A HIGH-FREQUENCY PLASMA PROCESS WHEREIN THE PLASMA IS EXCITED BY AN INDUCTIVE STRUCTURE IN WHICH THE PHASE AND ANTI-PHASE PORTIONS OF THE CAPACITIVE CURRENTS BETWEEN THE INDUCTIVE STRUCTURE AND THE PLASMA ARE BALANCED

Abstract: A process for fabricating a product (28, 119). The process comprises the steps of subjecting a substrate to a composition of entities, at least one of the entities emanating from a species generated by a gaseous discharge excited by a high frequency field in which the vector sum of phase and anti-phase capacitive coupled voltages from the inductive coupling structure substantially balances.

Description: PC17IB96/01270 A HIGH-FREQUENCY PLASMA PROCESS WHEREIN THE PLASMA IS EXCITED BY AN INDUCTIVE STRUCTURE IN WHICH THE PHASE AND ANTI-PHASE PORTIONS OF THE CAPACITIVE CURRENTS BETWEEN THE INDUCTIVE STRUCTURE AND THE PLASMA ARE BALANCED BACKGROUND OF THE INVENTION This invenuon relates generally to plasma processing. More parucularly, the invention is for plasma processing of devices using an inducuve discharge. This invenuon is illustrated tn an example with regard to plasma etching and resist stripping of semiconductor devices. The invenuon also is illustrated with regard to chemical vapor deposiuon (CVD) of semiconductor devices. But it will be recognized that the invenuon has a wider range of applicability. Merely by way of example, the invenuon also can be applied in other plasma etching appiicauons, and deposiuon of materials such as silicon, silicon dioxide, silicon nitride, polysilicon. among others. Plasma processing techniques can occur in a variety of semiconductor manufacturing processes. Examples of plasma processing techniques occur in chemical dry etching (CDE), ion-assisted etching (IAE), and plasma enhanced chemical vapor deposiuon (PECVD), including remote plasma deposiuon (RPCVD) and ion-assisted plasma enhanced chemical vapor deposiuon (lAPECVD). These plasma processing techniques often rely upon radio frequencv power (rf) supplied to an inducuve coil for providing power to gas phase species in forming a plasma. Plasmas can be used to form neutral species (i.e.. uncharged) for purposes of removing or forming films in the manufacture of integrated circuit devices. For instance, chemical dry etching generally depends on gas-surface reactions involving these neutral species without substantial ion bombardment. In other manufacturing processes, ion bombardment to substrate surfaces is often undesirable. This ion bombardment, however, is known to have harmful effects on properties of material layers in devices and excessive ion bombardment flux and energy can lead to intermixing of materials in adjacent device layers, breaking down oxide and "wear out, " injecting of contaminaove material formed in the processing environment into substrate material layers, harmful changes in substrate morphology (e.g. amophoαzanon), etc. SUBSTITUTE SHEcr Ion assisted etching processes, however, rely upon ion bombardment to the substrate surface in defining selected films. But these ion assisted etching processes commonly have a lower selecuvity relauve to conventional CDE processes. Hence, CDE is often chosen when high selecuvity is desired and ton bombardment to substrates are to be avoided. One commonly used chemical dry etching technique is conventional photoresist stripping, often termed ashing or stripping. Convenuonal resist stripping relies upon a reaction between a neutral gas phase species and a surface material layer, typicaily for removal. This reacuon generally forms volaule products with the surface material layer for its removal. The neutral gas phase species is formed by a plasma discharge. This plasma discharge can be sustained by a coil (e.g., helical coil, etc.) operating at a selected frequency in a convenuonal photoresist stripper. An example of the convenuonal photoresist stripper is a quarter-wave helical resonator stripper, which is described by U.S. Patent No. 4,368,092 in the name of Steinberg gj l. Referring to the above, an objective in chemical dry etching is to reduce or even eliminate ion bombardment (or ion flux) to surfaces being processed to maintain the desired etching selectivity. In practice, however, it is often difficult to achieve using convenuonal techniques. These convenuonal techniques generally attempt to control ion flux by suppressing the amount of charged species in the plasma source reaching the process chamber. A variety of techniques for suppressing these charged species have been proposed. These techniques often rely upon shields, baffles, large separation distances between the plasma source and the chamber, or the like, placed between the plasma source and the process chamber. The conventional techniques generally attempt to directly suppress charge density downstream of the plasma source by interfering wiui convecrive