EP0707663A1 - Dispositif de pulverisation - Google Patents

Dispositif de pulverisation

Info

Publication number
EP0707663A1
EP0707663A1 EP94921324A EP94921324A EP0707663A1 EP 0707663 A1 EP0707663 A1 EP 0707663A1 EP 94921324 A EP94921324 A EP 94921324A EP 94921324 A EP94921324 A EP 94921324A EP 0707663 A1 EP0707663 A1 EP 0707663A1
Authority
EP
European Patent Office
Prior art keywords
magnetron
sputter
plasma
drum
group
Prior art date
Legal status (The legal status is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the status listed.)
Withdrawn
Application number
EP94921324A
Other languages
German (de)
English (en)
Other versions
EP0707663A4 (fr
Inventor
Leroy Albert Bartolomei
Thomas Read
Current Assignee (The listed assignees may be inaccurate. Google has not performed a legal analysis and makes no representation or warranty as to the accuracy of the list.)
Deposition Sciences Inc
Original Assignee
Deposition Sciences Inc
Priority date (The priority date is an assumption and is not a legal conclusion. Google has not performed a legal analysis and makes no representation as to the accuracy of the date listed.)
Filing date
Publication date
Application filed by Deposition Sciences Inc filed Critical Deposition Sciences Inc
Publication of EP0707663A1 publication Critical patent/EP0707663A1/fr
Publication of EP0707663A4 publication Critical patent/EP0707663A4/fr
Withdrawn legal-status Critical Current

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Classifications

    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32—Gas-filled discharge tubes
    • H01J37/32431—Constructional details of the reactor
    • H01J37/32798—Further details of plasma apparatus not provided for in groups H01J37/3244 - H01J37/32788; special provisions for cleaning or maintenance of the apparatus
    • H01J37/32853—Hygiene
    • H01J37/32862—In situ cleaning of vessels and/or internal parts
    • C—CHEMISTRY; METALLURGY
    • C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/0021—Reactive sputtering or evaporation
    • C23C14/0036—Reactive sputtering
    • C23C14/0047—Activation or excitation of reactive gases outside the coating chamber
    • C—CHEMISTRY; METALLURGY
    • C23—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; CHEMICAL SURFACE TREATMENT; DIFFUSION TREATMENT OF METALLIC MATERIAL; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL; INHIBITING CORROSION OF METALLIC MATERIAL OR INCRUSTATION IN GENERAL
    • C23C—COATING METALLIC MATERIAL; COATING MATERIAL WITH METALLIC MATERIAL; SURFACE TREATMENT OF METALLIC MATERIAL BY DIFFUSION INTO THE SURFACE, BY CHEMICAL CONVERSION OR SUBSTITUTION; COATING BY VACUUM EVAPORATION, BY SPUTTERING, BY ION IMPLANTATION OR BY CHEMICAL VAPOUR DEPOSITION, IN GENERAL
    • C23C14/00—Coating by vacuum evaporation, by sputtering or by ion implantation of the coating forming material
    • C23C14/0021—Reactive sputtering or evaporation
    • C23C14/0036—Reactive sputtering
    • C23C14/0073—Reactive sputtering by exposing the substrates to reactive gases intermittently
    • C23C14/0078—Reactive sputtering by exposing the substrates to reactive gases intermittently by moving the substrates between spatially separate sputtering and reaction stations
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32—Gas-filled discharge tubes
    • H01J37/32009—Arrangements for generation of plasma specially adapted for examination or treatment of objects, e.g. plasma sources
    • H01J37/32192—Microwave generated discharge
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32—Gas-filled discharge tubes
    • H01J37/32009—Arrangements for generation of plasma specially adapted for examination or treatment of objects, e.g. plasma sources
    • H01J37/32321—Discharge generated by other radiation
    • H01J37/3233—Discharge generated by other radiation using charged particles
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32—Gas-filled discharge tubes
    • H01J37/32431—Constructional details of the reactor
    • H01J37/3266—Magnetic control means
    • H01J37/32678—Electron cyclotron resonance
    • H—ELECTRICITY
    • H01—ELECTRIC ELEMENTS
    • H01J—ELECTRIC DISCHARGE TUBES OR DISCHARGE LAMPS
    • H01J37/00—Discharge tubes with provision for introducing objects or material to be exposed to the discharge, e.g. for the purpose of examination or processing thereof
    • H01J37/32—Gas-filled discharge tubes
    • H01J37/34—Gas-filled discharge tubes operating with cathodic sputtering
    • H01J37/3402—Gas-filled discharge tubes operating with cathodic sputtering using supplementary magnetic fields
    • H01J37/3405—Magnetron sputtering

