ROTATING MAGNETRON SPUTTERING CATHODE APPARATUS AND METHOD OF DEPOSITING MATERIAL WITH THE SAME
This application claims priority to The present invention relates to a rotating magnetron sputtering cathode apparatus utilizing a cylindrical cathode and radio frequency emissions, and a method of depositing material with a rotating cylindrical magnetron sputtering cathode apparatus using radio frequency emissions. Sputtering rotating magnetron cathode apparatuses utilizing cylindrical cathodes are known in the art. However, such apparatuses are adapted for operation with direct current or low- to medium-frequency alternating current, and do not operate using radio frequency ("RF") emissions. As a result, such apparatuses generally require metal doping to deposit non-metallic materials. The present invention overcomes such limitations by providing a cylindrical rotating magnetron sputtering cathode apparatus that incorporates electrical isolation of the cathode and electrode, components formed of non-ferrous materials, liquid cooling, and improved power delivery. Significantly, the apparatus of the present invention is fully capable of RF operation and provides a method of depositing materials, including oxides, with RF emissions that reduces or eliminates the need for metal doping. The distinction between alternating current and RF is understood in the art. While RF current is an alternating current as opposed to a direct current, the energy transmitted by an RF power supply need not be transmitted by direct electrical contact. Instead, RF energy may be transmitted through a medium (such as air or water) to the target material. In this way, an electrode attached to an RF power supply can be seen as acting as an antenna transmitting RF emissions as opposed to acting purely as a conductor of an alternating current. Traditionally, rotating magnetron sputtering cathode apparatuses utilizing a cylindrical cathode, which are adapted for operation with alternating current, have utilized two rotating cathodes and are adapted such that the power signal alternates between them. Such arrangements are not required where RF power is utilized. However, RF power can generate inductive and magnetic effects that previously made it impractical to sputter materials using RF emissions with rotating cylindrical cathodes. The present invention addresses these limitations and allows for RF operation of a rotating magnetron sputtering cathode apparatus utilizing a single cylindrical cathode. Document Document Document Disclosed herein is a rotating magnetron sputtering cathode apparatus according to claim 1. While the cathode could be entirely made up of the material to be deposited (the target material), in other embodiments only a portion of the outer surface of the cathode will comprise the target material, with the remainder of the cathode comprising other materials. The electrode is electrically isolated from the shaft, and is preferably not in direct electrical contact with the cathode, but may be in direct contact in some embodiments. To address issues created by magnetic fields induced by high frequency operation, the electrode and shaft are preferably formed from non-ferrous materials. The shaft is generally coaxial with the cathode and is mechanically connected to the cathode such that rotating the shaft causes the cathode to rotate about the magnetic field source and a portion of the electrode. The connection is such that the shaft and said cathode are also electrically isolated so that electrical energy is not transmitted directly from the cathode to the shaft in substantial quantities. The drive motor is adapted to rotate the shaft and, thereby the cathode, and the power supply is adapted to supply RF energy at frequencies of 1 MHz or higher, with no set upper limit. The electrode is electrically connected to the power supply and transmits the RF emissions generated by the power supply to the cathode during operation. The RF energy causes the cathode to eject particles of the target material as the cathode rotates, preferably onto a substrate positioned near the cathode. Also disclosed is a method of depositing material with a rotating cylindrical magnetron sputtering cathode apparatus, according to claim 12. The apparatus likewise comprises an RF power supply, a power delivery assembly, a rotating cathode, a shaft and a drive motor. The power delivery assembly preferably comprises a magnetic field source positioned within the rotating cylindrical cathode and an electrode extending within the cathode. At least a portion of the outer surface of the cathode comprises a target material, but the entire cathode may be formed of target material as well in certain embodiments. The