and diffusive transport of charged species. They tend to promote recombinauon of charged species by either increasing the surface area (e.g., baffles, etc.) reladve to volume, or increasing flow αme, which relates to increasing the distance between the plasma source and the process chamber. These baffles, however, cause loss of desirable neutrai etchant species as well. The baffles, shields, and alike, also are often cumbersome Baffles, shields, or the large separation distances also cause undesirable recombinauve loss of acuve species and someumes cause radio frequency power loss and ou er problems These baffles and shields also are a potenual source of paniculate contamination, which is often damaging to integrated circuits. Baffles, shields, spatial separauon. and alike, when used alone also are often insufficient to substanuaily prevent unwanted parasiuc plasma currents These plasma currents are generated between the wafer and the plasma source, or between the plasma source and wails of the chamber. It is commonly known that when initial charged species levels are present in an electrical field, the charged species are accelerated and dissociauve collisions with neutral panicles can muluply the concentrauon of charge to higher levels. If sufficient "seed" levels of charge and rf potentials are present, the parasiuc plasma in the vicinity of the process wafer can reach harmful charge density levels. In some cases, these charge densities may be similar to or even greater d n plasma density within the source plasma region, thereby causing even more ion flux to the substrate. Charge densiues also create a voltage difference between the plasma source and processing chamber or substrate support, which can have an addiuonal deleterious effect. This voltage difference enhances electric fields that can accelerate extracαon of charge from the plasma source. Hence, their presence often induces increased levels of charge to be irregularly transported from the plasma source to process substrates, thereby causing non-uniform ion assisted etching. Conventional ion assisted plasma etching, however, often requires control and maintenance of ion flux intensity and umformity within selected process limits and within selected process energy ranges. Control and maintenance of ion flux intensity and umformity are often difficult to achieve using convenuonal techniques. For instance, capaciuve coupling between high voltage selecuons of the coil and die plasma discharge often cause high and uncontrollable plasma potentials relative to ground. It is generally understood that voltage difference between the plasma and ground can cause damaging high energy ion bombardment of a icles being processed by the plasma, as illustrated by U.S. Patent No. 5,234.529 in the name of Johnson. It is further often understood that rf component of u e plasma potential varies in time since it is derived from a coupling to time varying rf excitation. Hence, the energy of charged particles from plasma in convenuonal inductive sources is spread over a relatively wide range of energies, which undesirably tends to introduce uncontrolled variations in the processing of articles by the plasma. The voltage difference between the region just outside of a piasma source and the processing chamber can be modified by introducing internal conductive shields or electrode elements into the processing apparatus downstream of die source. When the plasma potential is elevated with respect to these shield electrodes, however, there is a tendency to generate an undesirable capacitive discharge between the shield and plasma source. These electrode elements are often a source of contamination and the likelihood for contamination is even greater when there is capacitive discharge (ton bombardment from capacitive discharge is a potential source of sputtered material). Contamination is damaging to d e manufacture of integrated circuit devices. Another limitation is that the shield or electrode elements generally require small holes therein as structural elements. These small holes are designed to allow gas to flow therethrough. The small holes, however, tend to introduce unwanted pressure drops and neutral species recombination. If the holes are made larger, the plasma from the source tends to survive transpon through the holes and unwanted downstream charge flux will often result. In addition, undesirable discharges to these holes in shields can, at times, produce an even more undesirable hollow cathode effect. In convenuonal helical resonator designs, conductive external shields are interposed between die inductive power (e.g., coil, etc.) and walls of the vacuum vessel containing the plasma. A variety limitations wiώ these external capacitive shielded plasma designs (e.g., helical resonator, inductive discharge, etc.) have been observed. In