Definitions

  • the present invention deals with a device and process for enhancing the plasma at a sputter target and the use of this enhanced plasma to react a selected material deposited on a substrate.
  • Hartsough claims a technique in which the substrate on which the metallic compound is to be deposited is alternately passed over the sputter target and through a reactive atmosphere. In this manner deposition of the metal atoms is at least partially separated in time and space from the compounding of the film. The degree of separation depends on the degree of atmospheric isolation between the sputtering and compounding zones. Hartsough also teaches the use of a plasma in the compounding zone for speeding the rate of reaction. Thus, for example, deposition of an oxide film is enhanced if oxygen in the compounding (oxidizing) zone is activated by a plasma, since excited oxygen species react much more readily with the metallic film than do ground state 0 2 molecules.
  • Scobey et al. in U.S. Patent No. 4,851,095 claim a specific embodiment of the general device claimed by Hartsough. While Hartsough claims broadly the separation of the deposition and reaction zones, with no specification or restriction as to the degree of separation, and teaches the advantage of using an activating plasma in the reaction zone, Scobey et al. claim a localized plasma as the reaction zone, and emphasize the need for this plasma to be physically and atmospherically separated from the deposition zone. In fact, Scobey et al. differentiate from Hartsough's teaching by emphasizing the physical and atmospheric separation of reaction and deposition zones. There are several shortcomings which are unavoidable consequences of practicing the art as described above.
  • the present invention avoids these shortcomings by bringing the sputter and activation zones atmospherically and physically together while eliminating any baffles or differential pumping, thereby effectively blending the plasmas of these two zones into a single, continuous plasma which serves to both sputter material from the target and react it at the substrate.
  • the present invention is a device and process for enhancing and spatially broadening the plasma at a sputter target and the use of this enhanced, broadened plasma to sputter a selected material onto a substrate and to react the material deposited on the substrate.
  • the device can be incorporated into various vacuum chamber configurations, such as those suggested by U.S. Patent No. 4,851,095, it is readily incorporated into a system comprising a vacuum chamber and a drum rotatably mounted within the chamber, the drum supporting a substrate which is moved past the device located on the circumference of the chamber.
  • the invention comprises a magnetron sputter device capable of depositing the selected material onto the substrate and a plasma generating device positioned immediately adjacent to the magnetron device. Both the plasma generating device and the magnetron are capable of creating a plasma, but in practice the plasmas generated by these two components interdiffuse to become one continuous, activating and sputtering plasma.
  • Fig. 1 is a simplified schematic cross sectional view-of a drum vacuum coater incorporating the present invention.
  • Fig. 2 is a simplified cross sectional view of a conventional, balanced magnetron sputter device showing the balancing of center and edge magnets.
  • Fig. 3 is a simplified cross sectional view of an unbalanced magnetron sputter device showing the lack of balance between the edge magnets and center magnet and the resulting diverging magnetic field above the target.
  • Fig. 4 is a conceptual drawing of the enhanced broadened plasma generated by the present invention, showing the current paths through the plasma and associated generating system.
  • Fig. 5 is a graph showing a current-voltage characteristic of a magnetron sputter device without an adjacent auxiliary plasma and a current voltage characteristic of a magnetron sputter device operating in one embodiment of the invention.
  • Fig. 6 is a simplified schematic view of a preferred embodiment of the invention, showing details of the microwave injection system and electron cyclotron resonance field coils.
  • Fig. 7 is a simplified cross sectional view of another embodiment of the present invention, showing a microwave form designed to broaden the auxiliary plasma to better match a linear target plasma.
  • Fig. 8 is a table showing the relation between sputtering yield and voltage for a silicon target.
  • Fig. 9 is a simplified cross sectional view showing a magnetron sputter device and an adjacent. coupled plasma generating device positioned inside a substrate supporting drum.
  • Fig. 10 is a simplified cross sectional view showing magnetron sputter devices and associated adjacent, coupled plasma generating devices inside and outside a substrate supporting drum.
  • Fig. 11 is a simplified cross sectional view of a vacuum chamber with cylindrical inner and outer walls both of which house magnetron sputter devices and associated, coupled auxiliary plasma devices for coating from both sides of a rotating substrate bearing drum.
  • the process of the present invention is carried out in a vacuum chamber, housing a rotary drum much like the device disclosed in Scobey et al. U.S.Patent 4,851,095, the disclosure of which is hereby incorporated by reference.
  • the Scobey et al.-like vacuum drum is modified pursuant to Fig. 1.
  • sputtering system 10 comprises housing 1 whose circumference defines a vacuum or low pressure environment.
  • housing 1 can be connected to a suitable vacuum pumping system (not shown) .
