Introduction to
CMOS VLSI
         Design
Silicon-on-Insulator (SOI)
           Curtis Nelson
       Walla Walla University
                       Outline
 q   Overview of Silicon-on-Insulator (SOI)
 q   Floating Body Voltage
 q   SOI Advantages
 q   SOI Disadvantages
 q   Implications for Circuit Styles
 q   Summary
Silicon on Insulator                            Slide 2
                       SOI Overview
q SOI-based devices differ from conventional silicon-built devices
    in that the silicon junction is above an electrical insulator,
    typically silicon dioxide or sapphire (these types of devices are
    called silicon on sapphire, or SOS). The choice of insulator
    depends largely on intended application, with sapphire being
    used for high-performance radio frequency (RF) and radiation-
    sensitive applications, and silicon dioxide for diminished short
    channel effects in microelectronics devices.
Silicon on Insulator                                            Slide 3
                       SOI Overview
q   The implementation of SOI technology is one of several manufacturing
      strategies employed to allow the continued miniaturization of microelectronic
      devices, colloquially referred to as extending Moore's Law. Reported benefits
      of SOI technology relative to conventional silicon (bulk CMOS) processing
      include:
         Lower parasitic capacitance due to isolation from the bulk silicon, which
           improves power consumption.
         Resistance to latchup due to complete isolation of the n- and p-well
           structures.
         Higher performance at equivalent VDD. Can work at low VDD's.
         Reduced temperature dependency due to no doping.
         Better yield due to high density, better wafer utilization.
         Reduced antenna issues.
         No body or well taps are needed.
         Lower leakage currents due to isolation thus higher power efficiency.
         Inherently radiation hardened ( resistant to soft errors ), thus reducing the
           need for redundancy.
Silicon on Insulator                                                               Slide 4
                       SOI Overview
q Adopted for IBM PowerPC processors in 1998
       Higher performance and lower power than CMOS
       Higher manufacturing cost and complicated circuit design
q Differences from bulk CMOS
       Transistor source, drain, & body (channel) surrounded by
         insulating SiO2 rather than substrate (well)
       Eliminates most diffusion parasitic Capacitance
       Body no longer tied to GND or VDD
            Any change in body voltage modulates Vt (which has its own
              advantages and disadvantages)
Silicon on Insulator                                                 Slide 5
                       SOI Overview
q   IBM began to use SOI in the high-end RS64-IV "Istar" PowerPC-AS
      microprocessor in 2000. Other examples of microprocessors built on SOI
      technology include AMD's 130 nm, 90 nm, 65 nm, 45 nm and 32 nm single,
      dual, quad, six and eight core processors since 2001. Freescale adopted SOI
      in their PowerPC 7455 CPU in late 2001, currently Freescale is shipping SOI
      products in 180 nm, 130 nm, 90 nm and 45 nm lines. The 90 nm Power
      Architecture based processors used in the Xbox 360, PlayStation 3 and Wii use
      SOI technology as well. Competitive offerings from Intel however continues to
      use conventional bulk CMOS technology for each process node, instead
      focusing on other venues such as HKMG and Tri-gate transistors to improve
      transistor performance. In January 2005, Intel researchers reported on an
      experimental single-chip silicon rib waveguide Raman laser built using SOI.
q   As for the traditional foundries, on July 2006 TSMC claimed no customer
      wanted SOI, but Chartered Semiconductor devoted a whole fab to SOI.
Silicon on Insulator                                                         Slide 6
                       SOI Inverter
q Process starts with a wafer containing a thin layer of SiO2
    buried beneath a thin single-crystal silicon layer
Silicon on Insulator                                              Slide 7
                 IBM SOI Process
q Scanning electron micrograph of a 6-transistor static RAM cell
    in 0.22 um IBM SOI process
Silicon on Insulator                                          Slide 8
                Two Types of SOI
q Partially depleted (PD)
       Body thicker than channel depletion width
       Body voltage changes, depending on the amount of charge
         injected into bulk
       Causes history effect, which changes Vt
q Fully depleted (FD)
         Body thinner than channel depletion width
         Fixed body charge
         Body voltage does not change
         Thin body makes this very hard to manufacture
         Therefore, seldom used
Silicon on Insulator                                        Slide 9
        Floating Body Voltage
q Key to understanding SOI is to follow the body voltage
q Body voltage varies as body charges/discharges
q Charge paths to/from floating body
Silicon on Insulator                                         Slide 10
             Body Charge Paths
q Reverse-biased drain-to-body Ddb and
    source-to-body Dsb junctions
       Carry small diode leakage currents into
         body
q High-energy carriers cause impact
    ionization
       Create e hole pairs
             Injected into gate or gate oxide
             Cause hot e wearout
             Corresponding holes accumulate in
               body
       Most pronounced at VDS > intended
         operating point
       Iii is impaction ionization current into body
Silicon on Insulator                                     Slide 11
Ways for Charge to Exit Body
q As body voltage increases
      Source-to-body Dsb junction slightly
        forward biases
      Charge exiting from Dsb balances charge
        entering from Ddb
q Rising gate/drain voltage capacitively
    couples body upward
      May strongly forward-bias source-to-body
        Dsb junction and spill charge out of body
      During long idle periods (micro-seconds),