particular, the capaciύvely shielded design often produces plasmas that are difficult to tune and even ignite. Alternauvely, the use of unshielded plasma sources (e.g., conventional quaner-wave resonator, conventional half-wave resonator, etc.) attain a substanual plasma potenuai from capaciuve coupling to the coil, and hence are prone to create uncontrolled parasitic plasma currents to grounded surfaces. Accordingly, the use of either the shielded or the unshielded sources using convenuonal quarter and half-wave rf frequencies produce undesirable results. In many convenuonal plasma sources a means of cooling is required to maintain the plasma source and substrates being treated below a maximum temperature limit. Power dissipauon in the structure causes heaung and thereby increases the difficulty and expense of impiemenung effecuve cooling means. Inducuve currents may also be coupled from the excitauon coil into internal or capacitive shields and these currents are an additional source of undesirable power loss and heaung. Conventional capacitive shielding in helical resonator discharges utilized a shield which was substantially split along d e long axis of the resonator to lessen eddy current loss. However, such a shield substantially perturbs the resonator characteristics owing to unwanted capacitive coupling and current which flows from d e coil to the shield. Since there are no general design equauons. nor are properties currendy known for resonators which are "loaded" with a shield along the axis, sources using this design must be sized and made to work by tnal and error. In inducuve discharges, it is highly desirable to be able to substantially control me plasma potential relative to ground potenuai, independent of input power, pressure, gas composition and other variables. In many cases, it is desired to have the plasma potential be substantially at ground potenuai (at least offset from ground potential by an amount insignificantly different from die floaung potential or intrinsic DC plasma potential). For example, when a plasma source is utilized to generate neutral species to be transported downstream of die source for use in ashing resist on a semiconductor device substrate (a wafer or flat panel electroruc display), me concentration and potential of charged plasma species in me reaction zone are desirably reduced to avoid charging damage from electron or ionic current from the plasma to the device. When there is a substantial potential difference between plasma in the source and grounded surfaces beyond die source, there is a tendency for unwanted parasitic plasma discharges to form outside of d e source region. Anod er undesirable effect of potential difference is the accelerauon of ions toward grounded surfaces and subsequent impact of d e energetic ions with surfaces. High energy ion bombardment may cause lattice damage to the device substrate being processed and may cause the chamber wall or other chamber materials to sputter and contaminate device wafers. In other plasma processing procedures, however, some ion bombardment may be necessary or desirable, as is die case panicuiarly for anisotropic ion-induced plasma etching procedures (for a discussion of ion-enhanced plasma etching mechanisms See. Flamm (Ch. 2, pp.94- 183 in Plasma Etching, An Introduction, D. M. Manos and D.L. Flamm. eds.. Academic Press, 1989)). Consequentiy, uncontrolled potential differences, such as that caused by "stray" capacitive coupling from d e coil of an inducuve plasma source to d e plasma, are undesirable. Refernng to the above limitations, conventional plasma sources also have disadvantages when used in conventional plasma enhanced CVD techniques. These techniques commonly form a reaction of a gas composition in a plasma discharge. One conventional plasma enhanced technique relies upon ions aiding in rearranging and stabilizing the film, provided the bombardment from the plasma is not sufficiently energetic to damage die underlying substrate or de growing film. Conventional resonators and outer types of inductive discharges often produce parasitic plasma currents from capacitive coupling, which oft n detrimentally influences film quality, e.g., an inferior film, etc. These parasitic plasma currents are often uncontrollable, and highly undesirable. These plasma sources also have disadvantages in other plasma processing techniques such as ion-assisted etching, and others. Of course, the particular disadvantage will often depend upon the application. To clarify certain concepts used in this application, it will be convenient to introduce ώese definitions. Ground (or ground potential): These terms are defined as a reference potential which is generally taken as the potential of a highly conductive shield or odier highly conductive surface which surrounds the plasma source. To be a true ground shield in the 5 sense of this definiuon, the RF conductance at the operating frequency is often substantially high so that potenuai differences generated by current wiϋ in die shield are of negligible magnitude compared to potenuals lntenuonally applied to d e various structures and elements of the plasma source or substrate suppoπ assembly. 