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University of
Southampton
University of
Southampton
Influence of HInfluence of H22 Preconditioning on thePreconditioning on the
Nucleation and Growth ofNucleation and Growth of
Self-Assembled Germanium IslandsSelf-Assembled Germanium Islands
on Silicon (001)on Silicon (001)
G. D. M. Dilliway, D. M. Bagnall, P. Ashburn
University of Southampton
N. E. B. Cowern, C. Jeynes, E. Mendoza
University of Surrey
Lu Xu, P. J. McNally
Dublin City University
University of
Southampton
University of
Southampton
OutlineOutline
 Introduction:
 Ge self-assembled nanostructures on Si (001)
 The role of hydrogen
 Experimental set-up:
 Deposition method
 Characterisation techniques
 Results
 Summary
 Conclusions
University of
Southampton
University of
Southampton
Self-assembled Ge islands on SiSelf-assembled Ge islands on Si
Self-assembly of Ge nanostructures compatible with Si-
based technology
 Si and Ge crystallise in a diamond cubic structure
 Ge lattice constant > Si lattice constant by 4.2%
Stranski-Krastanov growth mode
 After the coherent growth of ~3ML of Ge (wetting
layer), 3D islands form to relieve the misfit strain
Understanding the influence of the growth conditions on
the self-assembly process controlling the size
distribution
University of
Southampton
University of
Southampton
The role of hydrogenThe role of hydrogen
During pre-deposition:
 Ex- or in-situ for hydrogen-terminated surfaces
 In-situ for desorbing SiO2
During deposition:
 H2 is used as a carrier-gas
 For growth from hydrides, as a by-product
The need to understand the influence of hydrogen
on the nucleation and evolution of Ge self-assembled
nanostructures
 Annealing in H2 at high temperatures the
formation of steps and terraces on the (001) Si surface
 The higher the H2 pressure the higher the density
of defects
T. Komeda, Y. Kumagai, Phys. Rev. B 53(3), 1385 (1997)
In our study, H2 is present :
1. during pre-deposition
2. during deposition
University of
Southampton
University of
Southampton
Growth sequenceGrowth sequence
‘RCA’ oxide
desorption in
H2 100 sccm 1Torr
950ºC
Pump-down
chamber
to 10-3
Torr
Si high T buffer
from pure SiH4
100 sccm 1Torr
5 min
2 min 30s
40 s 40 s
650ºC
4 min 3 different durations
Time
Temperature
Pump-down
chamber
to 10-3
Torr
Lower temperature
to 650ºC at
10-3
Torr
(standard set)
Lower temperature
to 650ºC in H2
100 sccm 1Torr
(preconditioned set)
Ge self-assembled
islands from GeH4
(10.2% in H2) 30 sccm
0.5 Torr
University of
Southampton
University of
Southampton
Characterisation techniquesCharacterisation techniques
 Rutherford backscattering spectrometry
(RBS) in ‘random’ orientation
 Atomic force microscopy (AFM) tapping
mode
 Micro-Raman spectroscopy ( Raman) inμ
backscattering configuration
University of
Southampton
University of
Southampton
RBS resultsRBS results
0
2
4
6
8
10
0 2 4 6 8 10 12 14
Growth duration (s)
Gesurfacecoverage
(ML)
Standard Preconditioned
wetting layer
University of
Southampton
University of
Southampton
AFM results (shortest duration)AFM results (shortest duration)
Mixed islands: 7 mμ -2
Small height: 5-10 nm
(97%) width: 30-50 nm
Large height: 70 nm
width: 300 nm
PreconditionedStandard
Small islands: 4 mμ -2
Narrow size
distribution
Height: 3-8 nm
Width: 20-40 nm
University of
Southampton
University of
Southampton
AFM results (intermediate duration)AFM results (intermediate duration)
Preconditioned
Mixed islands: 10 mμ -2
Bimodal size distribution
Small height: 8-15 nm
(62 %) width: 50-100 nm
Large height: 20-30 nm
width: 120-200
nm
Standard
Mixed islands: 3 mμ -2
Bimodal size distribution
Small height: 5-8 nm
(70%) width: 30-50 nm
Large height: 20-40 nm
width: 100-180
nm
University of
Southampton
University of
Southampton
AFM results (longest duration)AFM results (longest duration)
Preconditioned
Mixed islands: 11 mμ -2
Bimodal size distribution
Small height: 8-20 nm
(54%) width: 50-100 nm
Large height: 25-40 nm
width: 150-200
nm
Standard
Mixed islands: 7 mμ -2
Bimodal size distribution
Small height: 10-20 nm
width: 100-120
nm
Large height: 25-40 nm
(60%) width: 200-250
nm
University of
Southampton
University of
Southampton
ISi-Ge/IGe-Ge= 2(1-x)/Bx ISi-Ge , IGe-Ge intensities of the Si-Ge and Ge-Ge
peaks
B = 2.218
wGe-Ge = 282.5 + 16x - 384ε wGe-Ge shift of the Ge-Ge peak
x Ge concentration (%)
ε strain
 Diffusion activation barrier for Ge adatoms on a strained Ge (001)
surface increases with compressive strain
A. Van de Walle, M. Asta, P.W. Voorhees, Phys. Rev. B 67, 041308 (2003)
 The periphery of the island is the location of the highest strain
P. Raiteri, L. Miglio, F. Valentinotti, M. Celino, Appl. Phys. Lett. 80(20), 3736
(2002)
Raman resultsμRaman resultsμ
Sample Ge
conc.
