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    FinFET and other NewTransistor Technologies

    Chenming Hu

    Univ. of California

    Chenming Hu, July 2011

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    2

    NY Times news article:

    Intel will use 3D FinFET for 22nm

    Most radical change in decades

    There is a competing SOI technology

    May 4 2011 NY Times Front Page

    Chenming Hu, July 2011

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    3

    TSMC, IBMnew transistors soon

    Since 2001 ITRS shows FinFET and

    ultra-thin-body UTB-SOI as the twosuccessor MOSFETs

    SOITEC UTB-SOI recently available

    IBM 2009 5nm UTB SOI paper

    Other Background Info

    Chenming Hu, July 2011

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    4

    New MOSFET Structures

    Chenming Hu, July 2011

    Cylindrical FET

    Ultra Thin Body SOI

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    5

    Vt, S (swing) and Ioff

    are sensitive to Lg &

    dopant variations.

    high design cost high Vdd, hence

    high power usage

    Good Old MOSFET Nearing Limits

    Finally painful enough for change.

    Chenming Hu, July 2011

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    Power Consumption Problems

    1.Not just a chip and package thermal

    issue.2.ICs use a few % of worlds electricity

    today and

    Power per chip is growing.

    IC units in use also growing.

    3.If power consumption is not reduced,industry future growth is at risk.

    Chenming Hu, July 2011

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    7

    Want Low Vt and Low Ioff

    Need smaller

    S and less

    variations of

    S and Vt

    Chenming Hu, July 2011

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    MOSFET becomes resistor at very

    small L - Drain competes with Gate tocontrol the channel barrier.

    0.0 0.3 0.6 0.910

    -11

    10-9

    10-7

    10-5

    10-3

    DrainC

    urrent,ID

    S(A/m

    )

    Gate Voltage, VGS

    (V)

    Size

    shrink

    How Vt Variation & S Got So Bad

    L

    Gate

    Insulator

    Source Drain

    Cg

    Cd

    Gate

    or larger Vd

    Smaller

    size

    Chenming Hu, July 2011

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    Reducing EOT is Not Enough

    Gate cannot control the

    leakage current pathsthat are far from the gate.

    Gate

    Source Drain

    Leakage Path

    Chenming Hu, July 2011

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    One of Two Ways to Better Vt and S

    The gate controls a thin body from

    more than one side.

    Gate

    Gate

    Source Drain

    FinFET body is a

    thin finN. Lindert et al., DRC paper II.A.6, 2001

    S

    ource

    Drain

    Fin Width

    Fin Height

    Gate Length

    Chenming Hu, July 2011

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    FinFET- 1999

    Undoped Body. 30nm etched thin fin.Vt set with gate work-function (SiGe).

    X. Huang et al., IEDM, p. 67, 1999

    -0.6

    -0.4

    -0.2

    0.0

    0.2

    0.4

    0.6

    0 10 20 30 40 50

    Lg [nm]

    Vt[V]

    Vt at 100 nA/m, Vd = 0.05 V

    Fin width: 20 nm

    Chenming Hu, July 2011

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    STI

    Gate

    SiSTI

    STI

    Gate

    SiSTI

    State-of-the-Art FinFET on Buk Si20nm Hi PerfC.C. Wu et al.,

    2010 IEDM

    28nm SoC

    C.C. Yeh et al.,2010 IEDM

    Chenming Hu, July 2011

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    FinFET is Easy to Scale

    because leakage is well suppressed if

    Fin thickness =or< LgThin fin can be made with the same Lgpatterning/etching tools.

    Chenming Hu, July 2011

    Lg=5 nm

    5nm Lg TSMC2004 VLSI Symp

    10nm Lg AMD2002 IEDM

    3nm Lg KAIST2006 VLSI Symp

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    Second Way to Better Vt and S

    Ultra-thin-body SOI (UTB-SOI)No leakage path far from the gate.

    1.E-12

    1.E-10

    1.E-08

    1.E-06

    1.E-04

    1.E-02

    0 0.2 0.4 0.6 0.8 1

    Gate Voltage [V]

    Dra

    inCurrent[A/um]

    Tsi=8nm

    Tsi=6nm

    Tsi=4nm

    Y-K. Choi, IEEE EDL, p. 254, 2000

    Gate

    Source DrainUTB

    SiO2

    Si

    Chenming Hu, July 2011

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    Most Leakage Flows >5nm Below Surface

    Y-K. Choi et al., IEEE Electron Device Letters, p. 254, 2000Chenming Hu, July 2011

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    Y-K. Choi et al, VLSI Tech. Symposium, p. 19, 2001

    3nm Silicon Body, Raised S/DUTB-SOI

    Chenming Hu, July 2011

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    State-of-the-Art 5nm

    Thin-Body SOI

    ETSOI, IBMK. Cheng et al, IEDM, 2009

    Chenming Hu, July 2011

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    Both Thin-Body Transistors Provide

    Better swing.