10 However, some realizauons of plasma sources do not incorporate a shield or surface with adequate electrical susceptance to meet tins definition. In implementauons where there is a surrounding conducuve surface that is somewhat similar to a ground shield or ground plane, the ground potenuai is taken to be the fictiuous 15 potential which die imperfect grounded surface would have equilibrated to if it had zero high frequency impedance. In designs where there is no physical surface which is adequately configured or which does not have insufficient susceptance to act as a "ground" according to die above definition, ground potential is the potential of 20 a fictitious surface which is equi-potential with d e shield or "ground" conductor of an unbalanced transmission line connection to de plasma source at its RF feed point. In designs where die plasma source is connected to an RF generator with a balanced transmission line RF feed, "ground" potential is the average of the driven feed 25 line potentials at the point where the feed lines are coupled to the plasma source. Inducαvely Coupled Power: This term is defined as power transferred to d e plasma substantially by means of a tune-varying 30 magnetic flux which is induced witiiin he volume containing die plasma source. A time-varying magnetic flux induces an electromotive force in accord wirh Maxwell's equauons. This electromotive force induces motion by electrons and other charged particles in the plasma and thereby imparts energy to these particles. 35 RF inductive power source and bias power supply: In most conventional inducuve plasma source reactors, power is supplied to an inductive coupling element (ώe inducuve coupling element is often a multi-turn coil which abuts a dielectric wall containing a gas 40 where the plasma is ignited at low pressure) by an rf power generator. Conventional Helical Resonator: Convenuonal helical resonator can be defined as plasma applicators. These plasma applicators have 45 been designed and operated in multiple configurations, which were described in, for example, U.S. Patent No. 4,918,031 in the names of Flamm ςj. ]., U.S. Patent No. 4,368,092 in die name of Steinberg & ]. , U.S Patent No. 5,304,282 in the name of Flamm. U.S. Patent No. 5,234,529 in the name of Johnson, U.S. Patent No 5,431,968 in the name of Miller, and others In these configurauons, one end of die helical resonator applicator coil has been grounded to its outer shield. In one convenuonal configuration, a quarter wavelength helical resonator secuon is employed with one end of die applicator coil grounded and the other end floaung (i.e., open circuited). A tnmming capacitance is someumes connected between the grounded outer shield and the coil to "fine tune" the quarter wave structure to a desired resonant frequency that is below die nauve resonant frequency without added capacitance. In anodier convenuonal configurauon, a half- wavelength helical resonator secuon was employed in which botii ends of the coil were grounded. The funcuon of grounding the one or both ends of die coil was believed to be not essenual, but advantageous to "stabilize the plasma operating charactensucs" and "reduce the possibility of coupling stray current to nearby objects. " See. U.S. Patent No. 4,918,031. Convenuonal resonators have also been constructed in oώer geometrical configurauons. For instance, die design of helical resonators widi a shield of square cross section is described in Zverev si a]., IRE Transacuons on Component Parts, pp. 99-110, Sept. 1961. Johnson (U.S. Patent No. 5,234,529) teaches that one end of die cylindrical spiral coil in a convenuonal helical resonator may be deformed into a planar spiral above the top surface of d e plasma reactor tube. U.S. Patent No. 5,241,245 in die names of Barnes ej aj. teach the use of convenuonal helical resonators in which die spiral cylindrical coil is enurely deformed into a planar spiral arrangement with no helical coil component along d e sidewalls of the plasma source (this geometry has often been referred to as a "transformer coupled plasma, " termed a TCP). From die above it is seen that an improved technique, including a method and apparatus, for plasma processing is often desired. SUMMARY OF THE INVENTION The present invention provides a techmque, including a method and apparatus, for fabncaung a product using a plasma discharge. The present techmque relies upon the control of d e instantaneous plasma AC potential to selecuvely control a vanety of plasma