Transcript Slide 1

EBB 323 Semiconductor
Fabrication Technology
Epitaxy
Dr Khairunisak Abdul Razak
Room 2.16
School of Material and Mineral Resources Engineering
Universiti Sains Malaysia
[email protected]
Topic outcomes
At the end of this topic, students
should be able to:
• Name 2 types of epitaxy
• Describe the applications of
epitaxial layers
• Explain techniques to produce
epitaxial layers
• Describe structure and defects in
epitaxial layers
Introduction
•
Epitaxy comes from Greek words:
–
–
•
Epi: upon
Taxis: ordered
Epitaxial growth: single crystal growth of a
material in which a substrate serve as a seed
2 types of epitaxy:
•
1.
2.
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Homoepitaxy – material is grown epitaxially on a
substrate of the same material. E.g. grow of Si on Si
substrate
Heteroepitaxy – a layer grown on a chemically different
substrate. E.g. Si growth on sapphire
Similar crystal structures of the layer and the
substrate, BUT
–
–
The shift of composition causes difference in lattice
parameters
Limit the ability to produce epitaxial layers of
dissimilar materials
Film deposited on a
<111> oriented wafer
<111> orientation
The presence of SiO2
Layer cause depositing
atoms have no
structurepolysilicon
Epitaxial and polysilicon film growth
Applications of epitaxial layers
1. Discrete and power devices
2. Integrated circuits
3. Epitaxy for MOS devices
1. Discrete and power devices
• Technology change: junction transistors 
diffused planar structure
– Requires a material structure that are not achieved by
diffusion of dopants from the surface
• Si epitaxy was developed to enhance the electrical
performance of discrete bipolar transistors
• Breakdown voltage of the discrete transistor was
limited by the field avalanche breakdown of the
substrate material
– Use higher resistivity substrates produced higher
breakdown voltages but increased collector series
resistance
• Structure needed: thin, lightly doped and single
crystal layer of high perfection upon more heavily
doped Si substrate
– But, the use of a more heavily doped substrate reduces
the collector series resistance while the base-collector
breakdown voltage is governed by the lighter doping in
the near surface region
• Epitaxial deposition of a lightly doped P+ epitaxial
layer on a N+ substrate make the desired
properties are achievable
• Epitaxial grows also allows accurate control of
doping levels and advantages which arises from
a generally low oxygen and carbon levels in
epitaxial layer
• Epitaxial technique was developed to 2 and 3
layers epitaxial structure
– For lightly doped area of collector
– Based region was also grown epitaxially
• E.g. of multilayer structures: Si-Controlled
Rectifier (SCR), Triac, high voltage or high power
discrete products
Mesa discrete transistor fabricated in an epitaxial
layer on a heavily doped N+ substrate
Transistors
Diodes
2. Integrated circuit (IC)
• Development of planar bipolar IC caused the requirement for
devices built on the same substrate to be electrically
isolated
– The use of opposite typed substrate and epitaxial layer
met part of the requirement
– Device isolation was completed by the diffusion of
“isolation” region through the epitaxial layer to contact
the substrate between active areas
• In planar bipolar circuits, common to employ a heavily
doped diffused (or implanted) region under the transistor
– Usually called ‘buried layer’ or ‘DUF’ for diffusion under film
– The buried layer
• serves to lower the lateral series resistance between collector area
below the emitter and the collector contact
• produce uniform planar operation of the emitter, avoiding current
crowding which leads to hot spots near edges of the emitter
Integrated circuits
(a) A junction isolated bipolar
device fabricated as part of an
integrated circuit using a buried
layer subcollector and a lightly
doped n-epitaxial layer
(b) An N-Well CMOS structure
fabricated in a lightly doped pepitaxial layer
3. Epitaxy for MOS devices
• Unipolar devices such as junction fieldeffect transistors (JFETs), VMOS, DRAMs
technology also use epitaxial structures
• VLSI CMOS (complimentary metal-oxidesemiconductor) devices have been built in
thin (3-8 micron) lightly doped epitaxial
layers on heavily doped substrates of the
same type (N or P)
– That epitaxial structure reduces the “latch up”
of high density CMOS IC by reducing the
unwanted interaction of closely spaced devices
Advantages of epitaxy
• Ability to place a lightly oppositely
doped region over a heavily doped
region
• Ability to contour and tailor the
doping profile in ways not possible
using diffusion or implantation alone
• Provide a layer of oxygen free
material that is also contained low
carbon
Techniques for silicon epitaxy
1.
