Title: Fabrication of GaAs on Si heterostructures by hydrogen implantation and
1Fabrication of GaAs on Si hetero-structures by
hydrogen implantation and direct wafer
bonding 06. 09. H.J. Woo, H.W. Choi, G.D.
Kim, W. Hong, J.K. Kim, H.R. Lee Ion Beam
Application Group, KIGAM, Korea
IBA GROUP
2Introduction
- GaAs on Si technology presents a huge potential
of interest as it combines the superior
electrical and optical properties of GaAs with
the mechanical and economical advantages and
density of integration of silicon. - To obtain this structure, hetero-epitaxial growth
has been investigated extensively, but due to the
large lattice mismatch (4), an unacceptable
high density (typically gt 107/cm2) of threading
dislocations could not be avoided. - Ion-cut concept based on ion implantation and
direct wafer bonding is recognized as a major
breakthrough to obtain this structure from
technical and economical points of view. - The aim of this paper is to investigate the role
of implant temperature and ion fluence on
blistering of the surface after a subsequent
annealing in detail, and to develop ion-cut
process allowing GaAs thin film to be transferred
onto a full silicon wafer.
3Ion-cut process flows for GOI wafers fabrication
Si cleaning
SiO2 deposition on GaAs 300-400 nm PECVD CMP
SOG (300-500 nm) Deposition baking (180?)
Si cleaning
- Proton implantation
- fluence 1.01.6x1017 H/cm2
- implant temp. 120160?
- He-H co-implantation
- He, low dose, RT
- H, high dose, RT
GaAs cleaning
RT bonding
Low-temp. ion-cut splitting (200-230?, 10-15 h)
high-temp. annealing CMP polishing
4Ion-cut technology
Ion implantation technology (precise definition
of layer thickness)
Wafer bonding technology (keeping the original
GaAs quality)
Ion-cut GOI wafers
Schematic of the ion-cut process
for GaAs-on-insulator wafers fabrication
5Hydrogen ion implantation
- GaAs wafer semi-insulating (100) oriented, 2"
GaAs - Fluence range 4.0x1016 2.0x1017 H/cm2
- Implant temperature (on wafer surface) 40300?
- Ion flux 1.0x1013 H cm-2s-1
Low Energy Implantation System
Inner view of the target chamber
6Estimated depth profile of hydrogen concentration
for a fluence of 8x1016 H/cm2 at 40 keV in GaAs
wafer
Hydrogen concentration profiles in GaAs implanted
with 8x1016 H/cm2 at different temperatures as
determined by the SIMS analysis.
7Optical microscopic images after proton
implantation (40 keV, 1.6x1017 H/cm2) and/or
annealing. a) as-implanted at 140?, and implanted
at 120? and annealed for 30 min. b) at 300? and
(c) at 400?.
FE-SEM micrographs of GaAs surface with 40 keV
1.6x1017 H/cm2 implant at 120?, following the
annealing step at a) 300? for 30 min and b) 400?
for 60 min.
2 µm
2 µm
8Optimum condition for ion-cut
Approximate temperature windows for microcrack
development by hydrogen ion implantation
9Fluence and temp. boundaries of blister formation
in hydrogen- implanted GaAs
- New optimum temperature window 120160?
- Optimum fluence range 1.0x1017 1.6x1017 H/cm2
10Lattice damage profiling
Random and aligned RBS/channeling spectra for
GaAs single crystals implanted at different
temperatures
11Examination of microstructure
a)
b)
Cross section TEM images GaAs wafer a) after
hydrogen implantation (40 keV, 1.2x1017 cm-2) at
140? and b) after annealing at 300?
Platelet (microcrack, microcavity)
12Rq 12 nm
396 nm 273 nm
GaAs SiO2/SiNx Silicon
FE-SEM image of a transferred GaAs layer onto
silicon wafer via a PECVD oxide layer.
13Summary
- The GaAs ion-cut process is sensitive to both the
implant temperature and the fluence. At low
implant temperature (lt100?), hydrogen is unable
to form into the defect structure responsible for
blistering, and if the temperature is too high,
the platelets are not able to evolve and
blistering is less prolific because of the
out-diffusion of hydrogen. - It was found that the optimum implant temperature
window lie in 120160?, which is relatively lower
than the previously reported implant temperature
window probably due to the inaccuracy in
temperature measurement in other laboratories. - Thin GaAs layer was successfully transferred onto
a 100 mmF silicon wafer at 250?, and low
temperature splitting is of importance for layer
transfer between dissimilar materials with very
different thermal expansion coefficients as well
as for processed wafers containing
temperature-sensitive devices.