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Carrier mobility enhancement in strained silicon germanium channels
SiNANO Workshop Carrier mobility enhancement in strained silicon germanium channels David Leadley University of Warwick
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Collaborators Warwick IMEC SINANO partners KTH, Udine, Chalmers, AMO
Tim Grasby, Andy Dobbie, Chris Beer, Jon Parsons, Evan Parker, Terry Whall IMEC Gareth Nicholas, Marc Meuris, M Heyns, P Zimmerman, Matty Caymax, ++ SINANO partners KTH, Udine, Chalmers, AMO
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Why is mobility still critical ?
High mobility - light mass and minimal scattering ITRS – long term years By 2020, Lg=5nm, Vdd=0.7V Mobility enhancement factor of 1.04 each node Ballistic enhancement factor x2 Double gate structures – light doping
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Why add Ge? ADVANTAGES BUT… Smaller bandgap Lighter hole mass
Strain – splits bands and reduces scattering BUT… Native oxide no good Band-to-band tunnelling
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Pseudomorphic Si0.64Ge0.36 on Si
Mobility doubled
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Nicholas et al, Electronics Letters 41, 20052074
Impact Ionisation Reduced impact ionisation for SiGe, despite higher mobility Nicholas et al, Electronics Letters 41,
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High-k gated SiGe Deposited HfO2
Si cap – oxidises to thin SiO2 interlayer Metal HfO2 SiO2 SiGe Si Lowest EOT 12Å < 1nm
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Metal gate/HfO2 gate stack development for Si(cap)/Si0.8Ge0.2 channel
Interface state density (W gate) Gate leakage Warwick, AMO, Chalmers
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High-k/metal gated Si0.8Ge0.2 surface p-channel devices
enhancements beating Intel (IEDM 2004) KTH, Warwick, Chalmers, AMO
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KTH, Warwick, Chalmers, AMO
Effective Mobility Best SiGe (25%) devices show mobility enhancement over silicon control Mobility degradation compared to universal – interface roughness and Coulomb scattering important KTH, Warwick, Chalmers, AMO
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HOT SiGe Hybrid Orientation Technology
n on (100), p on (110) in Si, Yang et al. IEDM 2003 in Si, no variation with orientation for long channels, but <110> best for short channels, Saito et al VLSI 2006 50% enhanced Idsat for SiGe (110) over Si (100), 3.3x for mobility, Liu et al VLSI 2006 (110) substrate [001] [110] (100) substrate [011]
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Novel p-channel/substrate orientations
= 3.2 nm … enhancement beating Liu et al (VLSI Symp 2006) KTH, Warwick, Chalmers, AMO
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PMOS fabricated with Lg ~125 nm
Unstrained Ge pMOS High performance Ge pMOS devices using a Si-compatible process flow Zimmerman et al. IEDM 2006 4nm HfO2 2μm Ge on Si substrate 12Å EOT, TDD cm-2 PMOS fabricated with Lg ~125 nm IMEC
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Unstrained Ge Ge + anneal Si IMEC
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Uniformity restored after anneal
Nit spread 0.2-8x1012cm-2 affects Ids, gm and Vt Uniformity restored after anneal IMEC
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Thinner EOT? Starts to leak when too thin !
Si Starts to leak when too thin ! Mobility increase with thinner HfO2 less charge trapping Ragnarsson et al. IEEE TED 53, 1657 ( 2006) IMEC
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Mobility in unstrained Ge
μ > 300 cm2/Vs Correction required for Rsd in short channel devices Lg<0.25μm IMEC
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Investigating trapped charge
Dit varies across wafer x1012cm-2 Warwick, IMEC
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Interface charge density
Extract Dit in 3 ways at 300K: from Vt – average all energies subthreshold slope – specific energy charge pumping Interface charge density Warwick, IMEC
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Mobility modelling at 4K
At low T, with confinement only have one HH subband. Fit using ni and D as parameters ... Warwick, IMEC
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Modelled 4K mobility ni agrees with values from Dit
Annealed As grown ni agrees with values from Dit Δ decreases after anneal from 0.6nm to 0.5nm, hence μSR increases by 35% μ300K must also depend on surface roughness Warwick, IMEC
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Strain tuning buffers Strained-Si by local strain now in production
Si1-yGey virtual substrates for global strain y~0.2 for s-Si y~0.5 for s-Si1-xGex y~0.8 for s-Ge Need low TDD and zero pile-up
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Terrace Graded VS – better than industrial quality
20% Ge XTEM TDD ≤ 105cm-2, PUD=0 10x10um2 AFM image indicating RMS roughness 1.5nm Warwick, LETI, Jeulich
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State-of-the-art sSi electron mobility from TG-VSs
strain 0.6 – 1.1% State of the art F. Driussi et al., ULIS 2007 Warwick, Udine, KTH
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sGe global platform - 80% terrace grade
TDD=3x105/cm-2, PUD = 0, RMS ≈ 8nm Warwick, FZ-Jeulich, LETI
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Novel thin VS for sGe Warwick
Seed layer 300nm Si0.2Ge0.8 Grade Strained Ge Si Sub Strained Si 20x20 um2 AFM image. 1.3nm RMS, fully relaxed 80% platform TDD ≈ 106/cm2 range Warwick
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Positive Vt due to gate workfunction
Strained Ge pMOS 150nm TiN 4nm ALD HfO2 Positive Vt due to gate workfunction ASM, Warwick, IMEC
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Record Ge mobility via CMOS process
Peak μ = 650 cm2/Vs G. Nicholas et al., IEEE EDL 28, 825 (2007) Warwick, IMEC
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Further comments on s-Ge
Full band Monte Carlo calculations, incl. BTBT, SCE etc. show best prospect for pMOS … … strained-Ge directly on Si ! Krishnamohan et al (Stanford) VLSI (2006) For s-SiGe OI, Idsat enhancement in short channels exceeds μ increase in long channel. Tsutomu Tezuka et al. VLSI (2006) nMOS still a problem for Ge … … but tensile strain Si0.1Ge0.9 on relaxed Ge promising.
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Summary Addition of Ge improves mobility High-k makes Ge viable
Mobility enhancements relevant for nanometre scale devices
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Terrace grading – new generation of virtual substrates
TDD ≈ 4 x 104 cm-2 PUD = 0 30% Warwick
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LG 30% ≈105 cm-2 TDD Pile-up ≈1 cm-1
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High stability sSi layers
Linear Grading Relaxation (%) Terrace Grading Strained Si thickness (nm) J. Parsons et al., ULIS 2007 Warwick, FZ-Jeulich
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Extended Stacking Faults
Defect etch image of 20nm strained silicon layer PVTEM image of 180nm strained silicon layer J. Parsons et al., ULIS 2007 Warwick, FZ-Jeulich
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Extended Stacking Faults
“Perfect” dislocation Stacking fault Trailing (30°) “partial” dislocation Leading (90°) “Partial” dislocation S-Si SiGe
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Stacking faults – effective misfit dislocation blockers?
Defect etch images of 30nm strained silicon layer J. Parsons et al., ULIS 2007 Warwick, FZ-Jeulich
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50% terrace graded (for sSi)
TDD = 2x105 cm-2 PUD = 0 Warwick
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≈ 20% TG - slower growth (+sSi)
TDD = 4 x 104/cm2 PUD = 0
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Schottky Barrier MOSFET- world best?
Tunnelling f(m*) Thermionic emmision Measurement Modelling D.J. Pearman et al., IEEE Trans ED (accepted 2006) UCL, Warwick, Glasgow
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