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Lect' 21 Epitaxy

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Title: Lect' 21 Epitaxy


1
Lect. 21 Epitaxy
  • The term epitaxy (Greek epi "above" and taxis
    "in ordered manner") describes an ordered
    crystalline growth on a monocrystalline
    substrate.
  • Epitaxial films may be grown from gaseous or
    liquid precursors. Because the substrate acts as
    a seed crystal, the deposited film takes on a
    lattice structure and orientation identical to
    those of the substrate.
  • This is different from other thin-film deposition
    methods which deposit polycrystalline or
    amorphous films, even on single-crystal
    substrates.
  • If a film is deposited on a substrate of the
    same composition, the process is called
    homoepitaxy otherwise it is called
    heteroepitaxy.
  • Homoepitaxy is a kind of epitaxy performed with
    only one material. In homoepitaxy, a crystalline
    film is grown on a substrate or film of the same
    material. This technology is applied to growing a
    more purified film than the substrate and
    fabricating layers with different doping levels.
  • Heteroepitaxy is a kind of epitaxy performed with
    materials that are different from each other. In
    heteroepitaxy, a crystalline film grows on a
    crystalline substrate or film of another
    material. This technology is often applied to
    growing crystalline films of materials of which
    single crystals cannot be obtained and to
    fabricating integrated crystalline layers of
    different materials. Examples include gallium
    nitride (GaN) on sapphire or aluminium gallium
    indium phosphide (AlGaInP) on gallium arsenide
    (GaAs).

2
Epitaxy
Metastable phase
Transient layer
_at_ t1gtto
_at_ to
Stable phase (crystal)
Nuclei of Crystal phase
Crystallizationinterface
At time to, the before the epitaxy takes place
At the nucleation stage where thefirst crystal
layer is being formed
_at_ t3gtt2
_at_ t2gtt1
Transient layer
Transient layer
Local homoepitaxial interface
Nuclei of Crystal phase
Grown epitaxial layer
Grown epitaxial layer
Crystallizationinterface
Crystallizationinterface
Early stage of epitaxial growth
Hetroepitaxial interface
Epitxy proceeds
3
Epitaxy
  • The key processes of epitaxial growth are-
    Perpendicular mass transport from the bulk
    metastable phase material to the crystallization
    interface.- Lateral mass transport through
    lateral migration according to expitaxial order.
    - desorption from the crystallization area
    towards the bulk phase material.
  • The lattice constant of the epitaxially grown
    layer needs to be close to the lattice constant
    of the substrate wafer. Otherwise the bonds can
    not stretch far enough and dislocations will
    result.
  • Experimentally, it has proven that epitaxy growth
    occurs when the lattice misfit, defined as
    , is less than 15
  • MethodsEpitaxial silicon is usually grown
    using- vapor-phase epitaxy (VPE), a
    modification of chemical vapor deposition. -
    Molecular-beam (MBE)- liquid-phase epitaxy (LPE)
    are also used, mainly for compound semiconductors.

af
dislocation
as
Dislocation due to the difference betweenthe
substrate (s) and film (f) lattice constants
Film Substrate
() Epitaxy Physical Principles and Technical
Implementation  By Marian A. Herman, Wolfgang
Richter, Helmut Sitter
4
Epitaxy
  • The growth rate in Vapor phase deposition (VPE)
    epitaxy follows the same model as CVD.

Ref http//www2.ece.jhu.edu/faculty/andreou/495/2
007/LectureNotes/Handout7_Thin20Film20Deposition
.pdf
5
Epitaxy
  • Silicon is most commonly deposited from silicon
    tetrachloride in hydrogen at approximately 1200
    C
  • SiCl4(g) 2H2(g) ? Si(s) 4HCl(g)
  • This reaction is reversible, and the growth rate
    depends strongly upon the proportion of the two
    source gases. Growth rates above 2 micrometres
    per minute produce polycrystalline silicon, and
    negative growth rates (etching) may occur if too
    much hydrogen chloride byproduct is present. In
    fact, hydrogen chloride may be added
    intentionally to etch the wafer. An additional
    etching reaction competes with the deposition
    reaction
  • SiCl4(g) Si(s) ? 2SiCl2(g)
  • Silicon VPE may also use silane, dichlorosilane,
    and trichlorosilane source gases. For instance,
    the silane reaction occurs at 650 C in this way
  • SiH4 ? Si 2H2
  • This reaction does not inadvertently etch the
    wafer, and takes place at lower temperatures than
    deposition from silicon tetrachloride. However,
    it will form a polycrystalline film unless
    tightly controlled, and it allows oxidizing
    species that leak into the reactor to contaminate
    the epitaxial layer with unwanted compounds such
    as silicon dioxide.
  • VPE is sometimes classified by the chemistry of
    the source gases, such as hydride VPE and
    metalorganic VPE.

