MOLECULAR BEAM EPITAXIAL APPARATUS

Abstract: A molecular beam epitaxial apparatus comprising a growth chamber having a sink opening for exhaustion and a cooled inner wall and which has a shape, for example a paraboloid of revolution or truncated cone, such that the overall inner wall faces the sink opening; one or more molecular beam sources for leading one or more required molecular beams into the growth chamber; and a holder for a substrate which is arranged in the growth chamber in the lead-in direction of the molecular beam or beams and which has a structure such that the molecular flow which is reflected or reevaporated after it has been adsorbed by the substrate holder is directed into the sink opening. Parts of the molecular beam or beams reflected or reflected or reevaporated from the substrate are further reflected or reevaporated by the inner wall, so that a plurality of additional (i.e., secondary, ternary, ...) molecular beams are generated. These additional molecular beams are also directed into the sink opening. An auxiliary exhaust apparatus may be provided to ensure that the molecular beam portions which are unnecessary for the crystal growth, but which remain due to various attached apparatuses which are disposed in the growth chamber, are directed into the sink opening.

Description: The present invention relates to a molecular beam epitaxial (MBE) apparatus. A molecular beam epitaxial apparatus for growing a crystal by irradiating molecules or atoms onto a crystalline substrate under a ultra-high vacuum (UHV) condition is known. A conventional molecular beam epitaxial apparatus is constructed in the following manner. Namely, as shown in Fig. 1, a crystalline substrate 32 is supported in a vacuum growth chamber 31. Furnaces 33 l to 33 n of a plurality of kinds of elements are provided for the substrate 32. An epitaxial layer is grown on the heated substrate 32 by directing the molecular beams from desired furnaces under UHV conditions. Such a molecular beam epitaxial apparatus has the feature that a combination of molecular beams can be varied by mechanical shutters, so that multiple layers of different kinds of compound crystals can be sequentially grown in a direction corresponding to the thickness of the substrate on an atomic layer unit basis. In the conventional molecular beam epitaxial apparatus, in general, the degree of vacuum (partial pressure) deteriorates by one or two orders of magnitude for example, to the value of 10⁻⁹ to 10⁻⁸ Torr) during the growth of the crystal as compared with the degree of vacuum (total pressure) (e.g., 10⁻¹⁰ Torr) before the molecular flow is introduced for the crystal growth. This is because the molecular flow is introduced into the growth chamber 31 and added to the outgases in the growth chamber 31, so that the number of molecules to be exhausted increases. Such a conventional MBE apparatus is unsuitable for forming a device having a multilayer structure of a compound semiconductor as shown in an example in Fig. 2. In Fig. 2, reference numeral 35 denotes a substrate and A, B, C, and D indicate component elements, respectively. The layer consisting of the compound AB and the layer consisting of the compound CD are alternately formed on the substrate 35. For example, the compound AB may be CdTe and the compound CD may be InSb. It is required that the heterojunction interface between the layer of the compound AB and the layer of the compound CD be formed in a stepwise manner. In the case of forming such a device, the elements (Cd and Te) which are necessary for the growth of the nth layer (e.g., CdTe layer) must not remain in the growth chamber when the (n+1)th layer (e.g., InSb layer) grows. For this purpose, the UHV needs to also be maintained during the crystal growth or the partial pressure of the component molecules of gases of the nth layer needs to rapidly decrease when the (n+1)th layer grows. However, the conventional MBE apparatus has the drawback that it cannot satisfy the foregoing requirements since the degree of vacuum deteriorates during the crystal growth. In addition, when the epitaxial layer grows on an atomic layer unit basis, it is undesirable that the growth rate varies with an elapse of time. However, the conventional MBE apparatus has another disadvantage such that the intensity of the molecular beam is temporarily increased when the shutter is made operative (ON). In the following description, the term "molecules" is used as a general term including atoms, ions, and radicals as well as molecules. According to one aspect of the present invention a particle beam deposition apparatus comprises: a growth chamber having an evacuation port through which the chamber may be evacuated; and a particle beam source for directing a particle beam onto a substrate characterised in that the inner wall of the growth chamber is of such shape that particles reflected or re-emitted by the wall are generally directed towards the evacuation port. Parts of the molecular beam or beams reflected or reevaporated from the substrate and the substrate