charactensucs. These charactensucs include the amount of neutral species, the amount of charged species, overall plasma potential, the spaual extent and distnbuuon of plasma density, the distnbuuon of electncal current, and others. This technique can be used in appiicauons including chemical dry etching (e.g., stnpping, etc.), ion-enhanced etching, plasma immersion ion tmplantauon, chemical vapor deposiuon and material growth, and others. In one aspect of die invenuon, a process for fabncaung a product is provided. These products include a vaneues of devices (e.g., semiconductor, flat panel displays, micro-machined structures, etc.) and matenals, e.g., diamonds, raw matenals, plastics, etc. The process includes steps of subjecung a substrate to a composition of entities. At least one of the enuties emanates from a species generated by a gaseous discharge excited by a high frequency field in which the vector sum of phase and anu-phase capacitive coupled voltages (e.g., AC plasma voltage) from die inducuve coupling structure substanually balances. This process provides for a technique d al is substantially free from stray or parasitic capacitive coupling from the plasma source to chamber bodies (e.g., substrate, walls, etc.) at or near ground potential. In anotiier aspect of die invenuon, another process for fabncaung a product is provided. The process includes steps of subjecung a substrate to a composition of entities. At least one of the entities emanates from a species generated by a gaseous discharge excited by a high frequency field in which the vector sum of phase and anti-phase capacitive coupled voltages from the inducuve coupling structure is selecuvely maintained. This process provides for a techmque that can selectively control die amount of capacitive coupling to chamber bodies at or near ground potential. A further aspect of the invenuon provides yet another process for fabricating a product. This process includes steps of subjecting a substrate to a composition of entities. At least one of the enuties emanates from a species generated by a gaseous discharge excited by a high frequency field in which die vector sum of phase and anti-phase capacitive coupled voltages from the inducuve coupling structure is selectively maintained. A further step of selectively applying 10 a voltage between the at least one of the entities in d e plasma source and a substrate is provided. This process provides for a technique that can selecuvely control the amount of capacitive coupling to chamber bodies at or near ground potenuai, and provide for a driving voltage between the enuties and a substrate. Anodier aspect of d e invention provides another process for fabricating a product. The process comprises steps of subjecting a substrate to a composition of entities and using the resulting substrate for completion of the product. At least one of die entities emanates from a species generated by a gaseous discharge provided by a plasma applicator, e.g., a helical resonator, inductive coil, transmission line, etc. This plasma applicator has an integral current driven by capacitive coupling of a plasma column to elements with a selected potential greater than a surrounding shield potential substantially equal to capacitive coupling of die plasma column to substantially equal elements widi a potential below shield potential. In a further aspect, d e invention provides an apparatus for fabncaung a product. The apparatus has an enclosure comprising an outer surface and an inner surface. The enclosure houses a gaseous discharge. The apparatus also includes a plasma applicator (e.g., helical coil, inductive coil, transmission line, ex.) disposed adjacent to the outer surface. A high frequency power source operably coupled to die plasma applicator is included. The high frequency power source provides high frequency to excite t e gaseous discharge to provide at least one entity from a high frequency field in which die vector sum of phase and arm- phase capacitive current coupled from die inductive coupling structure is selectively maintained. In anodier aspect, die present invention provides an improved plasma discharge apparatus. This plasma discharge apparatus includes a plasma source, a plasma applicator (e.g., inductive coil, transmission line, etc.), and oώer elements. This plasma applicator provides a de-coupled plasma source. A wave adjustment circuit (e.g., RLC circuit, coil, transmission line, etc.) is operably coupled to die plas a applicator. The wave adjustment circuit can selectively adjust phase and anti-phase potentials of the plasma from an rf power supply. This 1 1 rf power supply is operably coupled to the wave adjustment circuit. The present invention achieves these benefits in the context of known process technology. However, a further understanding of the nature and advantages of d e present