3dintegquarter.doc

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3-D Integration Project Quarterly Report
Neil Goldsman, Zeynep Dilli
1. Overview
We designed and submitted two chips to the MOSIS fabrication service in June 2002 and
one in October 2002. The first chip used AMI Semiconductor’s 1.6 m feature size
technology, AMI ABN (lambda=0.8). The other two chips used the 0.6 m technology,
AMI C5N/F (lambda=0.3). The first two chips had similar structures on them to examine
the detrimental effect of bonding pads and pins on circuit performance and possibly to
conduct some interference tests. The third chip has been designed with post-fabrication
processing in mind, to integrate pairs of this chip vertically.
For the first two chips, we ordered two packaged and three unpackaged chips. For the
last run, we ordered one packaged and four unpackaged chips.
The circuitry on the chips, to be detailed below, consist of specially designed ring
oscillators, supporting test and on-chip built-in diagnostic structures, and 3-D integration
structures.
Using structures on the first 0.6 micron chip, we have demonstrated that the need to go
out to the PCB and come back on chip impedes circuit performance considerably
compared to a simple planar circuit. With our work on the new 0.6 micron chip,
expected back from fabrication in December, we hope to demonstrate that threedimensional integration will demonstrate comparable performance to a planar circuit and
a marked improvement over the speed of a signal-goes-out-of-chip type circuit.
The full layout for the 1.6 m chip is shown in Figure 1. The layout for the first 0.6 m
chip is shown in Figure 2, and for the second one, Figure 3.
Figure 1
The 1.6 m
technology chip sent
out for fabrication in
June 2002.
Figure 2
The 0.6 m
technology chip sent
out for fabrication in
June 2002.
Figure 4
The 0.6 m technology chip sent out for fabrication in October 2002.
2. Ring Oscillator Structures and Counters
In conventional circuit design that requires the functionality of more than one
commercially available integrated circuits, the communication through the circuits are
usually handled by the connection chain of circuit  bonding pad  bonding wire 
pin  PCB line  pin  bonding wire bonding pad  circuit. This arrangement adds
significant parasitic capacitance and inductance to the communication link, and has
detrimental effects on both circuit speed and power dissipation. Moreover, the need to
drive the large capacitance of bonding pads (this is large relative to in-chip capacitances)
requires large-transistor “buffer”s, usually a chain of progressively larger inverters, as the
last stage of any circuit component that has to have an output to the outside world, which
wastes real estate on chip and adds delay to the output stages of circuits.
To observe these effects in a circuit whose behaviour is simple and easily quantifiable,
we have designed and laid out basic ring oscillators for each of the three chips. In the
June 2002 ABN and C5N chips, there were two types ring oscillators laid out for these
purposes. The first ones were “internal”, or planar, ring oscillators, formed by directly
connecting the output of and inverter to the input of the next one. The 1.6 m and 0.6
m oscillators had 19 and 31 stages, respectively. The simulated operation frequencies
for these inverters were 63.3 MHz for the first chip and 132.45 MHz for the second.
The 0.6 m inverter is depicted in Figure 4.
Figure 4 The 31-stage ring oscillator comprised of minimum-size transistor in the 0.6 m
technology June chip.
The output stages of these ring oscillators are connected to frequency-divider-setup
counters in both chips. These counters serve a dual purpose. First is to reduce the
frequency of the output of the ring oscillators, and thus, aiding the ease of measurement.
The second is to avoid loading the output stages of the ring oscillators directly by the
bonding pad, wire, and probe capacitances, for a better comparison with the external ring
oscillator operation, to be described below. Thus these counters serve as on-chip test
structures.
The June 1.6m chip carried a 4-bit counter made of T-flip flops. The 0.6m chips carry
6-bit counters made of D-flip flops. The D-flip flop design and layout are given in
Figure 5; the schematic of the 6-bit counter is given in Figure 6.
Figure 5 Design
and 1.6 m layour of
a D-flip-flop.
Figure 6. Schematics for a 6-bit D-ff counter.
The second type of ring oscillator present in the June chips were “external” ring
oscillators, which are individual inverters getting their input from one bonding pad and
sending their output to another pad. This way, there would be two bonding pads (and the
out-of-the-chip connection chain) between each stage of the ring oscillator when these
inverters are linked externally to form it. On the layouts of these chips, in Figures 1 and
2, these inverters can be seen as lining the left side of the layout, going from the ground
pin to the Vdd pin.
The results obtained from the 0.6 m chip, measured on a breadboard using the 1-pF
input capacitance active probe from Tektronix, are as follows:
Internal Osc.
External Osc.
One-stage delay
112 MHz (31-stage)
398 KHz (11-stage)
~330 ps for internal, ~330
(equivalent to 1.16 GHz for (equivalent to 1.46 MHz for ns for external devices
3 stages)
3 stages)
Thus we can observe that going through the out-of-chip connection chain slows down
the circuit by about 800-fold.
The 11-stage external ring oscillator of the 1.6 m chip ran at 732.7 kHz on a PCB
measurement with the active probe. It would run at 278 kHz on the breadboard with a
25-pF input capacitance BNC probe. In these measurements, in an effort to determine
which part of the capacitive effect arose from the breadboard itself, a capacitive load vs.
rise/fall/delay times table was created with additional load capacitances inserted between
the output of an inverter and the ground on the breadboard. Using this table and
extrapolating, it is possible to deduce that the load capacitance of the bonding
pad+bonding wire+pin+breadboard+active probe ensemble is about 15 pF. The probe is
claimed to have 1 pF load. For the pad itself, Cadence extracts a capacitance of 0.24 pF,
however, this does not include the capacitances of the quite large ESD protection
transistors. We have planned to repeat this experiment using the PCB to deduce the
capacitance of the pin-PCB line connection chain. We could not get a meaningful result
out of the internal ring oscillator of the 1.6 m chip.
