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10GHz Clock Distribution using Coupled Standingwave Oscillators

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Title: 10GHz Clock Distribution using Coupled Standingwave Oscillators


1
10GHz Clock Distribution using Coupled
Standing-wave Oscillators
  • Frank OMahony (fomahony_at_stanford.edu)
  • Advisor Professor S. Simon Wong
  • Integrated Circuits Lab (ICL)
  • Stanford University

2
Outline
  • I. Proposed 10GHz clock network
  • II. Standing-wave oscillators (SWOs)
  • III. Clock grids from coupled SWOs
  • IV. 10GHz test chip results
  • V. Simulated jitter and clock buffer

3
Proposed 10GHz global clock network
  • Global clock network distributes a 10GHz clock
    through a grid of standing-wave oscillators
    (SWOs)
  • SWOs are coupled together and sustain
    synchronous, sinusoidal standing waves across the
    chip
  • A single clock source coupled into one oscillator
    injection-locks the entire grid
  • Clock buffers convert the signal to a digital
    clock to drive the local networks
  • The combination of standing waves and coupled
    oscillators enable low-skew, low-jitter clock
    distribution

Single SWO
Clkinj
4
Standing-wave grid waveform
  • Standing waves
  • ideally zero skew
  • amplitude varies with position

5
Standing wave oscillator (SWO)
  • SWOs compensate for interconnect loss with
    circuitry
  • Multiple, identically sized cross-coupled pairs
    provide gain
  • Differential transmission lines form a
    distributed tank
  • SWOs can be coupled together by connecting their
    interconnects and injection locked to an external
    source
  • These (effectively) lossless interconnects
    sustain ideal standing-waves with zero skew

LC oscillator vs. standing-wave oscillator (SWO)
Conditions for oscillation at fclk
6
SWO amplitude and skew
  • A test chip confirmed low-skew for single SWO
  • 8GHz clock (injection locked)
  • 0.18µm CMOS process
  • 90µm NMOS devices
  • 80mW total power
  • 4.1 mm TL resonator

Amplitude
Amplitude varies sinusoidally
Phase (ps)
Less than 1ps skew
7
Coupled standing-wave oscillators
  • Multiple SWOs can be coupled together to form a
    grid by connecting their wires
  • Each SWO can be viewed as an injection-locked
    oscillator
  • Networks of coupled oscillators have a
    phase-averaging effect that reduces jitter
  • A single external clock reference can be injected
    into one of the SWOs to lock the entire grid

Clkinj
8
10GHz clock grid test chip
  • Fabricated in a 0.18µm, 1.8V CMOS process with
    six AlCu metal levels
  • Five cross-coupled pairs per SWO
  • Differential microstrip transmission lines,14µm
    wide, 4µm spacing, 3.5µm oxide thickness
  • Grid is tunable with MOS varactors, allowed for
    intentional detuning of the grid
  • Clock receivers are not integrated due to the
    performance limitations of the devices at 10GHz

Clkinj
0.6mm
1.8mm
90µm/0.18µm cross-coupled pairs
9
Skew measurements
  • Tuned grid
  • Entire grid is tuned with a single control
    voltage
  • Worst-case skew 0.6ps
  • Detuned grid
  • One half of the grid is detuned by 1 (10.1GHz)
  • Detuning causes a skew gradient across the grid
  • Worst-case skew 3.3ps
  • Maximum skew between two adjacent points 1.4ps

10
Measuring sub-picosecond skew
  • Fold clock grid so timing nodes close together
  • Homodyne technique mixes the relative phase
    information down to baseband
  • Achieves good phase sensitivity (17mV/ps) and
    resolution (lt0.5ps) with careful on-chip delay
    matching in the timing path

4a
2a
3a
1a
3b
4b
1b
2b
?ref
chip boundary
Voltmeter
11
Jitter measurement
Tektronics CSA 803C
SWO clock grid injection-locked at 10.0 GHz
1.4ps rms jitter
HP83711B Signal Generator
Pad (to 50 ? CSA)
50?
Differential open-drain buffer
27µm0.18µm
1.5ps rms jitter
12
10GHz test chip
13
Jitter simulations for SWO grids
  • Coupling together multiple SWOs reduces the
    jitter caused by power supply variations
  • Each SWO in a grid is coupled with up to three
    other SWOs
  • For the simulated case of a 10 power supply drop
    at one cross-coupled pair, the jitter decreases
    as the grid gets larger

Power supply noise 10 variation with 100ps step
14
Clock buffer/converter
  • Clock buffer delay must not depend on the
    amplitude of the input, or it will add skew
  • LPF removes the harmonics that cause
    amplitude-dependent skew
  • Simulated with a 2GHz clock (7 FO4 clock period)
    using 0.18µm device models

Clk
Clk
Clock input
200mV
140mV
Vin
5.9ps skew (1.2 of clock cycle)
Sine-to-square converter
Limiting Amp and LPF
Clock output
15
Conclusions
  • Ideal, low-skew standing waves can be sustained
    on-chip by compensating for interconnect losses.
  • Networks of standing-wave oscillators can be
    coupled together to form a clock network with
    favorable skew and jitter characteristics.
  • A standing-wave clock network is feasible in a
    future technology for 10GHz clock distribution.

Current work
  • Develop a simple model for the behavior of
    networks of coupled standing-wave oscillators.
  • Compare the skew and jitter sensitivities of a
    complete multi-GHz standing-wave clock
    distribution to conventional clock networks.
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