  • the pressure within housing 1 is generally in the range of 10 "4 to 10 "2 Torr.
  • Magnetron sputtering device 5 is positioned on the circumference of vacuum housing of chamber 1 located in close proximity to plasma generating device 6.
  • an inert sputtering gas such as argon
  • a compounding gas such as oxygen
  • a metal film sputtered from target 5 is deposited. Reaction of this film with the compounding gas begins immediately as the film is deposited in region 9 under the target 5. As the substrate is carried into region 8 of the plasma, under the plasma generating device 6, this reaction continues, completing conversion of the film to a dielectric with the desired stoichiometry.
  • a distinguishing characteristic in practicing the present invention is that more than 50% of the conversion of target material to the different chemical species (dielectric) occurs in the region where the metal film is sputtered from target 5. This is in sharp contrast to Scobey et al where formation of the dielectric occurs virtually entirely in a zone isolated from the magnetron/target assembly.
  • Fig. 1 the sequence described above and shown in Fig. 1 can be repeated through rotation of the drum to build a dielectric film of a desired thickness.
  • multilayer films of various materials can be applied to substrates 3.
  • the present invention differs significantly from prior devices of this type in that plasma 11 is spatially continuous over target 5 and plasma generation device 6 and compounding of the film is accomplished continuously in plasma 11. Yet another distinguishing feature of the invention is that the plasmas over target 5 and device 6 form a single continuum 11 in which the free electron density of plasma 11 is at least 10 8 /cm 3 throughout the continuum. In fact, plasma 11 electrically couples the target and plasma generation device. Again, this is in marked contrast to Scobey et al. which specifically teaches the physical and atmospheric separation of the sputtering target and reaction zones.
  • plasma generating device 6 is a microwave device operating at 2.54 gigahertz.
  • the plasma 11 is then created by the microwaves and the sputter target operating in concert. If the free electron density of the plasma in region 8 is higher than the critical density for microwaves of 2.54 gigahertz, the frequency ordinarily used, then the plasma is substantially opaque to the microwaves and interdiffusion of the plasma in region 8 with the plasma in region 9 renders the plasma continuous. If the plasma is sufficiently transparent to the microwaves, either through an electron density below the critical density or through operating the microwave in a circularly polarized mode so that the so called whistler mode is operative, then the plasma 11 is rendered continuous through both interdiffusion and absorption of microwaves throughout the plasma.
  • the magnetic field lines 18 are substantially confined to the region just above the target 19. This is accomplished by making the center magnet 20 twice the width of the outside magnet 21, so that all flux from the outside magnets flows through the center magnet.
  • the so-called "unbalanced magnetron” the center magnet 24 is made smaller or replaced by a magnetically permeable material, so that a part of the flux 22 is "pushed" away from the target 23.
  • This fringing magnetic field carries part of the plasma away from the target and toward substrate 3 (Fig. 1) and contiguous plasma generating device 6 (Fig. 1) .
  • operation in this unbalanced mode can have other beneficial effects, as discussed below.
  • plasma 11 of Fig. 1 is shown in detail in Fig. 4 as plasma 16.
  • the current in plasma 16 is complex, consisting of both ion and electron components.
  • the external current through ground 17 to the power supply 15 and through the power supply to sputter target 13, is all electronic.
  • the plasma 16 there is a net electron current flow equal to that which passes through the power supply 15.
  • the plasma thus acts as a resistive current-carrying element.
  • the electron current can go to ground from the plasma at any number of points 12, depending on machine configuration, tooling and other considerations. But in any instance, an electron current is pulled from the plasma as voltage is applied to the target 13.
  • the plasma-ground-power supply-target circuit will exhibit a particular voltage at which the target strikes a plasma. Below this voltage, there will be no current. But as soon as the plasma is struck, the power supply begins to pull current from the plasma, the current increasing with increasing target voltage.
  • a typical current(I) -voltage(V) curve for a 5" x 15" silicon target is shown as curve A of Fig. 5 where the microwave device does not contribute to plasma generation. That is, the microwave is not used in generating Curve A.
  • the curve shows that below a particular voltage (410 volts in this case) at which the target struck a plasma, there was no current, but as the plasma was struck, the power supply began to pull current from the plasma.
  • curve B of Fig. 5 was based upon data generated by initially setting the sputter target voltage to 0 while striking a plasma using only the microwave device. Visually, it was observed that this plasma extended to envelop the sputter target.
  • voltage to the sputter target power supply was increased from 0, the power supply began immediately to pull current from the microwave generated plasma. As the voltage was increased further still, so that positive ions accelerated to the target caused secondary electron emission from the target surface, the sputter power supply began to contribute to the plasma.