electrode is electrically isolated from the shaft, which is generally coaxial with the cathode. The electrode and shaft are formed from non-ferrous materials. Utilizing such an apparatus, the method disclosed herein comprises the steps of causing the power supply to supply radio frequency energy at frequencies of 1 MHz or higher to the electrode, causing the cathode to rotate about the magnetic field source, and positioning a substrate proximate to the outside surface of the cathode, which comprises the target material. During operation, RF energy from the RF power supply causes particles of the target material to eject onto the substrate. Other features of the invention will become apparent from the attached drawings, which illustrate certain preferred embodiments of the apparatus of this invention, wherein
While the following describes preferred embodiments of the apparatus and methods of the present invention, it is to be understood that this description is to be considered only as illustrative of the principles of the invention and is not to be limitative thereof. Numerous other variations, all within the scope of the present invention, will readily occur to others, which invention shall be limited only by the claims herein. The term "adapted" shall mean sized, shaped, configured, dimensioned, oriented and arranged as appropriate. The term "radio frequency" or "RF" will denote frequencies of 1 MHz or higher, without upper limit. The term "electrically isolated" shall mean, with respect to two components, that there is no conductive connection between the components that would enable a direct current to flow from one to the other in substantial quantities. The term "doping" shall mean the practice of including a predetermined amount of a material into a target material to change the sputtering characteristics of the target material. Thus, a "doped material" shall refer to a target material in which doping was used. Doping is commonly used to enable sputtering of insulating materials by doping the insulating target material with conductive materials such as metals. Other types of doping, in which materials other than metals, are added to target materials are also possible. The term "non-ferrous" when used to describe a material shall indicate the material is substantially free of iron or is a non-magnetic metal such as aluminum, brass, or 304 stainless steel. Where a number is used immediately preceding "stainless steel" (e.g. "304 stainless steel"), the number refers to a grade of stainless steel and not an element number shown in the figures. Where specific materials such as particular grade of stainless steel are referenced in this detailed description, the reference is intended to disclose one example of an appropriate material which may be used, and is not intended to limit the present invention to components formed of those materials. Where reference is made herein to insulating ceramic bearings, such bearings are available in a variety of materials including, without limitation, Zirconia oxide, and are available from a variety of sources including, without limitation, Impact Bearings of San Clemente, California. Rotating cylindrical cathode sputtering systems typically include a power source, a cathode, and a magnet assembly. The power source is connected to the cathode through an electrode and the magnet is positioned within the rotating cathode. The cathode (or "target") is then placed in a substantially evacuated chamber together with an object to be coated and an inert gas, such as Argon. Power is applied to the rotating cathode through the electrode as a substrate is passed over the rotating cathode. The combination of the energy from the power source, the magnetic field of the magnet assembly and the Argon gas, causes particles to be ejected from the target material of the cathode, and onto the substrate, thereby coating the substrate with target material. Known sputtering cylindrical cathode deposition systems operate using direct current (DC) or low- to medium-frequency (typically in the kilohertz range) alternating current (AC). Where insulating target materials (such as ceramics or oxides) are to be deposited, such devices typically require the use of metal doping for effective sputtering. Such systems often rely on the reactive nature of oxygen to eliminate the metal doping material during deposition. Such elimination, however, may not be complete or even. The result can be pinholes or impurities in the deposited film, and may require coatings of a higher thickness than would otherwise be desirable, or the use of secondary processes. The apparatus and methods of the present invention allows for use of radio-frequency (RF) power in the sputtering