Semiconductor device manufacturing: process – Making field effect device having pair of active regions... – Having insulated gate
Reexamination Certificate
2001-06-08
2003-11-11
Tsai, Jey (Department: 2812)
Semiconductor device manufacturing: process
Making field effect device having pair of active regions...
Having insulated gate
C438S983000, C438S328000
Reexamination Certificate
active
06645802
ABSTRACT:
FIELD OF THE INVENTION
This invention relates generally to over-voltage protection circuits, and in particular to electrostatic-discharge protection circuits.
BACKGROUND
An electrostatic discharge, or ESD, is a transient discharge of static charge. A familiar example of an ESD is the spark that can occur between a person and a grounded object after the person walks across a carpet. The person acquires a static charge from the carpet; contact with the grounded object allows the static charge to discharge.
The energy associated with an ESD event can easily damage sensitive integrated circuit (IC) components. Protection circuits that can handle the high energies of ESD events are therefore integrated with sensitive IC components so that the protection circuitry can dissipate ESD energy. Typically, a voltage clamp limits the voltage on a selected external IC pin to a level that will not damage ESD-sensitive components. For a discussion of voltage clamps for ESD protection, see Ajith Amerasekera and Charvaka Duvvury, 
ESD in Silicon Intearated Circuits
, pp. 30-52 (1995), and U.S. patent application Ser. No. 09/150,503, entitled “Electrostatic Discharge Protection Circuit,” by Shahin Toutounchi and Sheau-Suey Li, filed Sep. 9, 1998. Both of these documents are incorporated herein by reference.
FIG. 1A
 is a schematic diagram of a conventional silicon-controlled rectifier (SCR) 
100
. SCRs are used extensively to protect ESD-sensitive components. SCR 
100
 is a two-terminal voltage clamp having an anode 
102
 and a cathode 
104
. SCR 
100
 responds to ESD events on anode 
102
 by sinking current to cathode 
104
, primarily via a pair of current paths: a PNP transistor 
106
 and a resistor 
108
 define the first current path; an NPN transistor 
110
 and a resistor 
112
 define the second. SCR 
100
 also includes a zener diode 
114
 connected between the bases of transistors 
106
 and 
110
. Zener diode 
114
 exhibits a reverse-bias breakdown voltage that is low relative to standard diodes. As described below, zener diode 
114
 acts as a trigger element to help turn on transistors 
106
 and 
110
 in response to ESD events on anode 
102
.
Anode 
102
 remains in some active voltage range relative to cathode 
104
 during normal circuit operation. In a typical logic circuit, for example, cathode 
104
 might be grounded (i.e., held at zero volts) and anode 
102
 might transition between zero and five volts or zero and 2.5 volts. Such differences in potential between anode 
102
 and cathode 
104
 are insufficient to turn on zener diode 
114
, so very little current passes through resistors 
108
 and 
112
. As a result, the voltages dropped across resistors 
108
 and 
112
 are normally insufficient to turn on respective transistors 
110
 and 
106
.
An ESD on anode 
102
 can raise the voltage between anode 
102
 and cathode 
104
 well above normal operating levels. Significant increases will exceed the break-down voltage of zener diode 
114
, causing zener diode 
114
 to conduct. The resulting voltages developed across resistors 
108
 and 
112
 will then turn on respective transistors 
110
 and 
106
, thereby sinking ESD current from anode 
102
 to cathode 
104
.
FIG. 1B
 is a graph of an illustrative I-V curve 
116
 for SCR 
100
 (FIG. 
1
A): the x-axis represents the voltage difference between anode 
102
 and cathode 
104
 (i.e., V
A
-V
c
) and the y-axis represents the current I
scr 
through SCR 
100
 between anode 
102
 and cathode 
104
.