  • I was increased under these conditions, curve B was generated.
  • the sputter magnetron and microwave device operate as an integral unit in the generation of a plasma and that changing one influences the operation of the other. This is made clearer still by noting, for example, that as the microwave power increases, the voltage required to maintain a given current through the magnetron sputter supply decreases. This is explained by noting that the increased microwave power lowers the resistance of the plasma.
  • the device and process of the present invention are capable of achieving higher sputter rates when compared to prior devices.
  • Higher sputter rates follow from the ability of the sputter cathode to draw current from the microwave-induced part of the plasma. This increase in rate is obvious at voltages less than the sputter target striking voltage without the microwave plasma.
  • the sputter rate is zero without a plasma being created by the microwave device (Curve A) .
  • the sputter rate is zero without a plasma being created by the microwave device (Curve A) .
  • 370 volts there is a significant sputter rate when operating pursuant to the present invention.
  • This ability of the present invention to draw ion current from the plasma at low voltages allows sputtering at voltages lower than those of corresponding prior art devices. Since the energy distribution of sputtered atoms shifts toward higher values with increased sputter ion energy, this ability is particularly advantageous in reducing the number of atoms sputtered with higher energies to minimize damage to the growing film. It was also observed that the sputter rate is increased at voltages higher than the striking voltage. This can be appreciated by considering the yield curve for the sputtered material and the dependence of sputter rate on yield and current; "yield” simply meaning the number of target atoms sputtered for each ion striking the target.
  • I is the target ion current in amperes
  • Y is the yield in number of atoms sputtered for each ion incident on the target.
  • the yield Y is a function of the target voltage V. This function can be measured and is indicated in Fig. 8 for silicon sputtered in argon. Examination shows that the function is well approximated by
  • the maximum sputter rate is limited by the power that can be applied to the target without damage by debonding from the backplate or warping through over heating.
  • the power is increased to the maximum possible.
  • R' and I' are the rate and current without the microwave device contributing to plasma generation, then from equation (3)
  • the rate of oxide deposition can be much higher than has been therefore achieved.
  • use of the present device has resulted in deposited clear Si0 2 at over-the-target rates exceeding 180 A/sec, nearly double those reported in U.S. Patent No. 4,420,385. This is also true for other materials as well, as the following discussion reveals.
  • the present invention increases the oxygen, or other reactive gas, that can be introduced into the vacuum chamber before the target surface becomes completely covered by an oxide layer; that is, before the target is "poisoned.” This results from the ability of the enhanced plasma to create active oxygen species which readily react with the growing film.
  • This film is in effect a second pump for the reactive gas, the vacuum system pump being the first.
  • the pumping speed of the second pump is greater as the oxygen, or other reactive gas, is made more reactive.
  • the device operates with 2 to 3 KW of microwave power distributed over a plasma 8 to 10 inches in length. This is in marked contrast to the few hundred watts over 20-25 inches cited in U.S. Patent No. 4,420,385, for example.
  • This high input power into the broadened enhanced plasma of the present invention is especially effective in exciting the reactive gas and therefore in increasing the pumping speed of the growing film. While it is often desirable to operate the system with the maximum reactive gas possible before target poisoning, it is sometimes not desirable. Because of its effectiveness in generating active species, the enhanced plasma device of the present invention often provides complete oxidizing, or nitriding, etc, at reactive gas flows well below the target poisoning level. This mode of operation is often convenient when very stable operation is desired; that is, when operation away from the poisoning knee of the system curve is desired.
  • the present invention is capable of striking a plasma at much lower pressures than those normally used in magnetron sputtering.
  • a DC magnetron requires pressure higher than 10 "3 Torr
  • the present invention is capable of striking a plasma at pressures well below 10 "4 Torr.
  • the present invention is capable of drawing sputtering current at pressures for which the mean collision path is greater than 50 cm. This can be advantageous when line-of-sight deposition is required; that is, when scattering of the sputtered atoms is detrimental to the growing film. This can, for example, prevent high angles of incidence deposition which can lead to porous or stressed films.
  • Low pressure operation is achieved by using a microwave generator as the plasma enhancing device.
  • the microwaves into the system through 6 reflect from the metal drum 2, causing an intense standing wave in the region above the drum 2, the region in which the plasma is desired.
  • the drum 2 becomes part of a high Q microwave cavity in which intense fields capable of plasma generations at pressures down to approximately 5 x 10 "4 Torr can be struck and maintained.