2.
3.
4.
Chemical Vapour Deposition (CVD)
Molecular Beam Epitaxy (MEB)
Liquid Phase Epitaxy (LPE)
Solid phase regrowth
1. Chemical Vapour Deposition (CVD)
• The most common technique in Si epitaxy
• In the CVD technique
– Si substrate is heated in a chamber: sufficient
heat to allow the depositing Si atoms to move
into position to
– Reactive Si containing gaseous compounds
are introduced
– Gaseous react on the hot surface of the
substrate and deposit a Si layer
– The deposit will take on Si substrate structure
if the substrate is atomically clean and the
temperature is sufficient for atoms to have
surface mobility
Schematic drawing of a simple horizontal flow, cold
wall, CVD reactor
Schematic CVD reactor geometries for
(a) True vertical reactor
(b) Classic horizontal flow reactor
(c) Modified vertical (or pancake) reactor
(d) Downflow cylinder reactor
CVD processes and products
CVD for silicon devices
CVD reactions
1.
Pyrolysis: chemical reaction is driven by heat alone, e.g.
silane decomposes with heating
SiH4  Si + 2H2
2.
Reduction: chemical reaction by reacting a molecule
with hydrogen, e.g. silicon tetrachloride- reduction in
hydrogen ambient to form solid silicon
SiCl4 + 2H2  Si + 4HCl
3.
Oxidation: chemical reaction of an atom or molecule
with oxygen, e.g. SiH4 decomposes at lower temperature
SiH4 + O2  SiO2 + 2H2
4.
Nitridation: chemical process of forming silicon nitride
by exposing Si wafer to nitrogen at high temperature e.g.
SiH2Cl2 readily decomposes at 1050C
3SiH2Cl2 + 4NH3  Si3N4 + pH + 6H2
CVD
CVD film growth steps
1.
Nucleation
•
Dependent on substrate quality
•
Occurs at first few atoms or molecules deposit on a
surface
2.
Nuclei growth
•
Atoms or molecules form islands that grow into larger
islands
3.
Island coalescence
•
The islands spread , and coalescing into a continuous
film
•
This is the transition stage of the film growth,
thickness several hundreds Angstroms
•
Transition region film possesses different chemical
and physical properties for thicker bulk film
4.
Bulk growth
•
Bulk growth begins after transition film is formed
CVD film growth steps
Types of film
structure
Amorphous
Polycrystalline
Single crystal
Basic CVD subsystem
• CVD Process steps:
Pre-clean
Deposition
Evaluation
• Pre-clean: remove particulates and mobile ionic
contaminants
• Deposition:
Load wafer into
chamber, inert
atmosphere
Heat
Introduce
chemical
vapour
• Evaluation: thickness, step coverage, purity,
cleanliness and composition
Remove vapour
Flush excess
chemical
vapour source
2. Molecular Bean Epitaxy (MBE)
• Uses an evaporation method
• MBE is carried out at a lower temperature than
1000-1200C (typical CVD temperature)
– Reduces outdiffusion of local areas of dopant
diffused into substrates and reduce autodoping
which is unintentionally transfer of dopant into
epitaxial layer
• MBE is favourable
– preparation of sub-micron thickness epitaxial layers or
– high frequency devices requiring hyper-abrupt transition
in the doping concentration between the epitaxial layer
and the substrate
• In MBE,
– Si and dopant(s) are evaporated in an ultra high vacuum
(UHV) chamber
– The evaporated atoms are transported at relatively high
velocity in a straight line from the source to the substrate
– They condense on the low temperature substrate
– The condensed atoms of Si or dopant will diffuse on the
surface until they reach a low energy site that they fit
well the atomic structure of the surface
– The “adatom” then bonds in that low energy site,
extending the underlying crystal by a vapour to solid
phase crystal growth
– Usual temperature range of the substrate is 400-800C.