holder are further reflected or reevaporated by the inner wall, so that a plurality of additional (i.e., secondary, ternary, ...) molecular beams are generated. These additional molecular beams are also directed into the sink opening. According to another aspect of an embodiment of the invention, an auxiliary exhaust apparatus may be provided to ensure that the molecular beam portions which are unnecessary for the crystal growth, but which remain due to various attached apparatuses such as a substrate holding mechanism, apparatus for RHEED (reflection high energy electron diffraction), quadruple-mass spectrometer, and the like which are disposed in the growth chamber, and directed into the sink opening. This may comprise means for blowing a molecular flow having a relatively large ratio of specific heat toward the sink opening. Further, when the shutters arranged in the growth chamber or molecular beam source chamber are in the inoperative (OFF) mode, the surface vectors of the reflecting surfaces of the shutters direct the molecular beam to the sink opening. In an embodiment, which will be explained hereinafter, the inner wall of the growth chamber is formed as a paraboloid of revolution. However, the invention can also be applied to the case where the growth chamber is formed in a conical shape. The molecular beam which is led into the growth chamber and irradiated onto the substrate contributes to the crystal growth. However, parts of the molecular beams are reflected or reevaporated by the substrate and the substrate holder, so that a secondary molecular flow is produced. Although almost all of the secondary molecular flow moves toward the sink opening, a part of the secondary molecular flow irradiates the inner wall. A part of the molecular flow reflected by the inner wall is further reflected once or a plurality of times and then moves toward the sink opening, while the other part is adsorbed by the inner wall. When the inner wall is cold, the reevaporation of the adsorbed molecules is suppressed. In addition, an exhausting action is attained by the molecular flow which is reflected by the shutter in the OFF state and which moves toward the sink opening. Conversely, the intensity of the molecular flow is maintained constant when the shutter is in the ON state. The sink opening is equipped with a vacuum pump such that reverse flow and reverse diffusion of the molecular flow to be exhausted do not occur. Molecular flow which is unnecessary for the crystal growth is discharged by the vacuum pump. This molecular flow also gives a kinetic energy to the residual molecules in the growth chamber (namely, the outgases from the inner wall and the like of the growth chamber and the gaseous molecules which were purposely led into the chamber for the preceding growth) so that they are directed toward the sink opening. Thus, by executing the exhausting action for the residual molecules, the crystal component molecules locally increase in the molecular flow during the crystal growth, but the partial pressure of the background other than the molecular flow decreases. According to a further aspect the present invention provides a particle beam deposition apparatus characterised by the combination of: a growth chamber; a holder for a substrate which is arranged in the growth chamber; a particle beam source means located outside the growth chamber, the particle beam source means including: a particle beam source; a beam source chamber for housing the particle beam source the beam source chamber being attached to the growth chamber, the walls of the growth chamber and the beam source chamber having aligned holes therein for leading the particle beam into said growth chamber the beam source chamber including an evacuation port for evacuation of the beam source chamber and a cooled inner wall shaped so that particles reflected or re-emitted by it are generally directed towards the evacuation port, and shutter means for selectively interrupting the particle beam and directing it toward the evacuation port. The invention therefore decreases the deterioration in the degree of vacuum when the crystal grows and also reduces the variation in the intensity of the molecular beam with an elapse of time when the shutter is made operative. The invention will be further described by way of non-limitative example with reference to the accompanying drawings, in which: Fig. 1 is a schematic diagram for explaining a conventional molecular beam epitaxial apparatus; Fig. 2 is a cross-sectional view of an example of a compound semiconductor which can be advantageously formed using the present invention; Fig. 3 is a cross-sectional view of an embodiment of the present invention; Fig. 4 is a schematic diagram for explaining the reevaporation of the adsorbed molecules; Fig. 5 is a cross-sectional view of another embodiment of the invention; Fig. 6 is a cross-sectional view of still another embodiment of the invention; Fig. 7 is a horizontal cross-sectional view showing the arrangement of molecular beam sources in a modification of the Figure 6 