  • ECR electron cyclotron resonance
  • the magnetic field B for ECR operation can be generated in any number of ways.
  • a current carrying coil can be wrapped around the microwave waveguide as it enters the vacuum chamber.
  • a permanent magnet in the region of the microwave windows on the chamber. When this done, an ECR induced plasma will strike in those regions around the magnet where the magnetic field is 875 gauss.
  • the present invention is also capable of depositing some non-oxide dieletrics more effectively than is possible using prior art.
  • titanium nitride TiN
  • TiN titanium nitride
  • titanium dioxide is a clear coating often used in optical filters. Titanium metal reacts readily with oxygen but is essentially nonreactive with nitrogen. To obtain a good TiN film one thus needs a plasma to excite the nitrogen and render it more reactive, and one needs to exclude oxygen from the deposition system to the maximum degree possible.
  • a titanium target is employed and nitrogen gas bled into the system after an initial pumpdown.
  • the pumpdown removes oxygen from the system, with temperature and vacuum chamber history being important variables in determining the time required. For example, if the chamber has a thick, porous coating on its walls from previous runs, then a long time may be required for water vapor to be desorbed from the walls. As such, there will always be some residual oxygen in the system and this oxygen will compete with nitrogen in reacting with the sputtered Ti film.
  • substrates are placed upon the drum which is, for example, rotated at 30 rpm.
  • the microwave source is positioned on the counterclockwise side of the magnetron sputter target as shown in Fig. 1
  • the Ti metal is sputtered only in the vicinity of the magnetron whereupon the substrates pass directly into the zone dominated by the microwave device.
  • exposure to background oxygen is minimal, since the reaction started at the site of the target is completed at the site of the microwave device and no free Ti is available for reaction after passing through the microwave input zone.
  • the sputter target is configured in the unbalanced mode as briefly described earlier in reference to Fig. 3. It is well known that the quality of a thin film can be influenced through bombardment of the film by energetic atoms during deposition. The energy of these atoms is preferably great enough to move atoms around on the growing film and small enough to avoid significant sputtering of the film. To restate, it is desirable to increase the mobility of the atoms while avoiding their resputtering. This is best accomplished when the energy of the bombarding species is between about ten and one hundred electron volts. The unbalanced magnetron of Fig. 3 provides ions at the substrate in this energy range.
  • the unbalanced magnetron can be used as the sputter target in the present invention with plasma enhancement and broadening being provided by, for example, the microwave system discussed above as part of a preferred embodiment.
  • auxiliary plasma generator in conjunction with a contiguous sputter target which itself may or may not be unbalanced.
  • the unbalanced auxiliary would operate in the poisoned mode to provide an intense plasma while sputtering at a low rate and the sputter target per se would operate in the unpoisoned mode to provide the desired metal atoms at a high rate.
  • This dual operation of two targets, one poisoned and one unpoisoned is easily achieved even though the reactive gas pressure is the same over both by simply running the sputter target at a power high enough to insure that it does not poison while running the auxiliary at a power low enough to insure that it does poison.
  • the auxiliary target was of the same material as the main sputter target, so that any material sputtered from it would simply add to the growing film and not contaminate it. This can sometimes be inconvenient and/or less efficient than desired in enhancing the plasma, the latter when insufficient power is applied without cleaning the auxiliary target of it's poisoned surface layer.
  • a preferred embodiment of the present invention utilizes a microwave generator as the plasma enhancement device 6 of Fig. 1. One embodiment is shown in Fig.
  • a microwave transparent window 30 made of, for example, fused quartz, is mounted on the wall of the chamber.
  • a waveguide 28 directs microwaves " through the window 3 enhancing the plasma 31.
  • the microwave frequency is 2.54 GHz and the waveguide and window are suitably sized for this frequency.
  • the waveguide is WR284, which is rectangular and measures 3 inches x 1.5 inches.
  • the window is circular and approximately 3 inches in diameter.
  • the microwave power supply is capable of generating 3 KW of microwave power. This is tuned to the plasma 30 using a stub tuner 29 in the waveguide 28.
  • the sputter target in one embodiment is 5" x 15" and is positioned on the outside circumference of the vacuum chamber 25 adjacent to the microwave window 30.
  • the separation of the target and window is typically less than about ten inches, allowing the plasma 31 to diffuse readily between the microwave window 30 region and the target region so that the advantages of the invention as discussed previously can be realized.
  • a rainbow-like coating is observed at the microwave window. This is a metal oxide coating formed by metal atoms from the sputter target and oxygen, and it evidences a coupling of the plasmas generated at the target and the microwave generating device as well as a significant excitation of metal and oxygen atoms in the entire region of the continuous plasma..