Higher than 800C is possible but it will increase
outdiffusion or lateral diffusion of dopants in the
substrate
Schematic drawing of a molecular beam
epitaxial system
• Insitu cleaning of the substrate
– Can be done by high temperature bake at 1000-1250C
for several minutes under high vacuum to decompose
the native surface oxide and to remove other surface
contaminants
– Other technique is by using a low energy beam of inert
gas to sputter clean the substrate
– Difficult to remove carbon but will decrease at the
surface by diffusion into the substrate during short
anneal at 800-900C
• Wider range of dopants for MBE than CVD
epitaxy:
– Typical dopants: Antimony, Sb (N-type), aluminum, Al or
gallium (Ga) for P-type
– N-type dopant: As and P, evaporate rapidly even at
200C. Difficult to control
– P-type dopant: Boron, evaporate slowly even at 1300C
Schematic drawing of a multiple chamber MBE
system
MBE Equipment
Liquid Phase Epitaxy (LPE)
• LPE technique is widely used for preparation of
epitaxial layers on compound semiconductors
and for magnetic bubble memory films on garnet
substrate
• In films growth by LPE from solution melts, low
cooling rates, when the surface reaction (growth)
• Kinetics are rapid compare to the mass transport
of Si to the seed, epitaxial layer thickness will vary
in proportion to the temperature drop
• Increase cooling rates, mass transport rate will
increase and the growth rate will increase with
cooling rate until growth rate becomes limited by
surface reaction kinetics
• Growth rate increases with
cooling rate up to about 1
degree/min while growth rate
above 2 degree/min occurred
under kinetically limited
conditions
LPE growth rate increasing with
cooling rate up to about 1 micron per
minute
Schematic drawing of a typical silicon liquid
phase epitaxy (LPE)
•Fabrication sequence for a vertical
channel field effect transistor
•N and N+ epitaxial structure can be
built using liquid or vapour phase
epitaxial growth
•Preferential etching can be used to
open areas part way through the N
type epitaxial layer
• In this figure, LPE is used to fill the
etched out gate areas which control
current flow vertically from the top
side source to the N+ substrate drain
region
Schematic of fabrication steps in the fabrication
vertical field effect transistors by etch and LPE refill
techniques
4. Solid Phase Re-growth
i.
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•
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Re-growth of amorphous layers
Surface layers subjected to high dose ion
implants are in amorphous structure due to the
heavy damage inflicted on the lattice as the
energetic ions are absorbed
Annealing above 600C  amorphous layer recrystallize
Re-crystallisation occurs from interface moves
toward the surface and results in solid phase
epitaxial re-growth
ii.
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•
•
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Re-crystallisation of thin films
Involves re-crystallisation of a deposited amorphous or
polysilicon film
Si film is deposited on a Si substrate or more commonly
SiO2  heated using a strip heater passed over the
surface or by a scanned pulsed laser to crystallise the
film to single crystal or large grain polysilicon
This fabrication technique is used to produce a stacked
n-channel device in re-crystallised polysilicon on a
thermally grown or deposited oxide
Oriented epitaxial growth can be obtained by making
series of holes in the oxide to allow points of contact
between the underlying substrate and the deposited
polysilicon
The contact points become “seeds” areas for
establishing re-growth orientation
Re-crystallisation solid phase
epitaxy using a moving strip heater
A stacked MOS structure over an
insulating oxide fabricated in a recrystallised polysilicon layer
Structure and defects in epitaxial layer
•
Surface morphology of Silicon epitaxial
deposits is affected by growth and substrate
parameters
Growth parameters:
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–
–
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Temperature
Pressure
Concentration of Si containing gas
Cl : H2 ratio
Substrates parameters
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Substrate orientation
Defects in the substrate
Contaminants on the surface of the substrate
Typical defects in epitaxial layers
1.
