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2Device scaling laws
3Interconnect scaling laws
4Example Al and oxide technology
- Typical scaling factor over 4 years are
- S0.6, f2, D1.3,
- Since the metal and the dielectric materials are
the same - rloc2/3, r1, k1.
- The intrinsic gate delay drops by a factor of 0.6
- The local interconnect delay drops by 2/3
- The global interconnect delay increases by
krD2/S24.69
5Example Switching to Cu and low-k technology
- Typical scaling factor over 4 years are
- S0.6, f2, D1.3,
- The metal and the dielectric materials have been
changed, - The local interconnect technology has not
changed - rloc2/3, r1/2, k1/2.
- The intrinsic gate delay drops by a factor of 0.6
- The local interconnect delay drops by 1/3
- The global interconnect delay increases by
krD2/S21.17
6The signal propagation effect
- The signal can not propagate faster than the
speed of the electromagnetic wave Vc
- The speed of the electromagnetic wave Vc is
proportional to 1/(LC)1/2
The inductance L is constant while the
capacitance is proportional to k. Therefore
7Effect of scaling on Timing
- Clock frequency increases
- The global interconnect delay becomes dominant
- Coupling capacitance becomes important
- Inductance becomes an issue
- Clock skew variations limits the clock frequency
8Gate and Interconnect delays
9Effect of scaling on noise
1. Cross talk - signal propagation to neighboring
wires 2. Simultaneous switching noise on the
power line 3. Charge sharing effects - affects
mostly dynamic logic 4. Leakage current - affects
DRAM and switch capacitor filters.
10Effect of scaling on the power
1. Higher frequency - higher power dissipation
(P) 2. Lowering VDD is a solution - limited by
noise margins. 3. Higher capacitance increases
P 4. Lowering threshold improves margins but
increases the leakage current 5. Higher CMOS
transition current and dissipation
11Effect of scaling on the reliability
1. Higher power per unit area --gt higher working
temperature 2. Higher current density --gt higher
electromigration 3. Higher interconnect stress
levels --gt stress voiding
12Interconnect models
Rr L/A
At higher frequency the skin effect reduces the
interconnect cross section. The skin depth, d, is
defined by the penetration distance at which the
current density drops by 1/e
Where f is the frequency, r is the resistivity
and m is the magnetic permeability
13Interconnect models
Ce0er A/d
Inductors are more difficult to calculate. Some
models will be described I the next lecture.