  • a magnetic field 32 is generated in the plasma 31 by a current carrying coil 33 wrapped around the waveguide 28.
  • the ampere turns in this coil are sufficient to create a field strength of 875 G over some surface in the plasma 31, thereby causing ECR operation at that surface. It has been found that 400 amperes through * 75 turns is sufficient to " accomplish this.
  • the magnetic field 32 can also act as a magnetic mirror to keep the hot plasma 31 away from the window 30, thereby allowing higher power without damaging the window or vacuum seals.
  • the magnetic mirror effect occurs at field levels below those needed for ECR operation and the invention can be so operated if desired.
  • a film deposited on substrates 27 spaced over 8-12 inches can be reacted. This is because reactive species of the plasma 31 readily diffuse to regions, beyond the 3 inch microwave window 30.
  • the number of microwave inputs each the same as shown in Fig. 6, can be used. For example, three such sources readily suffice for use with a 25" target, the three plasma zones diffusing into each other and into the region under the target.
  • the invention can also utilize a microwave horn as shown in Fig. 7.
  • microwaves are injected through a WR284 waveguide 35 into a microwave horn 36.
  • the length of this horn along the drum is approximately 15 inches when used with a 25" target.
  • the microwave window 37 mounted in the chamber wall 38 is rectangular, measuring fifteen inches by 5 inches. In this arrangement a long plasma 39 is created allowing activation of film on substrates 40 and coupled operation with the sputter target (not shown) .
  • Microwave Power 1.5 Kw Drum Rotation Rate 30 rpm Drum 2 was first rotated counterclockwise to produce Sample A and the direction of rotation reversed to a clockwise direction to create Sample B.
  • the resulting films were partially transparent but Sample B more so than Sample A.
  • the conductivity of Sample A was measured at 10 ohms/square while that of Sample B was 25 ohms/square. These measurements clearly indicate that Sample A was better nitrided than Sample B. Stated differently. Sample B was partially oxidized by its longer exposure to the oxygen background.
  • the device as depicted in Fig. 1 was configured with a tantalum metal target and the deposition conditions listed in Table 3 were established. Under these conditions a clear film of Ta 2 0 5 was deposited at an over the target rate of 120 A/sec which was obtained without baking the part after deposition; a process commonly used to complete oxidation of thin films as taught in U.S. Patent No. 4,851,051.
  • deposition rates can be increased if a post deposition bake can be used to complete reaction of the film; that is, to remove residual absorption from the film. This is true for the present invention.
  • a post deposition bake can be used to complete reaction of the film; that is, to remove residual absorption from the film. This is true for the present invention.
  • the device was configured as depicted in Fig. l and the deposition conditions listed in Table 4 were established and a one.micron,film-was-deposited ⁇ at a rate of 210 A/sec.
  • the film was absorbing upon removal from the coating chamber but cleared after baking for 30 minutes at 600° C. This is in contrast to the 150 A/sec achieved in U.S. Patent 4,851,095.
  • the present invention has a wide variety of appli ⁇ cations, including multilayer interference filters, opaque wear resistant coatings, transparent wear re ⁇ sistant coatings-, layered ultrathin coherent, structures (LUCS) , transparent conductive coatings, and others. Some of these applications are briefly described below.
  • the invention was employed to deposit a conductive tin oxide using a tin target and a microwave generated auxiliary plasma. The resulting coating was clear with conductivity 10 *4 ohm-cm.
  • the invention is also suitable for depositing filters on lamps. For example, a filter transmitting in the visible and reflecting in the infrared, out to about 2 microns, has been used as an energy device for incandescent lamps, especially tungsten halogen lamps.
  • the reflected infrared energy maintains the filament temperature at a given level with less electrical input, thereby yielding visible light at lower cost.
  • filters and lamps are well known. They are produced in volume by The General Electric Co. , and are described in U.S. Patent 4,851,095. These IR reflecting filters on lamps can be deposited using the present invention by providing tooling to rotate the lamps as they pass through the sputtering - activating plasma. Nb 2 0 5 /Si0 2 and Ti0 2 /Si0 2 have been used as material pairs to make the filters.
  • MR 16's form an example of the latter. These are half paraboloids measuring 16 eighths of an inch across. They are used, for example, in overhead projectors.
  • the present invention is particularly suitable for coating these MR 16's. It's high deposition rates allow very stable oxides to be deposited economically in this commodity product.
  • Fig. 9 shows an auxiliary plasma generating device 6 coupled to a sputter target 5 on the inside of a rotating, substrate bearing drum 2.
  • Fig. 10 shows coupled auxiliary devices 6 and sputter targets 5 on both the inside and outside of a substrate bearing drum 2.
  • Fig. 11 shows a novel "donut" configuration in which the vacuum chamber 1 has cylindrical inner and outer vacuum walls 1 with coupled auxiliary devices 6 and sputter targets 5 mounted in the walls 1. It is obvious that such a configuration allows coating of substrates facing either in or out on the drum and therefore effectively doubles the load size.