operation. The use of RF power allows for sputtering of non-conductive materials such as ceramics and oxides with minimal or no metal doping, allows for higher quality coatings with fewer imperfections, and reduces the need for secondary processing, thereby allowing for more efficient operation. Problems that occur when attempting to sputter with RF energy include inductive heating and magnetic effects caused by the RF energy in ferrous components. The present invention addresses these problems and enables RF sputtering of un-doped insulating materials with a rotating magnetron cylindrical cathode sputtering apparatus. The present invention also allows, in certain preferred embodiments, the use of only one cathode, whereas prior-known AC sputtering devices typically use two electrically-linked cathodes. Other embodiments of the present invention allow for the use of multiple cathodes, but it is understood that the use of multiple cathodes is rendered optional by the present invention. Referring to Shaft assembly 300 passes into mounting plate assembly 500 and mechanically connects to cathode 200. The interfaces between cathode 200 and mounting plate assembly 500, and/or between shaft assembly 300 and mounting plate assembly 500 are adapted to minimize or eliminate leaks in the substantially evacuated chamber (not illustrated), as is understood by those of ordinary skill in the art. As is illustrated, shaft assembly 300 is generally coaxial with cathode 200. The connection between shaft assembly 300 and cathode 200 is adapted such that rotation of shaft assembly 300 causes rotation of cathode 200, but isolates cathode 200 from shaft assembly 300 electrically. Preferably, little or no electrical energy should transfer between shaft assembly 300 and cathode 200 through direct electrical contact/ conduction. In this way, the energy transfer to cathode 200 during operation is entirely, or almost entirely, through power deliver assembly 100. The result is more efficient delivery of power to cathode 200 than would otherwise occur. A suitable means of connection is described further below. Drive motor assembly 400 is adapted to rotate shaft assembly 300. While a variety of rotation speeds may be used, and the present invention is not limited to any particular range of rotation speeds, speeds between one rotation per minute and twelve rotations per minute are suitable for most applications with the apparatus of the present invention. Drive motor assembly 400 may conveniently attach to outer housing assembly 700 and inner housing assembly 600 with mechanical fasteners. As illustrated in To enable sputtering with RF emissions, the RF power supply 800 is preferably adapted to supply RF energy at frequencies of 1 MHz or higher. Suitable power supplies are available from suppliers including MKS of Rochester, New York, including, without limitation, the Sure Power RF Plasma Generator, model QL10513, which is a sweeping frequency RF power supply, and but one example of an RF power supply suitable for use in preferred embodiments of the present invention. Frequencies of 13MHz or higher, 25MHz or higher, 300MHz or higher, and 1 GHz may be used in various sputtering applications depending on the target material utilized, the sputtering energy available, and the desired substrate material and coating characteristics. Radio frequencies suitable for use in industrial sputtering applications are further described in 47 C.F.R. § 18 (Code of Federal Regulations of the United States of America related to industrial, scientific and medical equipment). The present invention, however, is not limited to any one frequency range, and is suitable for sputtering with frequencies from 1 MHz to well above 1 GHz, including into the microwave range. By utilizing RF power at or above 1 MHz, electrode 110 acts as an antenna transmitting RF energy into cathode 200 instead of conducting it through a brush. That energy, in combination with the magnetic field generated by magnetic field source 140 causes the target material in the outer surface of cathode 200 to eject during operation, an effect known as "sputtering." When RF power is used, it is desirable to maintain a constant and preferably optimal load on power supply 800 in order to allow it to operate efficiently. To help ensure a consistent load on power supply 800, load matching tuner 810 may be used. Power supply 800 is electrically connected to power delivery assembly 100 through load matching tuner 810. Load matching tuner 810 may conveniently be a load matching tuner comprising capacitors and/or inductors, such as are known to those of ordinary skill in the art. Suitable tuners are available from suppliers including MKS of Rochester, New