(%)
Strain (%) d[Ge]/dt
(%/s)
QD2H 53 -1.649
QD3H 47 -1.264
-3.0
Sample Ge
conc.
(%)
Strain (%) d[Ge]/dt
(%/s)
QD2 52 -1.045
QD3 55 -0.928
+1.5
Standard Preconditioned
University of
Southampton
University of
Southampton
Summary and conclusionsSummary and conclusions
standard samplesstandard samples
RBS, AFM and Raman results on Ge self-assembledμRaman results on Ge self-assembledμ
islands on two types of Si surfaces:islands on two types of Si surfaces:
1. Standard well-known steady evolution:
- low density of small islands, narrow size distribution
- bimodal size distribution resulted from ripening:
- small islands still dominate
- strain in the large islands is relived trough
intermixing
- predominantly large islands in which strain is relieved
through both intermixing and defect formation
University of
Southampton
University of
Southampton Summary and conclusionsSummary and conclusions
preconditioned samplespreconditioned samples
2. Preconditioned very accelerated initial evolution, which
then saturates:
 The addition of H2 during the ramp-down preserves a non-
equilibrium surface morphology:
- double the density of slightly larger islands (narrow size
distribution) + a very low density of unusually large island
(still under study)
- increase in the density and size through nucleation and
growth; misfit strain relaxes through intermixing
 During the final stages, evolution slows down because of
the high compressive strain in the deposited layer :
- saturation of the nucleation and growth; misfit strain
increases intermixing increases

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MRS 2004

  • 1. University of Southampton University of Southampton Influence of HInfluence of H22 Preconditioning on thePreconditioning on the Nucleation and Growth ofNucleation and Growth of Self-Assembled Germanium IslandsSelf-Assembled Germanium Islands on Silicon (001)on Silicon (001) G. D. M. Dilliway, D. M. Bagnall, P. Ashburn University of Southampton N. E. B. Cowern, C. Jeynes, E. Mendoza University of Surrey Lu Xu, P. J. McNally Dublin City University
  • 2. University of Southampton University of Southampton OutlineOutline  Introduction:  Ge self-assembled nanostructures on Si (001)  The role of hydrogen  Experimental set-up:  Deposition method  Characterisation techniques  Results  Summary  Conclusions
  • 3. University of Southampton University of Southampton Self-assembled Ge islands on SiSelf-assembled Ge islands on Si Self-assembly of Ge nanostructures compatible with Si- based technology  Si and Ge crystallise in a diamond cubic structure  Ge lattice constant > Si lattice constant by 4.2% Stranski-Krastanov growth mode  After the coherent growth of ~3ML of Ge (wetting layer), 3D islands form to relieve the misfit strain Understanding the influence of the growth conditions on the self-assembly process controlling the size distribution
  • 4. University of Southampton University of Southampton The role of hydrogenThe role of hydrogen During pre-deposition:  Ex- or in-situ for hydrogen-terminated surfaces  In-situ for desorbing SiO2 During deposition:  H2 is used as a carrier-gas  For growth from hydrides, as a by-product The need to understand the influence of hydrogen on the nucleation and evolution of Ge self-assembled nanostructures  Annealing in H2 at high temperatures the formation of steps and terraces on the (001) Si surface  The higher the H2 pressure the higher the density of defects T. Komeda, Y. Kumagai, Phys. Rev. B 53(3), 1385 (1997) In our study, H2 is present : 1. during pre-deposition 2. during deposition
  • 5. University of Southampton University of Southampton Growth sequenceGrowth sequence ‘RCA’ oxide desorption in H2 100 sccm 1Torr 950ºC Pump-down chamber to 10-3 Torr Si high T buffer from pure SiH4 100 sccm 1Torr 5 min 2 min 30s 40 s 40 s 650ºC 4 min 3 different durations Time Temperature Pump-down chamber to 10-3 Torr Lower temperature to 650ºC at 10-3 Torr (standard set) Lower temperature to 650ºC in H2 100 sccm 1Torr (preconditioned set) Ge self-assembled islands from GeH4 (10.2% in H2) 30 sccm 0.5 Torr