embodiment of the invention; and Figs. 8 and 9 are a vertical cross-sectional view and a horizontal cross-sectional view, respectively, of yet another embodiment of the invention. In Fig. 3, reference numeral 1 denotes a growth chamber as a whole. The growth chamber 1 includes a hollow casing 2 having an inner wall shaped as a paraboloid of revolution. A shroud 3, similarly having an inner wall shaped as a paraboloid of revolution, is mounted coaxially with and next to the inner surface of the casing 2. The shroud 3 is formed with a lead-in port 3A of liquid nitrogen as a refrigerant and an exhaust port 3B for the gasified refrigerant. The bottom portion of the growth chamber 1, namely, the plane perpendicular to the axis of the paraboloid of revolution is used as a sink opening 4 (indicated by a virtual line in the diagram). An intake port of a vacuum pump, for example, turbo molecular pump 20 is coupled with the sink opening 4. The pump 20 comprises: a rotary wing portion 22 in which a plurality of wings are attached at regular intervals on the outer peripheral surface of a cylindrical, rotary collar wheel 21; and fixed wings 24 attached on the inner peripheral surface of a cylindrical casing 23 at regular intervals in a manner such that the fixed wings 24 and the wings of the rotary wing portion 22 are alternately positioned. The intake port over the arrangement of the rotary wing portion 22 and fixed wings 24 is coupled with the sink opening 4 of the growth chamber 1. When the rotary wing portion 22 of the pump 20 is rotated at a high speed by a motor 25, a suction is created in the direction from the intake port (sink opening 4 of the growth chamber 1) to an exhaust outlet 26. This produces an exhausting action in the direction from the top of the chamber to the sink opening 4 in the bottom, as indicated by an arrow A in the diagram. Although not shown, an auxiliary pump such as an oil rotating pump or the like is provided for the exhaust outlet 26. A conical deflecting device 27 is arranged on the edge surface of the rotary collar wheel 21 of the pump 20. Although not shown, the surface of the deflecting device 27 is cooled by circulating a refrigerant such as liquid nitrogen or the like in the deflecting device 27. In the case of the turbo molecular pump, there exist portions having surface vectors having a polarity opposite to the exhausting direction. Therefore, the deflecting device 27 is provided to reduce the adverse influence of these portions. Namely, a reverse flow by the reflection of inflowing molecules at the edge surface of the rotary collar wheel 21 of the pump 20 is prevented by the deflecting device 27. Since the surface of the deflecting device 27 is cooled, the reevaporation of that portion of the molecules which were adsorbed is suppressed, so that the final degree of vacuum in the growth chamber 1 can be significantly raised compared to prior art such devices. A substrate holder 5 is supported by a manipulator 7 at a location near the focal point of the growth chamber 1 of the paraboloid of revolution. The substrate holder 5 has a heater. A substrate 6 put on the substrate holder 5 is heated to a predetermined temperature. The molecular beam flows are emitted from a plurality of molecular beam sources 8 as narrow beams whose widths don't extend beyond the outside edges of the substrate holder 5. The molecular beam flows are irradiated onto the substrate 6. The substrate holder 5 is supported at an angle such that the reflecting direction of the incident molecular flow is directed to the sink opening 4. A flared reflecting plate 9 is arranged around the substrate holder 5 to allow the molecular flows which are reevaporated from the substrate 6 and substrate holder 5 to be directed toward the sink opening 4. A thin hole can be formed in the side surface of the reflecting plate 9 to allow an electron beam for the reflected electron beam diffrac­ tion (RHEED) to pass through this hole. For the molecular beam sources 8, it is possible to use a source having a construction such that the molecular flows from a Knudsen cell or Langmuir cell, which use solid elements, are converged so as to be irradiated only onto the substrate 6. The number and kinds of molecular beam sources 8 can be arbitrarily set in accordance with the kinds of crystals to be grown. In the case of using a plurality of molecular beam sources 8, it is necessary to attach shutters to control the molecular beam sources so as to irradiate desired kinds of molecular beams onto the surface of the substrate 6 for a desired period of time. Gaseous elements may be also used as the molecular beam sources 8. Parts of the molecular beams reflected or reevaporated from the substrate are further reflected or reevaporated by the inner wall, so that a plurality of additional (secondary, ternary, ...) molecular beams are generated. These additional molecular beams are also directed into the sink opening. In the foregoing embodiment, in addition to the molecules which are purposefully emitted into the growth chamber 1 for the growth of