In the October chip, we once again implemented the 31-stage internal ring oscillator with
the 6-bit counter as its output stage. However, we also implemented a structure that will
be post-fabrication processed into a 3-D ring oscillator. This structure, shown Figure 7,
consists of six groups of inverters (five with five and one with six inverters each) placed
deliberately around the symmetry axis of the layout so that when two chips made from
this design are taken together, one is flipped over and placed over the other, with the
correct connections these inverters will form a ring oscillator. The output of this
oscillator also goes to a 6-bit counter.
Figure 7 Three-dimensional ring
oscillator. The proper pairs of pads,
visible as light blue squares in the
figure, have to be connected to each
other through vertical through-chip vias
post-fabrication for the circle to close.
The output of the oscillator goes to a 6bit counter through an inverter, visible
in the lower right corner of the figure.
The 3-D bonding pads used in this structure are comprised of three layers of metals,
connected with vias, squares with 12 m sides. Their to-substrate capacitance is of the
same order of magnitude as the input capacitance of a minimum size inverter in this
technology. Therefore, while the 3-D ring oscillator formed this way is expected to be
slower than the full planar oscillator, we do not expect a great detrimental effect to speed.
Moreover, we expect the performance of this oscillator to be better than the external
oscillators of the June chips.
3. Other Structures on the June chips
Small Counters The 1.6 m chip houses two small, 2-bit counters in independent
frequency-divider configurations. These counters have the exact same design and
schematic, but slightly different layouts. The difference lays in the compactness of the
layout and the path traversed by the clock signals. Feeding them with identical count
signals, we investigated possible differences in performance. Measurements on a PCB
with the active probe yielded the following results:
Counter A
Counter B
Rise time (ns)
Fall time (ns)
tPLH (ns)
tPHL (ns)
50.51
37.44
69.09
62.21
27.5
37
72
61
There is, therefore, a measurable difference in operation arising from layout differences
alone. The exact effects taking place are still under investigation.
Pn-junctions Both chips had an p+/n-well diode built in to be tested. This is one of the
possible diode configurations that can be used while laying out an optical detector cell or
a pixel in conventional CMOS technology. Rectification was observed, with the
characteristic diode IV curves, for both.
Large inverters Both chips had “reality-check” inverters laid out independently from the
external ring oscillator inverters, with somewhat larger feature sizes. These inverters
were tested operational for both designs, with rise and fall times smaller than the
minimum-size inverters’ times for the corresponding technology, as could be expected
from their higher current-driving capabilities.
Crosstalk measurement setup On the 0.6 m chip, two D-flip flops sharing the same
clock signal are connected in a two-stage latch configuration (the Q output of the first one
to the D input of the other). The connection between them is a rather long and snaking
metal1 line, as can be observed in Figure 8. Winding along with this line is an input line
for an ordinary inverter, shown in the figure below the two flip-flops. This circuit is
designed to observe possible fluctuations in the data line between the two flip-flops when
an input signal is applied to the inverter, with the possibility that the second ff might latch
an incorrect value. Test work is still under progress.
Figure 8 Crosstalk measurement layout on the 0.6 m chip.
4. Other structures on the October chip
“External” ring oscillator This layout features a three-stage ring oscillator, close to the
top edge of the die to the right of the Vdd pad, that is similar to the external ring
oscillators of the previous chips in that the bonding pads still load the inverters that form
its stages. However, in this oscillator the connections between the inverters are direct and
internal, with the bonding pads serving as only loads, not connection stages. This
structure aims at measuring the effect of the bonding pads more isolated from those of the
other stages of the out-of-chip connection chain. This structure is displayed in Figure 9.
Figure 9 “External” ring oscillator; three stages. The connectors to the bonding
pads are visible on the edges of the figure.
XOR with output buffer An XOR gate is useful in applications that require measuring
the relative phases of two signals or testing if two signals are identical. We designed,
simulated and laid out an XOR gate for use in such measurements in the future. For this
XOR to drive the extra capacitance of the bonding pad, through which its output will be
measured, a four-stage buffer comprising of progressively larger inverters was connected
to its output. This structure is visible close to the lower right corner of the chip.
Phase delay measurement setup These are two pairs of inverters whose outputs are sent
to corresponding XOR gates. In both pairs, the input paths to the inverters from bonding
pads are nearly equal. In one pair, the paths from the outputs of the inverters to the
inputs of the XOR are also equal. In the other, one path meanders, adding an extra
distance to the signal path approximately equal to that added to the 3-D ring oscillator
with signals going to and coming back from the connector pads. The XORs, once more
buffered with progressively larger inverters to their outputs at bonding pads, will detect
the phase difference between these two paths. This structure is placed on the bottom left
corner of the chip and depicted in Figure 10.
Figure 10 Signal delay measurement setup. The signal paths to the XOR input in the
top structure are equal. One signal path is longer than the other in the second structure.
More 3-D circuits At the top part of the layout, two D-flip flops are laid out
symmetrically so as to be connected in three dimensions in a 2-bit counter setup. Right
below that, identical flip flops are connected into a planar 2-bit counter. To the right and
left of this counter there are two inverters with 3-D connection pads furnished at input
and output for the creation of a 3-D buffer. To the right, there is a single planar buffer.
These structures are for the purposes of performance comparison.
Large NMOS Close to the bottom right corner of the chip, there is a NMOS 10 times the
minimum size (W=150 m, L=60m). The source is shorted to the body, which is at
ground level, as with all digital NMOSes on the chip. The gate and drain are connected
to bonding pads. We hope to conduct gate noise measurements with this FET.
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