In the absence of an ESD (or some other over-voltage event), the anode voltage V
A 
on anode 
102
 remains below the so-called “trigger” voltage V
T 
required to turn on SCR 
100
. The current through SCR 
100
 therefore remains very low. When an ESD raises the anode voltage V
A 
above trigger voltage V
T
, the anode voltage V
A 
will “snap back” to a holding voltage V
H
. Once triggered, SCR 
100
 sinks current from anode 
102
 to cathode 
104
 until most of the energy of the ESD event is dissipated. The trigger voltage V
T 
should be selected to ensure that SCR 
100
 triggers fast enough to avoid damaging any associated ESD-sensitive components (not shown).
Integrated circuits are becoming more complex as device engineers are able to pack more devices on each chip. These improvements are primarily due to advances in semiconductor processing technologies that afford the use of ever smaller circuit features. As features become smaller, reducing junction capacitance becomes increasingly critical to speed performance. One method of reducing junction capacitance involves the use of lower doping levels when forming substrates and well diffusions. Unfortunately, reducing doping levels complicates the task of providing adequate ESD protection.
ESD protection circuits typically include triggering mechanisms that depend upon the breakdown voltage of a selected junction. In general, the breakdown voltage of a given junction is inversely related to doping level. That is, lower doping levels provide higher breakdown voltages. The low well and substrate doping levels preferred for circuits with very small features can increase the breakdown voltage of ESD trigger mechanisms to unacceptably high levels. In modern 0.18-micron processes, the breakdown voltage of trigger mechanisms can approach the breakdown voltage of gate oxides. Consequently, an ESD-protection circuit can fail to trigger in response to an ESD event in time to avoid irreversibly damaging a neighboring gate oxide.
FIG. 1C
 is a cross-sectional diagram of an example of SCR 
100
 that addresses the problem of providing an adequate trigger mechanism for circuits with very small feature sizes. SCR 
100
 is formed on a p-type silicon substrate 
118
 using a conventional CMOS process. SCR 
100
 includes a number of diffusion regions, some of which are isolated from others by isolation regions 
120
. Isolation regions 
120
 are typically silicon dioxide formed using a conventional isoplanar isolation scheme. The diffusion regions include p+ regions 
122
, 
124
, and 
126
, n+ regions 
128
, 
130
, and 
132
, and an n− region 
136
. Of these, p+ diffusion 
126
 is formed within an n-well 
134
. A layer of silicide is divided into areas 
138
 that conventionally establish low-impedance electrical contact to the diffusion regions.
The various components of 
FIG. 1A
 are instantiated in substrate 
118
 as shown. For example, zener diode 
114
 is formed laterally between diffusion regions 
124
 and 
130
. A silicide block 
140
 prevents the zener junction formed between n− diffusion 
136
 and p+ diffusion 
124
 from shorting. Silicide block 
140
 is typically silicon dioxide. The break-down voltage of zener diode 
114
, and therefore the trigger voltage V
T 
of SCR 
100
, depends primarily on the doping concentration of n− diffusion 
136
.
Instantiating zener diode 
114
 laterally, as depicted in 
FIG. 1C
, allows process engineers a degree of flexibility in establishing the breakdown voltage of zener diode 
114
. The breakdown voltage of zener diode 
114
 can be adjusted by selecting an appropriate dopant dose for n− diffusion 
136
. Silicide block 
140
, typically silicon dioxide, then prevents zener diode 
114
 from shorting upon the formation of silicide layer 
138
. Unfortunately, the silicide blocking process is expensive and time consuming. Further, residual oxides from the formation of silicide block 
140
 can contaminate the subsequently formed silicide layers 
138
, and consequently increase their resistance. Finally, providing a sufficiently low breakdown voltage for zener diode 
114
 can be difficult for very dense ICs due to the use of reduced doping levels. There is therefore a need for an improved ESD protection circuit that works well in circuits with very small features and that does not require a silicide blocking process.
SUMMARY
The present invention is directed to a cost-effective ESD protection circuit that is easily integrated with circuits having very small features. One ESD protection circuit in accordance with the invention includes a bipolar t
Gitlin Daniel
Hart Michael J.
Li Sheau-Suey
Toutounchi Shahin
Wu Xin X.
Behiel Arthur J.
Tsai Jey
Webostand W. Eric
Xilinx , Inc.
Young Edel M.
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