the crystal, there is an unnecessary secondary molecular flow which is generated by reflection and reevaporation. However, the moving direction of the whole secondary molecular flow is directed to the sink opening 4 because of the paraboloid shape of the inner wall of the growth chamber 1. Namely, by setting the substrate 6 sample at the focal point of the paraboloid of revolution, the molecular flow can be moved toward the sink opening 4 by a single mirror reflection as indicated by an arrow B in Fig. 3 except the random reflection which is reflected in accordance with the cosine law. Therefore, in the growth chamber 1, the exhausting action is mainly performed in the direction from the chamber top to the exhaust port 4 in the bottom portion. Thus, a kinetic energy in the same direction as the exhausting direction is applied to the secondary molecular component. The residual gaseous molecules in the growth chamber 1 are effectively discharged by the secondary molecular flow in accordance with the principle of a vapor jet pump. To the extent that the secondary molecular flow is adsorbed by the inner wall, reevaporation must be suppressed by the cooled shroud 3, so that the components of the molecular flow in the direction opposite to the sink opening 4 are reduced and the final degree of vacuum can be further raised. Namely, as shown in Fig. 4, upon reevaporation, molecules, which are proportional in number to the lengths of the vectors indicated by arrows in the diagram, are emitted from the evaporating surface P in various directions in accordance with the law of cosines. Since the reevaporated components include the components which don't move toward the sink opening, it is highly desirable to suppress the reevaporation by cooling the inner surface 3. Fig. 5 shows another embodiment of the invention. In this embodiment, the growth chamber 1 and turbo molecular pump 20 are provided as in the foregoing embodiment. Those parts whose shapes differ from the shape of the inner wall of the growth chamber 1, can cause high molecular concentrations to be produced where the surface vectors are not directed to the sink opening 4 (namely, the parts whose shapes are not ideal such as the inner wall; for example, the attaching/­ detaching mechanism of the substrate 6, the apparatus necessary to evaluate the crystal, and the like). In Fig. 5, a recess portion C is an example of the space within the chamber in which to locate some of the above-mentioned apparatuses. To prevent the occurrence of high molecular concentrations, a Laval nozzle exhaust mechanism 10 is mounted in the chamber wall above the recess C and is directed toward the sink opening 4 of the growth chamber 1 in order to spout out vapors having a large specific heat ratio, for example, mercury vapors at a sonic speed. However, when the speed of the wings of the turbo molecular pump is subsonic, the vapor speed needs to be reduced to a speed corresponding to the speed of the wings in order to prevent reverse diffusion. A kinetic energy in the same direction as the exhausting direction is applied to the residual molecules in the growth chamber 1 by the vapors blown into the growth chamber 1, so that the remaining molecules in the growth chamber 1 are discharged. This raises the final degree of vacuum in the chamber. In operation, when the chamber is used for epitaxial growth, the gases in the growth chamber 1 are discharged to create a vacuum, the refrigerant is filled in the shroud 3, and the substrate 6 is heated to a specified temperature by means of a heater (not shown) in the substrate holder 5. Thereafter, the molecular beams are emitted from the molecular beam sources 8 and irradiated onto the surface of the substrate 6, thereby allowing the crystals to grow. In this case, the kinds of molecular beams and the irradiating time periods are selectively controlled, thereby allowing the epitaxial layers of compounds to grow. Fig. 6 shows still another embodiment of the invention, in which a beam source chamber 11 is provided independently of the growth chamber 1. The molecular flows from a plurality of molecular beam sources 8′ are converged. The outgases from the crucible, heater, and heat shielding plate which constitute the molecular beam sources 8′ and from their supporting members, and the unnecessary molecular flow are not led into the growth chamber. As shown in Fig. 6, the beam source chamber 11 is arranged so as to be tangent to the growth chamber 1 by rotating another similar vacuum chamber by the angle of 180°. The beam source chamber 11 also has an inner wall shaped as a paraboloid of revolution similar to that of the growth chamber 1. A turbo molecular pump 28 is provided in a sink opening 12 (indicated by a virtual line in Fig. 6) of the opening plane of the bottom portion. The pump 28 has the same construction as the pump 20 provided in the sink opening 4 of the growth chamber 1. Therefore, in the beam source chamber 11, the exhausting action is attained in the direction indicated by the arrow from the chamber top to the sink opening 