        body Voltage reaches equilibrium
      When switching resumes
          Charge spills off body
          Shifts body voltage and Vt significantly
Silicon on Insulator                                   Slide 12
                  SOI Advantages
q   Lower Cdiffusion  largely eliminated
q   Lower parasitic delay
q   Lower dynamic power consumption
q   Potential for lower Vt
       Bulk CMOS  Vt varies with channel length
            Poly etching variations cause Vt variations
            Must make Vt high enough to limit worst-case subthreshold
              leakage, so nominal Vt is typically higher that needs to be
       SOI
            Smaller threshold variations
            Nominal Vt can be closer to worst-case
            Faster transistors, especially at low VDD
Silicon on Insulator                                                  Slide 13
            Subthreshold Swing
q Bulk CMOS  subthreshold slope of n vT ln10
       vT = kT/q (thermal voltage, 26 mV at room temp)
       n is process dependent, usually about 1.5
q So subthreshold slope is about 90 mV/decade
       For each 90 mV decrease in Vgs below Vt, subthreshold
         leakage current is reduced by 10 X
q SOI (IBM) -- subthreshold slope of 75-85 mV/decade
q Double-gate MOSFETs and FINFETs are SOI
    variations
       Offer even lower subthreshold slopes
       Gate surrounds channel  turns off quicker
Silicon on Insulator                                        Slide 14
                       FINFETs
Silicon on Insulator              Slide 15
                       Latchup
q SOI is immune to latchup because the
    insulating oxide eliminates the parasitic
    bipolar devices that could trigger latchup
Silicon on Insulator                             Slide 16
              SOI Disadvantages
q History effect
      Changes in body V modulate Vt, vary gate delay
q Body voltage depends on whether device was idle or
    switching -- delay is a function of switching history
q Overall, elevated body voltage
      Reduces Vt and makes gates faster but the uncertainty makes
        circuit design more challenging
q Model history effect
      Assign different propagation and contamination delays to
        each gate
      History effect causes about 8% gate delay variation (IBM)
           Less than process and environmental variations
Silicon on Insulator                                          Slide 17
           More Disadvantages
q History effect
       Causes significant mismatches between otherwise matched
         transistors
            Sense amplifier (differential pair problems)
            Analog OPAMP
            Gilbert cell analog multiplier (mixer)
       May be solved by introducing substrate contact to make
         transistor pair behave identically
Silicon on Insulator                                         Slide 18
Parasitic Bipolar Transistor
q Can be a problem because the body/base floats
Silicon on Insulator                            Slide 19
      Current Pulse Problems
q Hold source & drain high for a long time
      While gate is low
      Base floats high through diode leakage
q Then, pull source low and npn transistor turns ON
      IB flows from body/base to source/emitter
      Causes IB to flow from drain/collector to source/emitter
            depends on channel length & doping but can be greater than 1
      Can get a current pulse from drain to source even though
        transistor should be OFF
Silicon on Insulator                                               Slide 20
                       Current Pulse
q This current pulse is sometimes called Pass-gate
    Leakage
q Often happens to OFF pass transistors where
    source & drain are initially high and then go low
       No problem for static circuits because the ON transistors
         oppose the glitch
       Causes malfunctions in dynamic latches in logic
            Need strong keepers to hold node steady
Silicon on Insulator                                           Slide 21
          Self-Heating Problem
q SiO2 is great thermal and electrical insulator
       Heat accumulates in transistors
       Rather than spreading to substrate as in CMOS
q Individual transistors with large power
       Heat substantially more than the die
       Deliver less current, slower
q Can raise T by 10 to 15 C for clock and I/O devices
       Less significant for logic
Silicon on Insulator                                     Slide 22
     Implications for Circuits
q SOI good for fast CMOS logic
       Smaller Cdiffusion gives lower parasitic delay
       Lower Vt gives better drive current and lower delay
q SOI attractive for low-power design
       Smaller Cdiffusion reduces dynamic power
       Easier to scale down VDD
       Consider FINFETs  sharper subthreshold slope
q Static CMOS in PD SOI
       Similar to bulk CMOS family, but faster
       History effect causes pattern dependent delay variation
Silicon on Insulator                                           Slide 23
                       Dynamic Gates
q New problem: pass-gate leakage
       Causes dynamic latches and gates to lose charge on
         dynamic node
       Fixed by staticizing the output
Silicon on Insulator                                          Slide 24
   Solve Pass-gate Leakage
q Staticize capacitive storage nodes
       Cross-coupled inverter pair for latches
q pMOS keeper for dynamic gates
       Can pre-discharge internal nodes to prevent pass-gate
         leakage
            Then have a charge sharing problem on internal nodes
q Staticizing transistors must be  as strong as
    normal path
       Slows down gates
Silicon on Insulator                                                 Slide 25
        Gated Clock Problems
q Gated clocks have increased skew
       History effect makes clock switch more slowly when
         activated after being disabled for a long time
Silicon on Insulator                                          Slide 26
                       Summary
 q   Overview of SOI
 q   Floating Body Voltage
 q   SOI Advantages
 q   SOI Disadvantages
 q   Implications for Circuit Styles
Silicon on Insulator                     Slide 27