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  • Metallurgy (AREA)
  • Organic Chemistry (AREA)
  • Health & Medical Sciences (AREA)
  • Public Health (AREA)
  • Epidemiology (AREA)
  • Physical Vapour Deposition (AREA)

Abstract

L'invention concerne un système de pulvérisation (10) pour réaliser un revêtement, utilisant une chambre à vide (1). Une surface mobile (2) est prévue dans la chambre et elle est agencée pour recevoir des substrats (3) et assurer leur déplacement. Au moins un dispositif de pulvérisation (5) à magnétron est placé au niveau d'un poste de travail au voisinage du support du substrat et il est agencé pour pulvériser au moins un matériau sélectionné sur le substrat. Au moins un second dispositif (6) est positionné près du premier dispositif pour fournir un plasma (11), afin d'améliorer le plasma formé par le premier dispositif.
EP94921324A 1993-06-17 1994-06-17 Dispositif de pulverisation Withdrawn EP0707663A4 (fr)

Applications Claiming Priority (3)

Application Number Priority Date Filing Date Title
US7876693A 1993-06-17 1993-06-17
US78766 1993-06-17
PCT/US1994/006908 WO1995000677A1 (fr) 1993-06-17 1994-06-17 Dispositif de pulverisation

Publications (2)

Publication Number Publication Date
EP0707663A1 true EP0707663A1 (fr) 1996-04-24
EP0707663A4 EP0707663A4 (fr) 1998-01-14

Family

ID=22146092

Family Applications (1)

Application Number Title Priority Date Filing Date
EP94921324A Withdrawn EP0707663A4 (fr) 1993-06-17 1994-06-17 Dispositif de pulverisation

Country Status (3)

