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Capcitive Parasitics
Presented By:
Niaz Shaikh
Instructor:
Engnr. Suresh Kumar
Agenda
• Wire parasitics.
• Capacitive parasitics.
 Diffusion wire capacitance.
 Depletion region capacitance.
• Poly/metal wire capacitance.
• Fringing Capacitance.
• Metal coupling capacitances.
Wire parasitics
• Wire and vias introduce parasitic elements in
our circuits.
• It is important to understand the structural
properties of our components that introduce
parasitic elements, and how to measure
parasitic element values from layouts.
Capacitve parasitic
Diffusion wire capacitance
• Capacitances formed by p-n junctions
Total Capacitance= sidewall capacitances+Bottom Wall Capacitance
n+ (ND)
depletion region
substrate (NA)
bottomwall
capacitance
sidewall
capacitances
Typical 0.5 micron process Diffusion wire
capacitance values:
• n-Type:
Bottomwall: 0.6fF/µm^2
Sidewall: 0.2fF/µm
• p-Type:
Bottomwall: 0.9fF/µm^2
Sidewall: 0.3fF/µm
In 0.5micron process , Lambda=0.25µm
Diffusion wire capacitance (cont:)
• An accurate measurement of diffusion wire
capacitance requires separate calculations for
the bottom and sides of the wire---the doping
density, and therefore the junction properties
, vary with depth.
• To measure total capacitance, we measure the
diffusion area, called bottom wall capacitance,
and perimeter, called side wall capacitance, as
shown in Fig:, and sum the contribution of
each.
Capcitive parasitics in mos
Depletion region capacitance
• Zero-bias depletion capacitance:
– Cj0 = si/xd. :- = 8.854×10−12 F/m
• Depletion region width (zero biased):
– xd = sqrt[2siVbi(1/NA + 1/ND) /q].
• Junction capacitance is function of voltage across
junction:
– Cj(Vr) = Cj0 *(1 - Va/Vbi)^-m
– m is a constant ranges from 0.3 to 0.5
• Junction capacitance
decreases as the reverse bias
voltage increases.
• Cdiff=Cjo*WL+Cjo*h*(2L+W)
Poly/metal wire capacitance
The capacitance mechanism for poly and
metal wires is, in contrast, the parallel plate
capacitance.
We take into account the changes in the
electrical field at the edges of the plate by
adding in a fringe capacitance per unit
perimeter.
These two capacitances are illustrated in Fig:
Capacitances can form between signal wires.
Poly/metal wire capacitance
• Two components:
–parallel plate;
–fringe.
plate
fringe
Fringing Capacitance
• Fringe capacitance is formed between non-overlapping sidewall of
one conductor and surface/sidewall of a second conductor on the
same or different layer from the first one.
• This type of capacitance becomes significant as we route in higher
layers because higher layers are thicker.
Fringing Capacitance
W - H/2H
+
(a)
(b)
Typical Poly/Metal Capaciatnce values for 0.5
micron process
• Poly: Metal2:
 plate: 0.09fF/µm^2 plate: 0.02fF/µm^2
 fringe: 0.04fF/µm fringe: 0.06fF/µm
• Metal1: Metal3:
 plate: 0.04fF/µm^2 plate: 0.009fF/µm^2
 fringe: 0.09fF/µm fringe: 0.02fF/µm^
Metal coupling capacitances
• Can couple to :
 adjacent wires on same layer,
 wires on above/below layers:
• Orthogonal Wires in Different Layers:
 Reduction of coupling capacitance between Layers
metal 2
metal 1 metal 1
Cm1m2
Cw1w2
Example: parasitic capacitance measurement
• n-diffusion: bottomwall=2 fF, sidewall=2 fF.
• metal: plate=0.15 fF,
fringe=0.72 fF.
3 m
0.75 m
1 m
1.5 m
Metal coupling capacitances
 As the number of metal levels increases and the substrate capacitance
decreases, wire-to-wire parasitics are becoming more important.
 Both capacitance between two different layers and between two wires on
the same layer are basic parallel plate capacitances.
 The parasitic capacitance between two wire on different layers, such as
Cm1m2 in Fig:, depends on the area of overlap between the two wires.
 The capacitance between two wires on the same layer, Cw1w2 in the Fig:, is
formed by the vertical sides of the metal wires.
 When two wires on the same layer run in parallel for a long distance, the
coupling capacitance can become very large.