  • 6. University of Southampton University of Southampton Characterisation techniquesCharacterisation techniques  Rutherford backscattering spectrometry (RBS) in ‘random’ orientation  Atomic force microscopy (AFM) tapping mode  Micro-Raman spectroscopy ( Raman) inμ backscattering configuration
  • 7. University of Southampton University of Southampton RBS resultsRBS results 0 2 4 6 8 10 0 2 4 6 8 10 12 14 Growth duration (s) Gesurfacecoverage (ML) Standard Preconditioned wetting layer
  • 8. University of Southampton University of Southampton AFM results (shortest duration)AFM results (shortest duration) Mixed islands: 7 mμ -2 Small height: 5-10 nm (97%) width: 30-50 nm Large height: 70 nm width: 300 nm PreconditionedStandard Small islands: 4 mμ -2 Narrow size distribution Height: 3-8 nm Width: 20-40 nm
  • 9. University of Southampton University of Southampton AFM results (intermediate duration)AFM results (intermediate duration) Preconditioned Mixed islands: 10 mμ -2 Bimodal size distribution Small height: 8-15 nm (62 %) width: 50-100 nm Large height: 20-30 nm width: 120-200 nm Standard Mixed islands: 3 mμ -2 Bimodal size distribution Small height: 5-8 nm (70%) width: 30-50 nm Large height: 20-40 nm width: 100-180 nm
  • 10. University of Southampton University of Southampton AFM results (longest duration)AFM results (longest duration) Preconditioned Mixed islands: 11 mμ -2 Bimodal size distribution Small height: 8-20 nm (54%) width: 50-100 nm Large height: 25-40 nm width: 150-200 nm Standard Mixed islands: 7 mμ -2 Bimodal size distribution Small height: 10-20 nm width: 100-120 nm Large height: 25-40 nm (60%) width: 200-250 nm
  • 11. University of Southampton University of Southampton ISi-Ge/IGe-Ge= 2(1-x)/Bx ISi-Ge , IGe-Ge intensities of the Si-Ge and Ge-Ge peaks B = 2.218 wGe-Ge = 282.5 + 16x - 384ε wGe-Ge shift of the Ge-Ge peak x Ge concentration (%) ε strain  Diffusion activation barrier for Ge adatoms on a strained Ge (001) surface increases with compressive strain A. Van de Walle, M. Asta, P.W. Voorhees, Phys. Rev. B 67, 041308 (2003)  The periphery of the island is the location of the highest strain P. Raiteri, L. Miglio, F. Valentinotti, M. Celino, Appl. Phys. Lett. 80(20), 3736 (2002) Raman resultsμRaman resultsμ Sample Ge conc. (%) Strain (%) d[Ge]/dt (%/s) QD2H 53 -1.649 QD3H 47 -1.264 -3.0 Sample Ge conc. (%) Strain (%) d[Ge]/dt (%/s) QD2 52 -1.045 QD3 55 -0.928 +1.5 Standard Preconditioned
  • 12. University of Southampton University of Southampton Summary and conclusionsSummary and conclusions standard samplesstandard samples RBS, AFM and Raman results on Ge self-assembledμRaman results on Ge self-assembledμ islands on two types of Si surfaces:islands on two types of Si surfaces: 1. Standard well-known steady evolution: - low density of small islands, narrow size distribution - bimodal size distribution resulted from ripening: - small islands still dominate - strain in the large islands is relived trough intermixing - predominantly large islands in which strain is relieved through both intermixing and defect formation
  • 13. University of Southampton University of Southampton Summary and conclusionsSummary and conclusions preconditioned samplespreconditioned samples 2. Preconditioned very accelerated initial evolution, which then saturates:  The addition of H2 during the ramp-down preserves a non- equilibrium surface morphology: - double the density of slightly larger islands (narrow size distribution) + a very low density of unusually large island (still under study) - increase in the density and size through nucleation and growth; misfit strain relaxes through intermixing  During the final stages, evolution slows down because of the high compressive strain in the deposited layer : - saturation of the nucleation and growth; misfit strain increases intermixing increases