Country Link
EP (1) EP0707663A4 (fr)
JP (1) JPH08511830A (fr)
WO (1) WO1995000677A1 (fr)

Families Citing this family (10)

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US6402902B1 (en) * 1995-02-13 2002-06-11 Deposition Sciences, Inc. Apparatus and method for a reliable return current path for sputtering processes
US5849162A (en) * 1995-04-25 1998-12-15 Deposition Sciences, Inc. Sputtering device and method for reactive for reactive sputtering
DE19644752A1 (de) * 1996-10-28 1998-04-30 Leybold Systems Gmbh Interferenzschichtensystem
EP0947601A1 (fr) * 1998-03-26 1999-10-06 ESSILOR INTERNATIONAL Compagnie Générale d'Optique Substrat organique avec des couches optiques déposé par pulvérisation magnétron et son procédé de fabrication
US6186090B1 (en) * 1999-03-04 2001-02-13 Energy Conversion Devices, Inc. Apparatus for the simultaneous deposition by physical vapor deposition and chemical vapor deposition and method therefor
DE10196278B3 (de) * 2000-05-31 2015-04-09 Isoflux Inc. Nicht balancierte Plasmaerzeugungsvorrichtung mit zylindrischer Symmetrie
DE10031280A1 (de) * 2000-06-27 2002-01-24 Roth & Rauh Oberflaechentechni Multifunktionale Mehrlagenschicht auf transparenten Kunststoffen und Verfahren zur ihrer Herstellung
US6635155B2 (en) 2000-10-20 2003-10-21 Asahi Glass Company, Limited Method for preparing an optical thin film
WO2002084702A2 (fr) * 2001-01-16 2002-10-24 Lampkin Curtis M Appareil de pulverisation cathodique et procede permettant de deposer des films superficiels
CN101796213B (zh) * 2007-08-30 2012-07-11 皇家飞利浦电子股份有限公司 溅射系统

Citations (1)

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EP0516436A2 (fr) * 1991-05-31 1992-12-02 Deposition Sciences, Inc. Dispositif de pulvérisation

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DE3378508D1 (en) * 1982-09-10 1988-12-22 Nippon Telegraph & Telephone Plasma deposition method and apparatus
US4466877A (en) * 1983-10-11 1984-08-21 Shatterproof Glass Corporation Magnetron cathode sputtering apparatus
US4560462A (en) * 1984-06-22 1985-12-24 Westinghouse Electric Corp. Apparatus for coating nuclear fuel pellets with a burnable absorber
EP0173164B1 (fr) * 1984-08-31 1988-11-09 Hitachi, Ltd. Vaporisation à l'aide de micro-ondes
DE3503398A1 (de) * 1985-02-01 1986-08-07 W.C. Heraeus Gmbh, 6450 Hanau Sputteranlage zum reaktiven beschichten eines substrates mit hartstoffen
US4885070A (en) * 1988-02-12 1989-12-05 Leybold Aktiengesellschaft Method and apparatus for the application of materials
US4911814A (en) * 1988-02-08 1990-03-27 Nippon Telegraph And Telephone Corporation Thin film forming apparatus and ion source utilizing sputtering with microwave plasma
US4851095A (en) * 1988-02-08 1989-07-25 Optical Coating Laboratory, Inc. Magnetron sputtering apparatus and process
US4990229A (en) * 1989-06-13 1991-02-05 Plasma & Materials Technologies, Inc. High density plasma deposition and etching apparatus
DE3920835C2 (de) * 1989-06-24 1997-12-18 Leybold Ag Einrichtung zum Beschichten von Substraten

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EP0516436A2 (fr) * 1991-05-31 1992-12-02 Deposition Sciences, Inc. Dispositif de pulvérisation

Non-Patent Citations (2)

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Title
LEHAN J P ET AL: "HIGH-RATE ALUMINUM OXIDE DEPOSITION BY METAMODETM REACTIVE SPUTTERING" JOURNAL OF VACUUM SCIENCE AND TECHNOLOGY: PART A, vol. 10, no. 6, 1 November 1992, pages 3401-3406, XP000322749 *
See also references of WO9500677A1 *

Also Published As

Publication number Publication date
JPH08511830A (ja) 1996-12-10
EP0707663A4 (fr) 1998-01-14
WO1995000677A1 (fr) 1995-01-05

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