6
Lect. 22 Epitaxy
  • Molecular beam epitaxy is a technique for
    epitaxial growth via the interaction of one or
    several molecular or atomic beams that occurs on
    a surface of a heated crystalline substrate.
  • Molecular Beam Epitaxy takes place in high vacuum
    or ultra high vacuum (10-8 Pa).
  • The most important aspect of MBE is the slow
    deposition rate (1 to 300 nm per minute), which
    allows the films to grow epitaxially.
  • The slow deposition rates require proportionally
    better vacuum in order to achieve the same
    impurity levels as other deposition techniques.
  • In solid-source MBE, ultra-pure elements such as
    gallium and arsenic are heated in separate
    quasi-knudsen effusion cells until they begin to
    slowly sublimate.
  • A typical Knudsen cell contains a crucible (made
    of pyrolytic Boron Nitride, quartz, tungsten or
    graphite), heating filaments (often made of metal
    Tantalum), water cooling system, heat shields and
    orifice shutter.
  • The gaseous elements then condense on the wafer,
    where they may react with each other. In the
    example of gallium and arsenic, single-crystal
    gallium arsenide is formed.
  • The term "beam" simply means that evaporated
    atoms do not interact with each other or any
    other vacuum chamber gases until they reach the
    wafer, due to the long mean free paths of the
    beams.

Refhttp//www-opto.e-technik.uni-ulm.de/forschung
/jahresbericht/2002/ar2002_fr.pdf
7
Epitaxy
  • the molecular beam condition that the mean free
    path of the particles
    should be larger than the geometrical size of
    the chamber is easily fulfilled if the total
    pressure does not exceed 10-5 Torr.
  • Also, the condition for growing a sufficiently
    clean epitaxial layer must be satisfied, e.g.
    requiring for the monolayer deposition times of
    the beams tb and the background residual vapor
    tres the relation tres lt 10-5 tb.
  • For a typical gallium flux J of 10-19 atoms/m2s
    and for a growth rate in the order of 1 ?m/h, the
    conclusion is that pres 10-11 Torr.
  • Thus, UHV is the essential environment for MBE.
    Therefore, the rate of gas evolution from the
    materials in the chamber has to be as low as
    possible.
  • So pyrolytic boron nitride (PBN) is chosen for
    the crucibles which gives low rate of gas
    evolution and chemical stability up to 1400 C.
  • molybdenum and tantalum are widely used for the
    shutters, the heaters and other components, and
    only ultrapure materials are used as source.
  • The operation time of a shutter of approximately
    0.1 s is normally much shorter than the time
    needed to grow one monolayer (typically 1 to 5 s)

8
Epitaxy
  • Reflection high-energy electron diffraction
    (RHEED) is a technique used to characterize the
    surface of crystalline materials.
  • RHEED systems gather information only from the
    surface layer of the sample, which distinguishes
    RHEED from other materials characterization
    methods that rely on diffraction of high-energy
    electrons.
  • Transmission electron microscopy, another common
    electron diffraction method samples the bulk of
    the sample due to the geometry of the system.
  • A RHEED system requires an electron source (gun),
    photoluminescent detector screen and a sample
    with a clean surface, although modern RHEED
    systems have additional parts to optimize the
    technique.
  • The electron gun generates a beam of electrons
    which strike the sample at a very small angle
    relative to the sample surface.
  • Incident electrons diffract from atoms at the
    surface of the sample, and a small fraction of
    the diffracted electrons interfere constructively
    at specific angles and form regular patterns on
    the detector.
  • The electrons interfere according to the position
    of atoms on the sample surface, so the
    diffraction pattern at the detector is a function
    of the sample surface.

9
Epitaxy
y
k2
k1
k0
x
ko
  • The oscillation of theRHEED signal
    exactlycorresponds to the timeneeded to grow a
    monolayer and thediffraction pattern on the
    RHEED window gives direct indicationover the
    state of the surface
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