York. The MWH-100-03, 10 kW Load Matching Network, available from MKS, is one example of a load matching tuner suitable for use in certain embodiments of the present invention. Depending on the frequencies, energy levels, target materials used, and substrate location, it may also be desirable to adjust the position of magnetic field source 140. By adjusting the mounting structure (described further below) of magnetic field source 140, magnetic field source 140 can be adjusted with respect to its proximity to the inside surface of cathode 200 by moving it closer to the inside surface of cathode 200 and away from electrode 110, or closer to electrode 110 and away from the inner surface of cathode 200. The position of magnetic field source 140 within cathode 200 may also be adjusted radially, allowing for adjustment of the angle at which material is ejected during operation, by rotating magnetic field source 140 about electrode 110. While operation at RF frequencies enables sputtering of insulating materials, such frequencies also have the potential to induce inductive heating and magnetic fields in ferrous components. Accordingly, it is preferred, when operating at RF frequencies, that cathode 200 be electrically isolated from the other components of sputtering cathode apparatus 1 and that non-ferrous materials be utilized where feasible, except in magnetic field source 140 (described further below). It is also desirable that sputtering cathode apparatus 1 be cooled during operation. This may be accomplished by adding a cooling pump 900 adapted to pump a cooling medium such as de-ionized water into cathode 200 during operation. While a variety of pumps and cooling systems may be used, a McQuay 20 ton chiller (not illustrated) used in conjunction with a high volume water pump 900 is one suitable choice for preferred embodiments of the present invention. Referring again to As illustrated, electrode 110 may be formed of connecting sections including, without limitation, outer section(s) 102, interior section 111, and one or more extending sections 112. In this way, a variety of electrode lengths may be used, thereby allowing for the use of cathodes of varying lengths, by adding or removing extending sections 112 or using extending sections 112 of different lengths. Where leakage of cooling medium is not desired, flanges (e.g. first electrode flange 106 and second electrode flange 108), with a gasket (e.g. electrode flange O ring 105, which may be conveniently formed of Viton) between, and mechanical fasteners 109 (preferably of non-ferrous metal), may be used to connect sections of electrode 110. Where leakage is not as much of a concern, a simple friction fitting may be used, as is shown between interior section 111 and extending section 112. As illustrated magnetic field source 140 (described further below) serves to keep interior section 111 and extending section 112 from separating during operation, but other means of securing, including without limitation set screws, mechanical fasteners, and friction-fitting may also be used if desired. Passages 1 14 are preferably at the outer end of final extending section 112, but may be placed elsewhere on electrode 110 either instead of, or in addition to, at the outer end of final extending section 112. Insulating, and preferably ceramic, end piece bushing 116 provides support for electrode 110 while allowing cathode 200 to rotate about it. ULTEM is one suitable material for end piece bushing 116. Electrode 110 may be formed of any material suitable for use in transmitting RF energy including, without limitation brass, and will preferably be a non-ferrous material to aid in minimizing undesirable magnetic effects, as should mechanical fasteners 109, which may suitably be 304 stainless steel. Magnetic field source 140 may attach to electrode 110 as illustrated with lower clamping members 146 and upper clamping members 144. By using larger upper clamping members 144, or other adjustment means known to those of skill in the art, the proximity of magnetic field source 140 to the inside surface of cathode 200 may be adjusted. Magnetic field source 140 may also be adjusted radially by loosening upper clamping member 144 and lower clamping member 146 and rotating magnetic field source 140 about electrode 110, before re-tightening. Magnetic field source 140 may conveniently comprise carrier 148 and magnets 142, with securing members 149 securing magnets 142 in place. While the precise magnets used will vary based on the sputtering application (as is understood in the art), a plurality of 12.7 mm x 12.7 mm x 6.35 mm (1/2" x 1/2" x 1/4") magnets of grade N42, stacked two-high to form 12.7 mm (1/2") cubes would be appropriate choices