18
Parastic Elements
• So far, we’ve concentrated on getting circuit
elements that we want for digital design
–Transistors
–Wires
• Parasitics - occur whether we want them or
not
–Capacitors
–Resistors
–Transistors (bipolar and FET)

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Capcitive parasitics in mos

  • 1. Capcitive Parasitics Presented By: Niaz Shaikh Instructor: Engnr. Suresh Kumar
  • 2. Agenda • Wire parasitics. • Capacitive parasitics.  Diffusion wire capacitance.  Depletion region capacitance. • Poly/metal wire capacitance. • Fringing Capacitance. • Metal coupling capacitances.
  • 3. Wire parasitics • Wire and vias introduce parasitic elements in our circuits. • It is important to understand the structural properties of our components that introduce parasitic elements, and how to measure parasitic element values from layouts.
  • 5. Diffusion wire capacitance • Capacitances formed by p-n junctions Total Capacitance= sidewall capacitances+Bottom Wall Capacitance n+ (ND) depletion region substrate (NA) bottomwall capacitance sidewall capacitances
  • 6. Typical 0.5 micron process Diffusion wire capacitance values: • n-Type: Bottomwall: 0.6fF/µm^2 Sidewall: 0.2fF/µm • p-Type: Bottomwall: 0.9fF/µm^2 Sidewall: 0.3fF/µm In 0.5micron process , Lambda=0.25µm
  • 7. Diffusion wire capacitance (cont:) • An accurate measurement of diffusion wire capacitance requires separate calculations for the bottom and sides of the wire---the doping density, and therefore the junction properties , vary with depth. • To measure total capacitance, we measure the diffusion area, called bottom wall capacitance, and perimeter, called side wall capacitance, as shown in Fig:, and sum the contribution of each.
  • 9. Depletion region capacitance • Zero-bias depletion capacitance: – Cj0 = si/xd. :- = 8.854×10−12 F/m • Depletion region width (zero biased): – xd = sqrt[2siVbi(1/NA + 1/ND) /q]. • Junction capacitance is function of voltage across junction: – Cj(Vr) = Cj0 *(1 - Va/Vbi)^-m – m is a constant ranges from 0.3 to 0.5 • Junction capacitance decreases as the reverse bias voltage increases. • Cdiff=Cjo*WL+Cjo*h*(2L+W)
  • 10. Poly/metal wire capacitance The capacitance mechanism for poly and metal wires is, in contrast, the parallel plate capacitance. We take into account the changes in the electrical field at the edges of the plate by adding in a fringe capacitance per unit perimeter. These two capacitances are illustrated in Fig: Capacitances can form between signal wires.
  • 11. Poly/metal wire capacitance • Two components: –parallel plate; –fringe. plate fringe
  • 12. Fringing Capacitance • Fringe capacitance is formed between non-overlapping sidewall of one conductor and surface/sidewall of a second conductor on the same or different layer from the first one. • This type of capacitance becomes significant as we route in higher layers because higher layers are thicker.
  • 13. Fringing Capacitance W - H/2H + (a) (b)
  • 14. Typical Poly/Metal Capaciatnce values for 0.5 micron process • Poly: Metal2:  plate: 0.09fF/µm^2 plate: 0.02fF/µm^2  fringe: 0.04fF/µm fringe: 0.06fF/µm • Metal1: Metal3:  plate: 0.04fF/µm^2 plate: 0.009fF/µm^2  fringe: 0.09fF/µm fringe: 0.02fF/µm^
  • 15. Metal coupling capacitances • Can couple to :  adjacent wires on same layer,  wires on above/below layers: • Orthogonal Wires in Different Layers:  Reduction of coupling capacitance between Layers metal 2 metal 1 metal 1 Cm1m2 Cw1w2
  • 16. Example: parasitic capacitance measurement • n-diffusion: bottomwall=2 fF, sidewall=2 fF. • metal: plate=0.15 fF, fringe=0.72 fF. 3 m 0.75 m 1 m 1.5 m
  • 17. Metal coupling capacitances  As the number of metal levels increases and the substrate capacitance decreases, wire-to-wire parasitics are becoming more important.  Both capacitance between two different layers and between two wires on the same layer are basic parallel plate capacitances.  The parasitic capacitance between two wire on different layers, such as Cm1m2 in Fig:, depends on the area of overlap between the two wires.  The capacitance between two wires on the same layer, Cw1w2 in the Fig:, is formed by the vertical sides of the metal wires.  When two wires on the same layer run in parallel for a long distance, the coupling capacitance can become very large.
  • 18. 18 Parastic Elements • So far, we’ve concentrated on getting circuit elements that we want for digital design –Transistors –Wires • Parasitics - occur whether we want them or not –Capacitors –Resistors –Transistors (bipolar and FET)