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Interconnect and Packaging Lecture 2: Scalability

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1 Interconnect and Packaging Lecture 2: Scalability
Chung-Kuan Cheng UC San Diego

2 Outlines Trends of Interconnect and Packaging Scalability References

3 I. Trends of High Performance Interconnect and Packaging
Year 2005 2010 2015 D1/2 Pitch nm 80 45 25 Chip size (mm2) 310 Pin count 3,400 4,009 6,402 Cents/pin 1.78 1.37 1.05 On-chip (MHz) 5,170 12,000 - Off-chip (MHz) 3,125 29,103 Power Density (w/mm2) 0.54 0.64

4 I. Trends Off-Chip Interconnect and Packaging On-Chip Interconnect
Delay (5-40 times of Speed of Light 5ps/mm) Power Density (> ½) Clock Skew: Variations (5GHz) Off-Chip Interconnect and Packaging Number of pins (limited growth) Wire density (scalability) Speed and distance of interconnect

5 I. Trends On-chip Global Interconnect trend
Concerns: Speed, Power, Cost, Reliability

6 I. Trend Scalability Distortion Clock Distribution IO Interface
Latency, Bandwidth Attenuation, Phase Velocity Distortion Intersymbol Interference, Jitter, Cross Talks Clock Distribution Skew, Jitter, Power Consumption IO Interface Density Impedance Matching Cross Talks, Return loops

7 II. Scalability: Interconnect Models
Voltage drops through serial resistance and inductance Current reduces through shunt capacitance Resistance increases due to skin effect Shunt conductance is caused by loss tangent

8 II. Scalability: Interconnect Models
Telegrapher’s equation: Propagation Constant: Wave Propagation: Characteristic Impedance

9 II. Scalability of Physical Dimensions
R= p /A = p/(wt) Z= ¼ (u/e)1/2 ln (b+w)/(t+w) C= v Z L= Z/v b w t p: resistivity of the conductor u: magnetic permeability e: dielectric permittivity v: speed of light in the medium

10 II. Scalability of Physical Dimensions
Resistance: Increases quadratically with scaling, e.g. p=2um-cm R=0.0002ohm/um at A=10umx10um R=0.02ohm/um at A=1umx1um R=2ohm/um at A=0.1umx0.1um Characteristic Impedance: No change Capacitance per unit length: No change Inductance per unit length: No change

11 II. Scalability of Frequency Ranges
RC Region LC Region Skin Effect Loss Tangent

12 II. Scalability of Frequency Ranges
1. RC Region e.g. on-chip wires R=2ohm/um(A=0.01um2) L=0.3pH/um, C=0.2fF/um R/L=0.67x1012

13 II. Scalability of Frequency Ranges: RC Region
Elmore delay model with buffers inserted in intervals l ltr ltr: length from transmitter to receiver l: interval between buffers rn: nmos resistance cn: nmos gate capacitance cg=(1+g)cn, g is pn ratio. rw: wire resistance/unit length cw: wire capacitance/unit length f: cd/cg

14 II. Scalability of Frequency Ranges: RC Region
Elmore delay model with buffers inserted in intervals Optimal interval Optimal buffer size Optimal delay

15 II. Scalability of Frequency Ranges
Example: w= 85nm, t= 145nm rn= 10Kohm,cn=0.25fF,cg=2.34xcn=0.585fF rw=2ohm/um, cw=0.2fF/um Optimal interval Optimal buffer size Optimal delay

16 II. Scalability of Frequency Ranges: RC Region
Year (On-Chip) 2005 2010 2015 rncn (ps) 0.86 0.39 0.18 rwcw (ps/mm)* 284 616 1510 l (um) 168 77 33 D (ps/um) 0.096 0.095 0.101 *no scattering, p=2.2uohm-cm

17 II. Scalability of Frequency Ranges: RC Region
Device delay, rncn, decreases with scaling Wire delay, rwcw, increases with scaling Interval, l, between buffers decreases with scaling In order to increase the interval, we add the stages of each buffer.

18 II. Scalability of Frequency Ranges
2. LC Region

19 II. Scalability 3. Skin Effect Skin Depth:
e.g. f=10GHz, p=2uohm-cm For 100umx25um RDC= ohm/um= 8ohm/m R= ohm/um=114ohm/m

20 II. Scalability 4. Loss Tangent

21 References E. Lee, et al., “CMOS High-Speed I/Os – Present and Future,” ICCD 2003. G.A. Sai-Halasz G.A. "Performance Trends in High-End Processors,“ IEEE Proceedings, pp , Jan M.T. Bohr, “Interconnect scaling-the real limiter to high performance ULSI” Electron Devices Meeting, 1995., International Dec pp.241 – 244.


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