12. Similar to the above embodiment, a Laval nozzle exhaust mechanism may be also provided for the beam source chamber 11. The molecular beam sources 8′ arranged on the side of the beam source chamber 11 may be an ordinary Knudsen cell, Langmuir cell, or gas exhaust nozzle, or such a nozzle equipped with a cracking furnace. The molecular beam flows emitted from the molecular beam sources 8′ are led into the growth chamber 1 through a plurality of holes 13 formed at the contact position between the growth chamber 1 and the beam source chamber 11 and are irradiated only onto the substrate 6. The unnecessary molecules of the molecular flows from the molecular beam sources 8′ which don't pass through the holes 13 are reflected by the inner wall of a shroud 14 of the beam source chamber 11 or adsorbed to the inner wall of the shroud 14. The reflected or reevaporated molecules become a secondary molecular flow to which a kinetic energy is applied in the exhausting direction toward the sink opening 12. Therefore, the residual gaseous molecules in the chamber 11 are discharged by the secondary molecular flow in a manner similar to a vapor jet pump so that the beam source chamber 11 is held to an excellent vacuum state. As in the case of individually providing shutters for a plurality of molecular beam sources 8′, as shown in Fig. 6, shutters 17 can be provided. The on-off operations of these shutters for every molecular beam source can be controlled from the outside through rotary lead-in terminals 16. Each shutter 17 is formed of a tiltable plate made of, for example, molybdenum or the like. The state in which the shutter 17 is ON (namely, in the operative state) is shown in the diagram. In this operative state, the molecular flow is irradiated onto the substrate 6 in the growth chamber 1 through the holes 13. The shutter position shown in virtual line in Fig. 6 indicates the OFF state (i.e., inoperative state) of the shutters 17. In this inoperative state, the shutters 17 are attached at angles so as to deflect the reflected molecular flows toward the sink opening 12. Since adsorbed molecules are reevaporated in various directions on the basis of the law of cosines, the shutters 17 may be also cooled to prevent molecules from being adsorbed when the shutter is in the OFF state. The molecular flow reflected by the shutter 17 in the OFF state contributes to discharge the residual molecules in the beam source chamber 11. For the embodiments shown in Figs. 3 and 5, respectively, where a plurality of, for example, two molecular beam sources 8₁ and 8₂ are used in the growth chamber 1, they may be arranged as shown in Fig. 7. In the embodiment shown in Fig. 6, the holes 13 are formed at the positions to align with the molecular beam sources 8₁ and 8₂ as shown in Fig. 7. In such a multibeam source embodiment, the contact area between the growth chamber 1 and the beam source chamber 11 must be larger than for a single beams source embodiment. Fig. 8 illustrates still another embodiment as an application of the invention in the case where a number of molecular beam sources are used. The growth chamber 1 is comprised of the casing 2 and the shroud 3, both of which have shapes which are paraboloids of revolution. In the example shown in Fig. 8, the substrate holder 5 is arranged in a plane which is parallel with the plane containing the sink opening 4. The molecular flows are irradiated onto the substrate 6 put on the substrate holder 5 from the molecular beam sources 8₁ and 8₂ arranged at substantially the same height positions as the sink opening 4, respectively. Since the substrate holder 5 is arranged in parallel with the sink opening 4, as shown in Fig. 9, to ensure that the molecular beam sources 8₁ and 8₂ are not polluted it is necessary that no other molecular beam sources be located in regions 18₁ and 18₂ into which the reflected molecular flows enter from the molecular beam sources 8₁ and 8₂, respectively. In addition to the turbo molecular pump, it is also possible to use other vacuum pumps such as a diffusion pump, cryopump, or the like which can prevent the reevaporation of the molecular flow and reverse diffusion by reflection. A sample preparation room and sample evaluation room which are separated by an air-lock mechanism can also be connected to the growth chamber 1. Further, it is also possible to install a nude ion gauge and a quadruple-mass spectrometer to measure the deposition rate (arrival rate), or a reflection high energy electron beam diffracting apparatus to evaluate the crystal during crystal growth, or the like. According to the invention, the gases are discharged by using the portion of the molecular flow which is not used for the crystal growth. Therefore, the vacuum pump is constructed as a whole apparatus. As compared with a conventional molecular beam epitaxial apparatus, the discharging rate of the growth chamber can be increased and the degree of vacuum during the crystal growth can be greatly raised. In particular, a crystal having an excellent multilayer structure can be allowed to grow.