    S & Vt less sensitive to Lg and Vd.

    No random dopant fluctuation.

    No impurity scattering.Less surface scattering (lower Eeff).

    Higher on-current and lower leakageLower Vdd and power consumptionFurther scaling and lower cost

    Chenming Hu, July 2011

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    Back-Gate Bias Option

    UTB-SOI FinFET

    STI

    STI

    Si

    Gate 1Gate 2

    Chenming Hu, July 2011

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    Similarities1996: UC Berkeley proposed to DARPA two

    25nm Transistors. Both of themuse body thickness as a new scaling parametercan use undoped body for high and no RDF1999: demonstrated FinFET2000: demonstrated UTB-SOI (Ultra-Thin Body)

    Since 2001: ITRS highlights FinFET and UTBSOI

    Now: Intel will use Trigate FinFET.Soitec readies +-0.5nm substrates for UTBSOI

    Both FinFET & UTBSOI better than planar bulk!Chenming Hu, July 2011

    ff

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    Main DifferencesFinFET body thickness ~ Lg. Investment by fabs

    UTBSOI thickness ~1/3 Lg. Investment by SoitecFinFET has clear long term scalability. UTBSOImay be ready sooner depending on each firms

    readiness with FinFET.FinFET has larger Ion or can use lower Vdd.UTBSOI has a good back-gate bias option.

    STI

    STI

    Si

    Gate 1 Gate 2

    UTBSOI

    FinFETChenming Hu, July 2011

    h

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    What May Happen

    FinFET will be used at 22nm by Intel and later

    by more firms through and beyond 10nm.Some firms may use UTBSOI to gain/protectmarket at 20 or 18nm if FinFET is not option.

    If so, competition between FinFET and UTBSOIwill bring out the best of both.

    If not----- back to first bullet.

    Chenming Hu, July 2011

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    Chenming Hu, July 2011

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    FinFET BSIM Compact Model Verified

    FinFET Fabricated at TSMC.

    Lg = 30 nm-10um

    0.0 0.4 0.8 1.20

    25

    50

    Vd = 1.2V

    Vd = 50mV

    Lg = 50nm

    Dr

    ainCurrent(A

    )

    Gate Voltage (V)

    1p

    1n

    1

    1m

    0.0 0.4 0.8 1.21p

    10p

    100p

    Vd = 1.2V

    Lg = 50nm

    Bu

    lkCurrent(A)

    Gate Voltage (V)

    Id-Vd

    0.0 0.4 0.8 1.20

    25

    50

    Vg = 1.2 - 0.4V

    Lg = 50nm

    Dra

    inCurrent(A)

    Drain Voltage (V)

    Id-Vg Ibulk Id-Vd

    Chenming Hu, July 2011

    M. Dunga, 2008 VLSI Tech Sym

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    Chenming Hu, July 2011

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    Chenming Hu, July 2011

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    Chenming Hu, July 2011

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    Chenming Hu, July 2011

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    30

    Reduce all capacitances.

    Reduce C

    2

    ddVCf

    Chenming Hu, July 2011

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    Vacuum-Sheath Interconnect

    Etch Stop layer

    Metal

    Dielectric Beam

    Mutual Capacitance : CM

    Total Capacitance : CTOTAL

    Load Capacitance : CO

    CTOTAL

    Delay, CM

    Crosstalk Noise

    J . Park, Electronics Letters, p. 1294, 2009

    Chenming Hu, July 2011

    Effective k of Vacuum Sheath

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    Effective k of Vacuum-SheathInterconnects

    No Solution

    B

    eamD

    ielectricConstant

    20 30 40 50 60 70 80

    Air Percentage (%)

    2.25

    2.9

    3.3

    3.6

    3.9

    1.3

    1.41.5

    1.6

    1.71.8

    1.92.02.1

    2.22.32.4

    2.5

    2.6No Solution

    J . Park, Electronics Letters, p. 1294, 2009Chenming Hu, July 2011

    V S t R d C

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    Vacuum Spacer to Reduce CGC

    CGCCGOX

    Gate

    Contacts

    CGC