invention may be realized by reference to the latter poπions of die specificauon and attached drawings. BRIEF DESCRIPTION OF THE DRAWINGS Fig. 1 is a simplified diagram of a plasma etching apparatus according to d e present invenuon: Figs. 2A-2E are simplified configurauons using wave adjustment circuits according to the present invention; Fig. 3 is a simplified diagram of a chemical vapor deposition apparatus according to die present invention; Fig. 4 is a simplified diagram of a stnpper according to die present invention; Figs. 5A-5C are more detailed simplified diagrams of a helical resonator according to de present invenuon: Fig. 6 is a conventional quarter-wave helical resonator plasma etching apparatus with stray plasma which results from d e coupling in die conventional design; Fig. 7 is a simplified diagram of the rf voltage distribution along the coil of me Fig. 6 apparatus; Fig. 8 is a simplified top-view diagram of a stripping apparatus according to the present experiments; and Fig. 9 is a simplified side-view diagram of a stripping apparatus according to the present experiments. DETAILED DESCRIPTION OF THE INVENTION Fig. 1 is a simplified diagram of a plasma etch apparatus 10 according to die present invention. This etch apparatus is provided widi an inductive applicator, e.g., inductive coil. This etch apparatus depicted, however. is merely an illustration, and should not limit the scope of the claims as defined herein. One of ordinary skilled in d e an may implement the present invenuon widi odier treatment chambers and die like. The etch apparatus includes a chamber 12, a feed source 14. an exhaust 16, a pedestal 18. an inducuve applicator 20. a radio frequency (rf) power source 22 to the inductive applicator 20, wave adjustment circuits 24, 29 (WACs), a radio frequency power source 35 to die pedestal 18, a controller 36, and odier elements. Optionally, die etch apparatus includes a gas distributor 17. The chamber 12 can be any suitable chamber capable of housing a product 28, such as a wafer to be etched, and for providing a plasma discharge therein. The chamber can be a domed chamber for providing a uniform plasma distribution over the product 28 to be etched, but the chamber also can be configured in other shapes or geometries, e.g., flat ceiling, truncated pyramid, cylindrical, rectangular, etc. Depending upon die application, the chamber is selected to produce a uniform entity density over the pedestal 18, providing a high density of entities (i.e.. etchant species) for etching uniformity. The present chamber includes a dome 25 having an interior surface 26 made of quaru or other suitable matenals. The exterior surface of die chamber is typically a dielectnc material such as a ceramic or the like. Chamber 12 also includes a process kit widi a focus ring 32, a cover (not shown), and other elements. Preferably, die plasma discharge is derived from the inductively coupled plasma source that is a de-coupled plasma source (DPS) or a helical resonator, although other sources can be employed. The de-coupled source originates from rf power derived from the inductive applicator 20. Inductively coupled power is denved from die power source 22. T e rf signal frequencies ranging from 800 kHz to 80 MHz can be provided to die inductive applicator 20. Preferably, the rf signal frequencies range from 5 MHz to 60 MHz. The inducuve applicator (e.g., coil, antenna, transmission line, etc.) overlying die chamber ceiling can be made using a variety of shapes and ranges of shapes. For example, the inductive applicator can be a single integral conductive film, a transmission line, or multiple coil windings. The shape of the inducuve applicator and its location relauve to the chamber are selected to provide a plasma overlying the pedestal to improve etch uniformity. The plasma discharge (or plasma source) is denved from d e inducuve applicator 20 operaung at selected phase 23 and anti-phase 27 potenuals (i.e., voltages) that substanually cancel each other. The controller 36 is operably coupled to die wave adjustment circuits 24, 29. In one embodiment, wave adjustment circuits 24, 29 provide an inducuve applicator operaung at full-wave muluples 21. This embodiment of full-wave muluple operauon provides for balanced capacitance of phase 23 and anu-phase voltages 27 along d e inducuve applicator (or coil adjacent to d e plasma). This full-wave muluple operauon reduces or substanually eliminates d e amount of capaciύvely coupled power from die plasma source to chamber bodies (e.g., pedestal, wails, wafer, etc.) at or close to ground potenuai. Altemauvely, the wave adjustment circuits 24, 29 provide an inducuve applicator that is effecuvely made shorter or longer than a full-wave length multiple by a selected amount, thereby operaung at selected phase and anu- phase voltages that are not full-wave