Page 415 - Academic Press Encyclopedia of Physical Science and Technology 3rd Chemical Engineering
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 Encyclopedia of Physical Science and Technology  EN009J-427  July 6, 2001  20:25






               500                                                                      Metalorganic Chemical Vapor Deposition


               “injector” or point of origin and the substrate surface with-  taxial films. These low-pressure MOCVD systems operate
               out interacting with any other molecules (especially im-  under controlled pressures using chemical-series vacuum
               purities like O 2 or CO 2 ).                      pump systems (now “dry” oil-free pumps are often used)
                                                                 to pull the reactants through the chamber at high gas ve-
                                                                 locities, thus reducing the boundary layer thickness and
                 3. Precursor Selection
                                                                 reducing the gas switching time in the chamber. The first
               The metalorganic precursor compounds that have been  work on low-pressure MOCVD (LP-MOCVD) was re-
               most commonly used to grow thin films of semiconduc-  ported by J. P. Duchemin et al. (Thompson CSF, France) in
               tors and related materials are listed below in Table I, along  1979, who reported the growth of InP using triethylindium
               with the currently available vapor pressure data. These  (TEIn) and PH 3 , and GaAs using triethylgallium (TEGa)
               precursors are typically pyrophoric liquids or high-vapor-  and AsH 3 ,at ∼100 Torr (∼13 kPa) in a horizontal re-
               pressure solids. The simple metal alkyls (methyl and ethyl  actor. This same group also reported the growth of In-
               derivatives) are the most often employed for the growth  GaAsP alloys lattice-matched to InP at low pressure using
               of III–V compound semiconductors since they have rea-  TEGa, TEIn, PH 3 , and AsH 3 . Using LP-MOCVD, they
               sonably high vapor pressures and can be readily delivered  also grew the first InGaAsP/InP injection lasers produced
               using a H 2 carrier gas and precursor source temperatures  by MOCVD.
               conveniently near room temperature.                 The MOCVD reactors that are in primary use today
                 These compounds are synthesized, purified, and loaded  are generally of one of two types: (1) a cylindrical cold-
               under well-controlled conditions into specially designed  wall stainless-steel reactor chamber using high-speed ro-
               and prepared all-welded stainless-steel vessels. The met-  tation (R rot ≥ 500 rpm) of a resistance-heated molybde-
               alorganic precursors are transported by passing a con-  num or graphite wafer carrier inside the chamber. Most
               trolled flow of the carrier gas through the precursor storage  current-generation vertical-geometry reactors using high-
               vessel and transporting the resulting vapor-phase mixture  speed rotation to produce a uniform temperature pro-
               into a gas mixing system, commonly referred to as the “in-  file, a thin boundary layer, and well-developed laminar-
               jection manifold” that is, in turn, connected to a mixing  flow gas streamlines. These chambers are based on the
               region at the inlet to the reaction chamber. The various  classical RDR (see Fig. 4). Or (2) a rectangular cross-
               precursor gases are again mixed with a high volume of  section cold-wall quartz-walled chamber employing RF
               the carrier gas and enter the “input zone” of the reaction  or lamp heating of a graphite susceptor that, in addi-
               chamber. The gas mixture passes over the heated substrate  tion to the rotation of the main “wafer platter,” employs
               and thermally driven chemical reactions occur, both in the  “gas-foil” rotation of individual wafers (R rot ∼ 1–3 rpm)
               gas phase (i.e., homogeneous reactions) and at the vapor–  to  improve  the  uniformity  of  the  growth  (see  Fig.  5).
               solid interface (i.e., heterogeneous reactions). Often the  Advanced horizontal-geometry reactors of this type are
               homogeneous reactions can lead to the formation of un-  also available commercially. The large chambers of this
               desirable intermediate compounds (e.g., adducts) formed
               between the Column III and Column V precursors. These
               adducts typically have extremely low vapor pressures and
               do not react to produce epitaxial materials, resulting in a
               reduction in the effective molar flow of useable precursors
               and a corresponding reduction of the growth rate.


                 4. General Description of MOCVD
                    Growth Systems
               The early vertical-geometry MOCVD reactors operated at
                                            5
               atmospheric pressure (760 Torr or 10 Pa) and consisted of
               a quartz chamber with a slowly rotating (∼5–20 rpm) SiC-
               coated graphite “susceptor” upon which the substrate was
               placed. Atmospheric-pressure horizontal growth systems
               employing circular cross section quartz chambers were
               also used. In most cases, induction heating of the graphite  FIGURE 4 Schematic diagram of a typical large-scale high-
               susceptor was provided by an RF generator.        speed vertical rotating-disk MOCVD reactor chamber including a
                                                                 simplified view of gas flow in a vertical RDR. The inlet gas stream
                 Today, most multiple-wafer MOCVD systems are op-
                                                                 contains the precursor flows and the main carrier gas flow. Typi-
               erated at sub-atmospheric pressure, in the 20–300 Torr  cally, the Column V and Column III sources are kept separate until
               (2.6–40 kPa) range to improve the uniformity of the epi-  a few inches above the heated susceptor.
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