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3. Advanced Rules & Models

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Presentation on theme: "3. Advanced Rules & Models"— Presentation transcript:

1 3. Advanced Rules & Models
Etienne Sicard

2 Summary New design rules MOS models (Model 1, 3, bsim4)
Interconnect model Crosstalk model Conclusion

3 1. New design rules By default salicide deposit
Low resistance N+,P+ and poly surface Removing salicide increases the resistance Protect from Salicide Default salicide deposit

4 1. New design rules Lateral Drain diffusion prevents hot carrier damage Hot carriers degrade Vt, IdSat (10% less than 1 year without LDD) ESD is improved without LDD LDD

5 1. New design rules During fabrication, plasma etching charges metal lines Charges degrade MOS Vt, or damage oxide Charges must be eliminated to the substrate Charges accumulated Gate damage Antenna ratio = Area (metal)/Area(gate) Do It Solution: Add diodes

6 Measured 10x10µm in 0.35µm ST (hcmos6)
2. MOS model Measured 10x10µm in 0.35µm ST (hcmos6) The MOS model 1 works fine in 0.35µm (Shockley, 1950) Scoop

7 MOS model 1 gives 150% error for L=0.35µm
Sad, sad 10x0.4 µm in 0.35µm ST (hcmos6) MOS model 1 gives 150% error for L=0.35µm (Shokley, 1950) No MOS level 1 in design rule manuals

8 2. MOS model Measure simulation
MOS level 3 includes short channel limitation effects MOS 3 is considered obsolete starting 0.5µm, but is still in used for first-order estimations

9 2. MOS model BSIM3v3 Berkeley New BSIM4
MOS Model 9 « MM9 » (ST, Philips) Soon stopped 20 Basic parameters 60 secondary parameters 120 fitting parameters

10 2. MOS model BSIM4 threshold model Berkeley Vth (V)
Short channel effects Channel length (µm)

11 2. MOS model BSIM4 threshold model Berkeley Ids Ids (Log) Vgs (V)
Vds (V)

12 2. MOS model Poor fit Width (µm) Reference Output pad Good fit
100.0 Reference Output pad 10.0 Good fit Length (µm) 1.0 0.0 2.5 5.0 7.5 10 The MOS model is reliable within its optimized range

13 2. MOS model Around 200 parameters Model gourous
Model is becoming a service Achieve good fit with static measurements using a wide set of tricks and internal arrangements

14 2. MOS model Layout W=100µm L=0.25µm in a square area?

15 2. MOS model Shielded MOS, for mixed signal applications 2D view
VSS 2D view

16 3. Interconnect Model C (F/m)= e0 er w/h Capacitance e0=8.85e-12 F/m
w=1µm e=1µm w Capacitance(aF/µm) e Total 1000 h 100 Plane 10 0.01 0.1 1.0 Fringing effects are comparable to area

17 C11= 0.r *(1,13*w/h+1.443(w/h)^0,11+1.475 (t/h)^0.425)
3. Interconnect Model Formulation in CAD tools based on 2D solvers Sakurai formulas Delorme formulas Page C11= 0.r *(1,13*w/h+1.443(w/h)^0, (t/h)^0.425)

18 3. Interconnect Model Resistance

19 3. Interconnect Model Simple line model Very short interconnect
Medium interconnect Long interconnect No precise info in DRM, still research

20 3. Interconnect Model Measurement/Simulations 5mm Voltage Near end
Far end Time (ns) CRC model fits well in 0.25µm (hcmos7)

21 3. Interconnect Model Al 0.35 µm 0.18µm 0.7 µm Cu Al 3Rx3C=9RC (680ps)
Volt Volt 2 1 3 Volt 4 5 1 3 2 0.5 1.5 1 2 0.35 µm 0.18µm 0.7 µm Cu Al Al 0.5 1.0ns 0.25 0.75 1.0 1.5ns 0.5 1 2 3ns 3Rx3C=9RC (680ps) Repeaters help to propagate signals at long distance 3mm 3RC+2tgate (380ps) 1mm 1mm 1mm

22 3. Interconnect Model Technology Gate delay (ps) Gate delay Aluminium
Copper 0.12µm 500 1000 1500 Gate delay (ps)

23 4. Crosstalk Effects Rising importance of coupling capacitance 0.7 µm
New parameters in DRM

24 4. Crosstalk Effects 4000µm 2200µm Critical routing length 0.25µm
Crosstak (V) 4000µm 2200µm Length (µm)

25 4. Crosstalk Effects Coupled line model Short coupled interconnects
Long coupled interconnects Used for investigating crosstalk

26 4. Crosstalk Effects Generation Probable Fault Fault Noise/VDD (%)
Alu SiO2 0.70µm Probable Fault 0.50µm Fault 0.35µm 0.25µm Cu Low K 0.18µm Noise/VDD (%) 0.12µm 25% 50% 75% 100% Crosstalk is a major signal integrity challenge

27 Conclusion Specific technological options described
Complex MOS models are mandatory BSIM3v3, soon BSIM4 Interconnect is the main delay limiting factor A C/R/C model is accurate for simulating signal transport Crosstalk is a major signal integrity challenge


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