2.
3.
4.
5.
Substrate orientation effects
Spikes and epitaxial stacking faults
Hillocks and pyramids in epitaxial layers
Dislocations and slip
Microprecipitates (S-pits)
1. Substrate orientation effect
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Growth of smooth epitaxial films can be
obtained on (100) and (110) oriented Si
substrates
Epitaxial growth on substrate surface on
oriented on (111) plane results in facetted
“alligator skin” surface
•
–
–
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(111) surfaces contain no atomic steps to provide a
density of growth sites
Without atomic steps, the growth produces pyramids
and terraces
Misorientation of the surface by  0.5 degree
introduces a sufficient density of steps for
growth of smooth planar films
2. Spikes and epitaxial stacking faults
i.
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•
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•
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Growth spike
Originate from Si particle on the surface not
removed by the pre-epitaxial cleaning process
Si Chips may expose faster growing crystal
planes than the plane of the substrate
Chips nucleate and produce polysilicon nodule.
The chips then protrude above the substrates
surface into a region of richer supply of
gaseous reactants
Results in nodule grows at 2-10 times the rate
of epitaxial film on the substrate.
May be removed mechanically before the next
step but will leave a region unusable for
functional materials
ii.
•
•
Epitaxial stacking faults
Crystallographic in nature and arise from
defects in atomic arrangement during film
growth
Could result from an extra atomic layer
(extrinsic fault) or a missing atomic layer
(intrinsic fault) along {111} type plane
Epitaxial growth spike
Stacking fault on <111> Si
3. Hillocks and pyramids in epitaxial layers
•
•
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Hillocks: Small oval mounds on the surface of
the epitaxial
Pyramids: Faceted regions on the epitaxial
surface
Density of hillocks and pyramids is dependent
on growth parameters such as type and
concentration of Si source and deposition
temperature
4. Dislocations and slip
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Non-uniform heating of a substrate results in non-uniform
thermal expansion of the substrate which produces
elastic stresses
The thermal stress can cause bowing which may lift the
edge of the substrate away from the substrate in
response to the thermal stress
At lower temperature (< 900C) the yield point of the Si
lattice is sufficiently high that the substrate behaves
elastically. During cooling, the thermal stress is removed
and the substrate returns to its original shape
If the stress exceeds a critical values, the substrate will
yield plastically  occurs due to generation and motion
of dislocations which are atomic level line defects which
glide along slip planes of the crystal
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•
•
•
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The passage of one dislocation offsets the material above
and below the slip plane by a unit known as “Berger’s
vector” of the dislocations
Dislocations normally propagate from near the edge of
the substrate (highest stress), and glide towards the
centre of the substrate and produce plastic deformation
of the substrate which relieves the thermal stress
Dislocation motions is slow because dislocation moves
to a region of lower shear stress
The continuous slow motion of the dislocations produces
“creep” deformation of the crystal
Device impact from slip normally comes from rapid “pipe
diffusion” of dopant along the core of the dislocations
Crystal slip
Typical wafer edge slip as a
result of excessive within
wafer temperature
gradients during heating or
during epitaxial film growth
5. Microprecipitates (S-pits)
•
•
•
Microprecipitates may come from metallic
elements such as copper, nickel, iron and
chromium
This is due to their solubility in Si at high
temperatures and fast diffusion rates through
the Si
The metal contaminants may exist in the
starting substrates or being pick up during
handling in the loading operation or from metal
parts or susceptors within the epitaxial reactor
itself