for magnets 142 for typical applications. By way of example, and without limitation, approximately 240 such magnets 142 arranged in three rows could be used with a cathode 200 of approximately 55.88 cm (approximately 22 inches). Such magnets are available from a host of suppliers such as K&J Magnetics, Inc. Carrier 148, upper clamping members 144, lower clamping members 146, securing members 149 and any fasteners used to secure those components, should preferably be of non-ferrous materials. While insulating materials such as PVC can be utilized, non-ferrous thermally conductive materials such as aluminum are preferred as they allow for better cooling and heat transfer. As illustrated, electrode 110 is not in direct electrical contact with cathode 200. In such embodiments, RF energy is transmitted from electrode 110 to cathode 200, as opposed to being transferred by conduction through direct contact. Where conductive transfer is also desired, brushes (not illustrated) may be used to create a direct electrical connection between electrode 110 and cathode 200 as well. However, the use of RF emissions means that such brushes are not required as they are with lower frequencies, at which direct electrical contact is needed. A variety of suitable brushes are known to those of ordinary skill in the art. Cathode assembly 200 is shown in further detail on Sacrificial target 205 is substantially hollow, and is adapted such that magnetic field source 140 will fit within sacrificial target 205, along with at least a portion of electrode 110, which preferably extends at least to the center point of the length of sacrificial target 205, thereby delivering RF power centrally within cathode assembly 200, which is preferred. Cathode flange assembly 220 comprises cathode flange 230, spiral cathode retaining ring 226, cathode flange O ring 224, and cathode flange insulator 222. Both cathode flange O ring 224 and cathode flange insulator 222 may conveniently be formed of Viton. Cathode flange 230, which may conveniently be formed of aluminum, fits over sacrificial target 205. Spiral cathode retaining ring 226 secures cathode flange 230. Tightening cathode flange fasteners 234 allows cathode 200 to operatively connect to shaft assembly 300 such that rotation of shaft assembly 300 rotates cathode assembly 200. Cathode flange insulator 222 (which may conveniently formed of a material with high dielectric resistance such as ULTEM) electrically isolates cathode assembly 200 from shaft assembly 300, which is desirable when dealing with high frequency RF power, for reasons including because it reduces the likelihood of arcing. Cathode flange fasteners 234 (which may be conveniently formed of 304 stainless steel) form the mechanical connection, but do so through cathode flange fastener insulators 232 (which may also be formed of ULTEM). The purpose is to provide electrical isolation by ensuring that cathode flange fasteners 234 are not in conductive contact with cathode assembly 200, thereby helping ensure that power transfers to cathode assembly 200 almost exclusively through power delivery assembly 100 and not secondarily through shaft assembly 300. Cathode end cap assembly 210 serves two purposes. First, it provides a seal that prevents leakage of the cooling medium. Second, it provides support for the end of electrode 110. Cathode end cap assembly 210 comprises cathode end cap retaining ring 211 (which may conveniently be formed of 304 stainless steel) and cathode end cap plate 212, which is also preferably formed of a non-ferrous material such as aluminum. Insulating cathode end plate bearing 215, which may conveniently be formed of a ceramic material such as Zirconia Oxide, supports the end piece bushing 116 and allows cathode 200 to rotate about it. Insulating cathode end plate bearing 215 is held within cathode end plate plug 214, which seals against the inner surface of sacrificial target 205 to prevent leakage of the cooling medium. Cathode end plate plug 214 may be attached to cathode end cap plate 212 with mechanical fasteners (not illustrated) and is sealed with cathode end plate O rings 213, which may conveniently be formed of Viton. Given the ability of apparatus 1 to operate at high frequency RF energy levels, a variety of materials may be used for target material in outer surface 206 of sacrificial target 205, including, without limitation, oxides and ceramics. Shaft assembly 300 is shown in greater detail in Key slot 312 is integrated into shaft 310 to allow for attachment of a lower pulley 418 via lower pulley key 420, as is shown in As has been discussed, mounting plate assembly 500 is attached to the wall 512 of the substantially evacuated chamber (not