multiples. Alternatively, more than two, one or even no wave adjustment circuits can be provided in odier embodiments. But in all of these above embodiments, die phase and anu-phase potentials substantially cancel each odier, diereby providing substanually no capaciuvely coupled power from die plasma source to the chamber bodies. In alternative embodiments, die wave adjustment circuit can be configured to provide selected phase and anu-phase coupled voltages coupled from die inducuve applicator to die plasma that do not cancel. This provides a controlled potenuai between die plasma and the chamber bodies, e.g., die substrate, grounded surfaces, walls, etc. In one embodiment, the wave adjustment circuits can be used to selectively reduce current (i.e., capaciαvely coupled current) to the plasma. This can occur when certain high potenuai difference regions of the inductive applicator to the plasma are posiuoned (or kept) away from the plasma region (or inductor-containing-the-piasma region) by making them go into die wafer adjustment circuit assemblies, which are typically configured outside of die plasma region. In this embodiment, capaciuve current is reduced and a selected degree of symmetry between the phase and anti-phase of the coupled voltages is maintained, thereby providing a selected potential or even substanually ground potenuai. In odier embodiments, the wave adjustment circuits can be used to selecuvely increase current (i.e., capaciuvely coupled current) to the plasma. As shown, die wave adjustment circuits are attached (e.g., connected, coupled, etc.) to ends of the inducuve applicator. Altemauvely, each of these wave adjustment circuits can be attached at an intermediate position away from the inducuve application ends. Accordingly, upper and lower tap posiuons for respective wave adjustment circuits can be adjustable. But both the inducuve applicator portions below and above each tap position are active. That is, they both can interact with d e plasma discharge. A sensing apparatus can be used to sense plasma voltage and use automauc tuning of die wave adjustment circuits and any rf matching circuit between the rf generator and die plasma treatment chamber. This sensing apparatus can maintain die average AC potential at zero or a selected value relative to ground or any other reference value. This wave adjustment circuit provides for a selected potential difference between d e plasma source and chamber bodies. These chamber bodies may be at a ground potenuai or a potenuai supplied by another bias supply, e.g., See. Fig. 1 reference numeral 35. Examples of wave adjustment circuits are described by way of the Figs, below. For instance. Figs. 2A to 2E are simplified configurauons using the wave adjustment circuits according to die present invention. These simplified configurations should not limit the scope of die claims herein. In an embodiment, these wave adjustment circuits employ substantially equal circuit elements (e.g., inductors, capacitors, transmission line sections, and others) such diat the electneal length of the wave adjustment circuits in senes widi the inducuve applicator coupling power to die plasma is substantially an integral multiple of one wavelengdi. In odier embodiments, die circuit elements provide for inducuve applicators at odier wavelength multiples, e.g., one-sixteenth-wave, one-eighm- wave, quarter-wave, half-wave, ihree-quarter wave, etc. In these embodiments (e.g., full-wave multiple, half-wave, quarter-wave, etc.), the phase and anu-phase relationship between the plasma potentials substantially cancel each odier. In further embodiments, the wave adjustment circuits employ circuit elements d at provide plasma applicators with phase and anti-phase potenuai relauonships d at do not cancel each odier out using a vanety of wave length portions. Fig. 2A is a simplified lllustrauon of an embodiment 50 using wave adjustment circuits according to d e present invenuon. This embodiment 50 includes a discharge rube 52, an inductive applicator 55, an extenor shield 54, an upper wave adjustment circuit 57, a lower wave adjustment circuit 59, an rf power supply 61, and odier elements. The upper wave adjustment circuit 57 is a helicai coil transmission line portion 69, outside of die plasma source region 60. Lower wave adjustment circuit 59 also is a helical coil transmission line portion 67 outside of the plasma source region 60. The power supply 61 is attached 65 to this lower helical coil portion 67, and is grounded 63. Each of die wave adjustment circuits also are shielded 66, 68. In this embodiment, the wave adjustment circuits are adjusted to provide substantially zero AC voltage at one point on die inducuve coil (refer to point 00 in Fig. 2A). This embodiment also provides substantially equal phase 70 and anu-phase 71 voltage distnbuuons in direcuons