Antenna effect
Figure 1: Illustration of the cause
of antenna effect. M1 and M2 are the first two metals interconnect layers.
The antenna effect, more formally plasma induced gate oxide damage, is an effect that can
potentially cause yield and reliability problems during the manufacture of MOS
integrated circuits. Fabs normally supply antenna rules, which are rules that
must be obeyed to avoid this problem. A violation of such rules is called an antenna violation. The word antenna is
something of a misnomer in this context—the problem is really the collection of
charge, not the normal
meaning of antenna, which is a device for converting
electromagnetic fields to/from electrical currents. Occasionally the phrase antenna
effect is used in this context, but this is less common since there are
many effects, and the phrase does not make clear which is meant.
Figure 1(a) shows a side view of a
typical net in an integrated circuit.
Each net will include at least one driver, which must contain a source or drain
diffusion (in newer technology implantation is used), and at least one
receiver, which will consist of a gate electrode over a thin gate dielectric
(see Figure 2 for a detailed view of a MOS transistor). Since the gate
dielectric is so thin, only a few molecules
thick, a big worry is breakdown of this layer. This can happen if the net somehow
acquires a voltage somewhat higher than the normal operating voltage of the
chip. (Historically, the gate dielectric has been silicon dioxide, so most of the literature refers to gate oxide damage
or gate oxide breakdown. As of 2007, some manufacturers are replacing
this oxide with various high-κ dielectric materials which may or may not be oxides, but the effect is
still the same.)
Once the chip is fabricated, this
cannot happen, since every net has at least some source/drain implant connected
to it. The source/drain implant forms a diode, which
breaks down at a lower voltage than the oxide (either forward diode conduction,
or reverse breakdown), and does so non-destructively. This protects the gate
oxide.
However, during the construction of
the chip, the oxide may not be protected by a diode. This is shown in figure
1(b), which is the situation while metal 1 is being etched. Since metal 2 is
not built yet, there is no diode connected to the gate oxide. So if a charge is
added in any way to the metal 1 shape (as shown by the lightning bolt) it can
rise to the level of breaking down the gate oxide. In particular, reactive-ion etching of the first metal layer can result in exactly the
situation shown - the metal on each net is disconnected from the initial global
metal layer, and the plasma etching is still adding charges to each piece of
metal.
Leaky gate oxides, although bad for
power dissipation, are good for avoiding damage from the antenna effect. A
leaky oxide can prevent a charge from building up to the point of causing oxide
breakdown. This leads to the somewhat surprising observation that a very thin
gate oxide is less likely to be damaged than a thick gate oxide, because as the
oxide grows thinner, the leakage goes up exponentially, but the breakdown
voltage shrinks only linearly.
Antenna
rules
Antenna rules are normally expressed
as an allowable ratio of metal area to gate area. There is one such ratio for
each interconnect layer. The area that is counted may be more than one polygon
—it is the total area of all metal connected to gates without being connected
to a source/drain implant.
- If the process supports different gate oxides, such as a thick oxide for higher voltages and a thin oxide for high performance, then each oxide will have different rules.
- There are cumulative rules, where the sum (or partial sum) of the ratios over all interconnect layers sets the limit.
- There are rules that consider the periphery of each polygon, as well.
Before signing-off a physical
design/layout for fabrication, the Antenna Rule Check
is therefore performed.
Fixes
for antenna violations
Figure 3: Illustration of three
possible fixes to an antenna violation.
- Change the order of the routing layers. If the gate(s) immediately connects to the highest metal layer, no antenna violation will normally occur. This solution is shown in Figure 3(a).
- Add vias near the gate(s), to connect the gate to the highest layer used. This adds more vias, but involves fewer changes to the rest of the net. This is shown in Figure 3(b).
- Add diode(s) to the net, as shown in Figure 3(c). A diode can be formed away from a MOSFET source/drain, for example, with an n+ implant in a p-substrate or with a p+ implant in an n-well. If the diode is connected to metal near the gate(s), it can protect the gate oxide. This can be done only on nets with violations, or on every gate (in general by putting such diodes in every library cell). The "every cell" solution can fix almost all antenna problems with no need for action by any other tools. However, the extra capacitance of the diode makes the circuit slower and more power hungry.