. In performing the
signal integration, the conventional multiplexed electronically
scanned array (MESA) [11] is used to select the detector
directly through MOS switches and the direct injection gate
(DIG). In the operation, the inevitable switching noise is easily
coupled to the detector bias. Moreover, using the DIG as a
buffer, it has the constraints on detector bias stability and the
same poor readout performance as in the DI readout circuit.
In this paper, a new current readout structure for the IR
FPA, called the switch-current integration (SCI) structure,
is proposed to solve the above mentioned problems and
improve the readout performance. It has been shown from
both simulation and experimental results that the proposed SCI
readout structure can achieve good readout performance in a
small pixel size through the use of the SCI technique, the off-
FPA shared integration capacitors, and the previously proposed
share-buffered direct injection (SBDI) input circuit [13], [14].
The circuit structure, readout strategy, and circuit performance
of the new SCI readout structure are described in Section II.
In Section III, both simulation results and experimental results
of the fabricated SCI readout chip are presented. Finally, a
conclusion is given.
II. S
WITCH-CURRENT INTEGRATION
(SCI) READOUT STRUCTURE
Fig. 1 shows the block diagram of the proposed SCI readout
structure which is composed of three major parts: the unit-cell
input stage, the shared off-FPA integration capacitor stage, and
the common output stage. The circuit operation is explained
as follows. The photon-generated current in the detector cell is
buffered and switched one row at one time by the vertical row
shift register to the shared off-FPA integration capacitor and
integrated. After an integrating interval, the voltage signal is
sampled, one column after the other by the horizontal column
shift register to the common output stage serially. In the
following, the detailed circuit structure and the operational
principle of each block are described.
0018–9200/97$10.00 1997 IEEE