illustrated). Mounting plate assembly 500 connects to inner housing assembly 600 (as shown in Inner housing seal 628 may conveniently be a rotating water pump shaft seal such as a John Crane shaft seal, type 21, and is adapted to operate in conjunction with race 630 to reduce or eliminate vacuum leaks, while still allowing shaft 310 to rotate. Second inner housing bearing 626 (which may also be an insulating ceramic bearing formed of a material such as Zirconia Oxide) further supports shaft assembly 300 without creating a direct electrical connection to inner housing body 610, and is held in place by second inner housing snap ring 629, second inner housing bearing seal 622, and spacer 624. First inner housing opening 640 and second inner housing opening 642 allow for monitoring for vacuum leaks, and possibly the use of a secondary vacuum pump to compensate for small vacuum leaks, which will occur over time as inner housing seal 628 wears. Inner housing oil seal retaining ring 620 (which may conveniently be formed of 304 stainless steel) acting to prevent leakage. Also disclosed herein is a method of depositing material with a rotating cylindrical magnetron sputtering cathode apparatus comprising a radio frequency power supply, a power delivery assembly, a rotating cathode, a shaft and a drive motor. Apparatus 1, described in detail above, is one suitable apparatus for use in connection with this method, but, as will be understood, it is not necessary to include all of the features of apparatus 1 in order to utilize the method. As has been described, power delivery assembly 100 comprises a magnetic field source 140 positioned within cathode 200 and an electrode 110 extending within cathode 200. The outer surface 206 of the sacrificial target 205 of cathode 200 comprises a target material. Electrode 110 is electrically isolated from shaft assembly 300, and shaft assembly 300 is generally coaxial with cathode 200. To facilitate RF operation, electrode 110 and said shaft assembly 300 are formed from non-ferrous materials. Given an apparatus with the above characteristics, material may be deposited by causing the power supply 800 to supply radio frequency energy at frequencies of 1 MHz or higher, through electrode 110. Cathode 200 is then caused to rotate about magnetic field source 140. By positioning a substrate (meaning an object on which material is to be deposited) 290 proximate to the outside surface of cathode 200, radio frequency energy from the power source, transmitted through the electrode, in combination with the magnetic field generated by magnetic field source 140 will cause particles of target material from outer surface 206 to eject onto substrate 290. Alternative frequencies may be used with this method, including frequencies of 13MHz or higher, 25MHz or higher, 300MHz or higher, and 1 GHz or higher (with no set upper limit). When frequencies above 1MHz are used in conjunction with this method, it is not necessary that electrode 1 10 be in direct electrical contact with cathode 200 as the RF energy will be transmitted if not conducted between the two. The utilization of higher frequency RF emissions in this method permits sputtering of target materials which are un-doped insulating materials substantially free of conducting materials. In this way, with an apparatus 1 comprising a radio frequency power supply 800 and a cylindrical rotating cathode 200 having an outer surface 206 of sacrificial target material comprising an oxide such as, without limitation, Zinc Oxide or Aluminum Oxide, can sputter the oxide directly without requiring doping. As has been described, this can be accomplished by causing power supply 800 to supply radio frequency energy at frequencies of 1 MHz or higher (with frequencies above 13MHz, 25MHz, 300MHz, and 1 GHz all being suitable in different applications, causing said cathode 200 to rotate, and positioning substrate 290 proximate to the outside surface of cathode 200, whereby the radio frequency energy and magnetic field cause cathode 200 to eject particles onto substrate 290. The above-described preferred embodiments are intended to be exemplary, and not limiting. Other variations and embodiments of the apparatus and methods of the present invention will be apparent to those of ordinary skill in the art in light of this specification, all of which are within the scope of the present invention as claimed. Further particular and preferred aspects of the invention are set out in the accompanying independent and dependent clauses. Features of the dependent clauses may be combined with those of the independent clauses and independent claims as appropriate and in combinations other than those explicitly set out in the clauses and claims.