Claims: 1. A particle beam deposition apparatus comprising: a growth chamber (1) having an evacuation port (4) through which the chamber (1) may be evacuated; and a particle beam source (8) for directing a particle beam onto a substrate (6) characterised in that the inner wall (3) of the growth chamber (1) is of such shape that particles reflected or re-emitted by the wall (3) are generally directed towards the evacuation port (4). 2. A particle beam deposition apparatus according to Claim 1 characterised by means for cooling the inner wall (3) of the growth chamber (1). 3. A particle beam deposition apparatus according to Claim 1 or 2 wherein a holder (5) for the substrate (6) is provided and characterised in that the holder is arranged such that particles which are reflected or reevaporated by it or the substrate (6) mounted thereon are generally directed towards said evacuation port (4). 4. A particle beam deposition apparatus according to any one of the preceding claims characterised in that it further comprises shutter means for interrupting the particle beam and diverting it toward the evacuation port. 5. A particle beam deposition apparatus characterised by the combination of: a growth chamber (1); a holder (5) for a substrate (6) which is arranged in the growth chamber (1); a particle beam source means located outside the growth chamber (1), the particle beam source means including: a particle beam source (8′); a beam source chamber (11) for housing the particle beam source (8′) the beam source chamber (11) being attached to the growth chamber (1), the walls of the growth chamber (1) and the beam source chamber (11) having aligned holes (13) therein for leading the particle beam into said growth chamber (1), the beam source chamber (11) including an evacuation port (12) for evacuation of the beam source chamber (11) and a cooled inner wall (14) shaped so that particles reflected or re-emitted by it are generally directed towards the evacuation port (12), and shutter means (17) for selectively interrupting the particle beam and directing it toward the evacuation port (12). 6. A particle beam deposition apparatus as recited in claim 5 characterised in that the growth chamber (1) includes: an evacuation port (4) through which the growth chamber (1) may be evacuated and a cooled inner wall (3) shaped so that particles reflected or re-emitted by it are generally directed towards the growth chamber evacuation port (4). 7. A particle beam deposition apparatus according to any one of the preceding claims characterised in that the inner wall of the growth chamber (1) or beam source chamber (11) or both are shaped as a paraboloid of revolution. 8. A particle beam deposition apparatus according to claim 7 characterised in that, in use, the substrate (6) is positioned in the growth chamber at the focal point of said paraboloid of revolution. 9. A particle beam deposition apparatus as recited in claim 4 or 5 wherein the shutter means is cooled. 10. A particle beam deposition apparatus according to any one of the preceding claims characterised in that it further comprises means (10) for directing a particle flow having a relatively large ratio of specific heat toward the evacuation port (4) of the growth chamber (1) or beam source chamber (11) or both. 11. A particle beam deposition apparatus according to any one of the preceding claims further comprising turbo molecular pump means (20, 28), including an exhaust outlet (26) and an inlet coupled to either or both of said evacuation ports. 12. A particle beam deposition apparatus according to claim 11 characterised in that the molecular pump means (28, 20) comprises: a conical deflecting device (27) arranged on the edge surface of a rotary collar wheel (21) having an outer peripheral surface, a plurality of rotary wings (22) which are attached at regular intervals on the outer peripheral surface of the collar wheel (21), a cylindrical casing (23) having an inner peripheral surface which surrounds the rotary wings (22), fixed wings (24) which are attached on the inner peripheral surface of the casing (23) at regular intervals in a manner such that the fixed wings (24) and the rotary wings (22) are alternately positioned, and means (25) for imparting rotation to the collar wheel (21) relative to the casing (23). 13. A particle beam deposition apparatus according to any one of the preceding claims characterised in that the substrate (6) is held with its deposition surface parallel to the growth chamber evacuation port (4). 14. A particle beam deposition apparatus according to any one of the preceding claims characterised in that there are a plurality of particle beam sources (8₁, 8₂) positioned to introduce the particle beams into the growth chamber (1) at the intersection of the growth chamber evacuation port (4) and the growth chamber inner wall (3). 15. A particle beam deposition apparatus according to any one of the preceding claims characterised in that the inner wall (3,14) is shaped as a truncated cone. 16. A chamber for use in a particle beam deposition apparatus, comprising a chamber wall (1, 11) and an evacuation port (4, 12) in said chamber wall characterised in that the inner surface (3, 14) of the chamber wall is so shaped that particles reflected or re-emitted from it are generally directed toward the evacuation port (4, 12). 17. A chamber according to claim 16 characterised in that the inner surface (3, 14) of the chamber is cooled. 18. A chamber according to claim 16 or 17 characterised in that the inner surface of the chamber is shaped as a paraboloid of revolution or a truncated cane.

Inventors: KIMATA, MORIHIKO
Applicants: KIMATA, MORIHIKO, SHIMADZU CORPORATION
Application year: 1986
Main classification: C30B23
IPC codes: C30B23, H01L21