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Carrier mobility enhancement in strained silicon germanium channels

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Presentation on theme: "Carrier mobility enhancement in strained silicon germanium channels"— Presentation transcript:

1 Carrier mobility enhancement in strained silicon germanium channels
SiNANO Workshop Carrier mobility enhancement in strained silicon germanium channels David Leadley University of Warwick

2 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

3 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

4 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

5 Pseudomorphic Si0.64Ge0.36 on Si
Mobility doubled

6 Nicholas et al, Electronics Letters 41, 20052074
Impact Ionisation Reduced impact ionisation for SiGe, despite higher mobility Nicholas et al, Electronics Letters 41,

7 High-k gated SiGe Deposited HfO2
Si cap – oxidises to thin SiO2 interlayer Metal HfO2 SiO2 SiGe Si Lowest EOT 12Å < 1nm

8 Metal gate/HfO2 gate stack development for Si(cap)/Si0.8Ge0.2 channel
Interface state density (W gate) Gate leakage Warwick, AMO, Chalmers

9 High-k/metal gated Si0.8Ge0.2 surface p-channel devices
enhancements beating Intel (IEDM 2004) KTH, Warwick, Chalmers, AMO

10 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

11 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]

12 Novel p-channel/substrate orientations
= 3.2 nm … enhancement beating Liu et al (VLSI Symp 2006) KTH, Warwick, Chalmers, AMO

13 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

14 Unstrained Ge Ge + anneal Si IMEC

15 Uniformity restored after anneal
Nit spread 0.2-8x1012cm-2 affects Ids, gm and Vt Uniformity restored after anneal IMEC

16 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

17 Mobility in unstrained Ge
μ > 300 cm2/Vs Correction required for Rsd in short channel devices Lg<0.25μm IMEC

18 Investigating trapped charge
Dit varies across wafer x1012cm-2 Warwick, IMEC

19 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

20 Mobility modelling at 4K
At low T, with confinement only have one HH subband. Fit using ni and D as parameters ... Warwick, IMEC

21 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

22 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

23 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

24 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

25 sGe global platform - 80% terrace grade
TDD=3x105/cm-2, PUD = 0, RMS ≈ 8nm Warwick, FZ-Jeulich, LETI

26 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

27 Positive Vt due to gate workfunction
Strained Ge pMOS 150nm TiN 4nm ALD HfO2 Positive Vt due to gate workfunction ASM, Warwick, IMEC

28 Record Ge mobility via CMOS process
Peak μ = 650 cm2/Vs G. Nicholas et al., IEEE EDL 28, 825 (2007) Warwick, IMEC

29 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.

30 Summary Addition of Ge improves mobility High-k makes Ge viable
Mobility enhancements relevant for nanometre scale devices

31

32

33 Terrace grading – new generation of virtual substrates
TDD ≈ 4 x 104 cm-2 PUD = 0 30% Warwick

34 LG 30% ≈105 cm-2 TDD Pile-up ≈1 cm-1

35 High stability sSi layers
Linear Grading Relaxation (%) Terrace Grading Strained Si thickness (nm) J. Parsons et al., ULIS 2007 Warwick, FZ-Jeulich

36 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

37 Extended Stacking Faults
“Perfect” dislocation Stacking fault Trailing (30°) “partial” dislocation Leading (90°) “Partial” dislocation S-Si SiGe

38 Stacking faults – effective misfit dislocation blockers?
Defect etch images of 30nm strained silicon layer J. Parsons et al., ULIS 2007 Warwick, FZ-Jeulich

39 50% terrace graded (for sSi)
TDD = 2x105 cm-2 PUD = 0 Warwick

40 ≈ 20% TG - slower growth (+sSi)
TDD = 4 x 104/cm2 PUD = 0

41 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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