A rotating magnetron sputtering cathode apparatus (1) comprising a radio frequency power supply (800), a power delivery assembly (100), a cylindrical rotating cathode (200), a shaft (300) and a drive motor (400) wherein The apparatus of claim 1 wherein said electrode (110) is arranged not to be in direct electrical contact with said cathode (200). The apparatus of claim 1 wherein said power supply (800) is adapted to supply radio frequency energy at frequencies of 13MHz or higher. The apparatus of claim 3 wherein said power supply is adapted to supply radio frequency energy at frequencies of 25MHz or higher. The apparatus of claim 4 wherein said power supply is adapted to supply radio frequency energy at frequencies of 300MHz or higher. The apparatus of claim 5 wherein said power supply is adapted to supply radio frequency energy at frequencies of 1GHz or higher. The apparatus of claim 1 wherein said target material (205) consists of an insulating material substantially free of conducting materials. The apparatus of claim 1 wherein the position of said magnetic field source (140) within said cathode (200) is adjustable with respect to its proximity to the inside surface of said cathode. The apparatus of claim 1 wherein the position of said magnetic field source within said cathode is radially adjustable about said electrode (110). The apparatus of claim 1 further comprising a cooling pump (900) adapted to pump a cooling medium wherein The apparatus of claim 10 wherein said channelled bearing assembly comprises a non-conductive ceramic bearing (314) in at least partial contact with said electrode. A method of depositing material with a rotating cylindrical magnetron sputtering cathode apparatus (1) comprising a radio frequency power supply (800), a power delivery assembly (100), a rotating cathode (200), a shaft (300) and a drive motor (400) wherein supplying radio frequency energy at frequencies of 1 MHz or higher to the electrode; rotating the cathode about said magnetic field source; and positioning a substrate (290) proximate to said outside surface of said cathode; The method of claim 12 wherein said electrode (110) is arranged not to be in direct electrical contact with said cathode (200). The method of claim 12 wherein said power supply (800) is adapted to supply radio frequency energy at frequencies of 13MHz or higher. The method of claim 14 wherein said power supply is adapted to supply radio frequency energy at frequencies of 25MHz or higher. The method of claim 15 wherein said power supply is adapted to supply radio frequency energy at frequencies of 300MHz or higher. The method of claim 16 wherein said power supply is adapted to supply radio frequency energy at frequencies of 1 GHz or higher. The method of claim 12 wherein said target material is formed of insulating materials and is substantially free of conducting materials. The method of claim 12, wherein said target material (205) is formed of an oxide.BACKGROUND
SUMMARY
BRIEF DESCRIPTION OF THE DRAWINGS
DETAILED DESCRIPTION
said power delivery assembly comprises a magnetic field source positioned within said cathode and an electrode extending within said cathode;
said electrode is electrically isolated from said shaft;
the outer surface of said cathode comprises a target material formed of insulating materials and substantially free of conductive materials;
said method comprising the steps of
causing said power supply to supply radio frequency energy at frequencies of I MHz or higher;
causing said cathode to rotate about said magnetic field source; and positioning a substrate proximate to outside surface of said cathode;
whereby said radio frequency energy a causes said rotating cathode to eject particles from said target material onto said substrate.
said method comprising the steps of
causing said power supply to supply radio frequency energy at frequencies of 1 MHz or higher;
causing said cathode to rotate; and
positioning a substrate proximate to said outside surface of said cathode;
whereby said radio frequency energy causes said cathode to eject particles from said target material onto said substrate.
said power delivery assembly comprises a magnetic field source (140) positioned within said cathode and an electrode (110) extending within said cathode; the outer surface (206) of said cathode comprises a target material (205); said electrode is arranged to be electrically isolated from said shaft;
said electrode and said shaft are formed from non-ferrous materials;
said shaft is arranged to be generally coaxial with said cathode and arranged to be mechanically connected to said cathode such that said shaft and said cathode are electrically isolated and rotation of said shaft causes said cathode to rotate about said magnetic field source and a portion of said electrode;
said drive motor is adapted to rotate said shaft;
said power supply is adapted to supply radio frequency energy at frequencies of 1GHz or higher; and
said electrode is arranged to be electrically connected to said power supply.
said electrode is substantially hollow and adapted to operatively connect to said cooling pump;
said electrode is adapted to deliver a cooling medium into said cathode from said cooling pump; and
said shaft and said power delivery assembly further comprise an insulating, channelled bearing assembly adapted to allow said cooling medium to flow out of said cathode; said cooling medium being arranged to flow into said hollow electrode and through said channelled bearing assembly, thereby cooling said power delivery assembly and said cathode.
said power delivery assembly comprises a magnetic field source (140) positioned within said cathode and an electrode, (110) extending within said cathode; the outer surface (206) of said cathode comprises a target material (205);
said electrode is arranged to be electrically isolated from said shaft;
said shaft is arranged to be generally coaxial with said cathode; and
said electrode and said shaft are formed from non-ferrous materials;
said method comprising the steps of
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