Electronic digital logic circuitry – Signal sensitivity or transmission integrity – Bus or line termination
Reexamination Certificate
2003-03-13
2004-06-08
Tokar, Michael (Department: 2819)
Electronic digital logic circuitry
Signal sensitivity or transmission integrity
Bus or line termination
C326S031000, C326S034000, C326S082000, C326S083000, C326S086000
Reexamination Certificate
active
06747476
ABSTRACT:
BACKGROUND OF THE INVENTION
1. Field of the Invention
The present invention relates to termination circuits and methods therefor. More particularly, the present invention relates to termination circuits that provide fast and efficient clamping for signals transmitted via transmission lines in electronic systems.
2. Description of Relevant Art
In the design and implementation of electronic systems (such as digital computers, consumer/commercial electronic devices, or the like), particularly those employing integrated circuits, undesired transmission line effects are of a particular concern. As signals travel down transmission lines, e.g., traces on a printed circuit board, reflections may occur on the lines. The reflections are due to, for example, mismatched impedances between the receiver circuit and the line, which may cause the signal to reflect back and forth, giving rise to ringing. These reflections and other undesired transmission lines effect are exacerbated as the operating speed of the signal increases. If left uncorrected, the reflections may cause the signal's voltage to swing outside of the defined “0” or “1” voltage levels, thereby causing the receiving device to incorrectly interpret the signal received and generate erroneous results.
To address this problem, a variety of techniques have been tried in the prior art. One such technique is shown in 
FIG. 1
 illustrating a termination circuit 
100
 includes a top active clamping device 
102
 and a bottom active clamping device 
104
. In the circuit 
100
, the top active clamping device 
102
 is implemented by a p-channel MOS device 
132
 and serves to clamp the signal on a transmission line 
106
 at about a second reference voltage (e.g., V
DD
). On the other hand, bottom active clamping device 
104
 is implemented by an n-channel MOS device 
120
 and serves to clamp the signal on transmission line 
106
 at a first reference voltage (e.g., ground or GND). In accordance with the convention utilized herein, the top devices are employed to clamp the voltage level of the signal on the transmission line at its upper range (e.g., to about V
DD
), while the bottom devices are employed to clamp the voltage level of the signal at its lower range (e.g., to about ground).
The source of MOS device 
132
 can be coupled to V
DD 
while the source of MOS device 
120
 can be coupled to ground. The drains of devices 
132
 and 
120
 are both coupled to transmission line 
106
 as shown. Referring now to bottom active clamping device 
104
, a gate 
114
 of MOS device 
120
 is coupled to both the gate and drain of a bottom threshold reference device 
113
 having an input impedance r
1
. As shown in 
FIG. 1
, bottom threshold reference device 
113
 includes an n-channel MOS device 
118
, which is arranged in a gate-to-drain connected configuration.
When sufficient current flows into the drain of n-channel MOS device 
118
 the current may be sourced from any conventional current sourcing arrangement, which is shown symbolically by current source 
116
 in FIG. 
1
), gate 
114
 of bottom active clamping device 
104
 is biased at about one threshold voltage V
T 
of n-channel MOS device 
118
 above ground. Typically, the voltage at gate 
114
 is biased at the threshold voltage V
T 
of n-channel MOS device 
118
 plus a small amount of overdrive voltage necessary to sustain the current through device 
118
.
When the signal on transmission line 
106
 begins to reflect and dips below ground, i.e., as soon as the potential difference between the gate of n-channel MOS device 
120
 of bottom active clamping device 
104
 and its source exceeds V
T
, n-channel device 
120
 begins to conduct to source current from its drain, which is connected to ground as shown in FIG. 
1
. Accordingly, the signal is clamped at about or slightly below ground. As noted, gate 
114
 of n-channel device 
120
 is typically biased slightly above V
T
. Consequently, it is typically the case that n-channel device 
120
 begins to conduct when the signal on transmission line 
106
 is slightly above ground (e.g., perhaps 0.1 V above ground). In this manner, n-channel device 
120
 would be in full conduction when the signal on transmission line 
106
 dips below ground.
A similar arrangement exists with reference to gate 
130
 of the p-channel MOS device 
132
 of top active clamping device 
102
 in that the gate 
130
 of MOS device 
132
 is coupled to both the gate and drain of a top threshold reference device 
111
 having an input impedance r
2
. More particularly, the gate 
130
 is coupled to the gate and drain of p-channel MOS device 
134
. The source of p-channel MOS device 
130
 is coupled to V
DD 
as shown. When sufficient current flows out of the drain of p-channel device 
134
, gate 
130
 of p-channel device 
132
 is biased at about V
DD
-V
T
, where V
T 
is the threshold voltage of p-channel MOS device 
134
. Actually, gate 
130
 of p-channel device 
132
 is biased slightly below this value (V
DD
-V
T
) due to the presence of the overdrive voltage necessary to sustain current through p-channel MOS device 
134
.
When the signal on transmission line 
106
 begins to reflect and rises above V
DD
, p-channel MOS device 
132
 turns on to clamp this signal at about V
DD
. Due to the presence of the aforementioned overdrive voltage, p-channel MOS device 
132
 typically turns on slightly before the voltage level of the signal on transmission line 
106
 reaches V
DD
, thereby ensuring that p-channel MOS device 
132
 is fully turned on when the signal's voltage level exceeds V
DD
.
As well known in the art, all junction type devices (including transistors) have intrinsic capacitance loading between the various junctions commonly referred to as parasitic capacitance. One such parasitic component particularly relevant to the inventive termination circuit are referred to as MOSFET capacitances. These parasitic components are mainly responsible for the intrinsic delay of logic gates. 
FIG. 2
 illustrates a typical MOSFET 
200
 having associated junction parasitic capacitances represented as lumped elements between the device terminals. Based on their physical origins, the parasitic device capacitances can be classified into two major groups: (1) oxide-related capacitances and (2) junction capacitances. In the example shown, the gate-oxide-related capacitances are Cgd (gate-to-drain capacitance), Cgs (gate-to-source capacitance), and Cgb (gate-to-substrate capacitance). It is well known in the art that the gate-to-channel capacitance is distributed and voltage dependent, and consequently, all of the oxide-related capacitances described here changes with the bias conditions of the transistor. Note that the total gate oxide capacitance is mainly determined by the parallel-plate capacitance between the gate and the underlying structures. Hence, the magnitude of the oxide-related capacitances is very closely related to (1) the gate oxide thickness, and (2) the area of the MOSFET gate.
Referring back to 
FIG. 1
, the gate to drain parasitic capacitance C
gd1 
(associated with transistor 
132
) and C
gd2 
(associated with transistor 
120
) degrade the clamping performance of the termination circuit 
100
 by causing the gate voltages of the clamping transistors 
132
 and 
120
 to vary in relation to the input voltage rise or fall on the transmission line 
106
. In some cases, this variation in gate voltage can be hundreds of millivolts.
In addition to the presence of the parasitic capacitances C
gd1 
and C
gd2 
that degrade the clamping performance of the termination circuit 
100
, DC power in excess of that required by the current source 
116
 is dissipated due to what is referred to as the short channel effect. Currents I
p 
and I
n 
are always flowing in the bias voltage generator circuits 
111
 and 
113
, respectively. However currents that may be an order of magnitude greater than bias currents I
p 
and I
n 
can flow in the clamping transistors when there exists both a voltage between the source and drain of greater than a threshold voltage, and also a voltage between the source
California Micro Devices
Eakin James E.
Nguyen Khai
Tokar Michael
LandOfFree
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