about this point (refer to 00- A and 00-C in Fig. 2A) and provides substanually equal capacitance coupling to die plasma from physical inductor elements (00-C) and (00-A), carrying die phase and anti-phase potentials. Voltage distributions 00-A and 00-C are combined wid C-D and A-B (shown by die phantom lines) would substanually compnse a full-wave voltage distribution in this embodiment where the desired configuranon is a selected phase/antiphase portion of a full-wave inductor (or helicai resonator) surrounding die plasma source discharge tube. In this embodiment, it is desirable to reduce or minimize capaciuve coupling current from die inducuve element to die plasma discharge in die plasma source. Since the capacitive current increases monoωmcaily with the magmtude of d e difference of peak phase and anti-phase voltages, which occur at points A and C in Fig. 2A, this coupling can be lessened by reducing tins voltage difference. In Fig. 2A, for example, it is achieved by way of two wave adjustment circuits 57, 16 59. Coil 55 (or discharge source) is a helical resonator and the wave adjustment circuits 57, 59 are helical resonators. The discharge source helical resonator 53 can be constructed using convenuonal design formulae. Generally, this helical resonator includes an electrical lengdi which is a selected phase portion "x" (A to 00 to O of a full- wave helical resonator. The helical resonator wave adjustment circuits are each selected to comprise a portion (2τ-x) of full-wave helicai resonators. Physical parameters for die wave adjustment helical resonators can be selected to realize practical physical dimensions and appropriate Q, Z,, etc values. In particular, some or even all of d e transmission line parameters (Q, Z,, etc.) of the wave adjustment circuit sections may be selected to be substantially die same as d e transmission line parameters of die inductive applicator. The portion of die inductive plasma applicator helical resonator, on the other hand, is designed and sized to provide selected uniformity values over substrate dimensions witiiin an economical equipment size and reduced Q. The wave adjustment circuit provides for external rf power coupling, which can be used to control and match power to the plasma source, as compared to conventional techniques used in helical resonators and d e like. In particular, conventional techniques often match to, couple power to, or match to the impedance of the power supply to d e helical resonator by varying a tap position along the coil above die grounded position, or selecting a fixed tap position relative to a grounded coil end and matching to the impedance at this position using a conventional matching network, e.g., LC network, r network, etc. Varying this tap position along the coil within a plasma source is often cumbersome and generally imposes a difficult mechanical design problems. Using die fixed tap and external matching network also is cumbersome and can cause unanticipated changes in die discharge Q, and therefore influences its operating mode and stability. In die present embodiments, die wave adjustment circuits can be positioned outside of the plasma source (or constrained in space containing the inductive coil, e.g., See. Fig. 2A. Accordingly, the mechanical design (e.g., means for varying tap position, change in die effective rf power coupling point by elecincal means, etc.) of d e tap position are simplified relative to ϋiose conventional techniques. In die present embodiment, rf power is fed into die lower wave adjustment circuit 59. Alternatively, rf power can be fed into die upper wave adjustment circuit (not shown). The rf power also can be coupled direcdy into the inductive plasma coupling applicator (e.g. , coil, etc.) in the wave adjustment circuit design, as illustrated by Fig. 2B. Alternatively, odier application will use a single wave adjustment circuit, as illustrated by Fig. 2C. Power can be coupled into this wave adjustment circuit or by conventional techniques such as a tap in the coil phase. In some embodiments, this tap in the coil phase is positioned above the grounded end. An external impedance matching network may dien be operably coupled to d e power for satisfactory power transfer efficiency from, for example, a conventional coaxial cable to impedances (current to voltage rations) existing between the wave adjustment circuit terminated end of the applicator. A further embodiment using multiple inductive plasma applicators also is provided, as shown in Fig. 2D. This embodiment includes multiple plasma applicators (PA1, PA2...PAn). These plasma applicators respectively provide selected combinauons of inductively coupled power and capaciϋvely coupled power from respective voltage potentials (VI, V2...Vn). Each of tiiese plasma applicators derives power from its power source (PS1, PS2...PS ) eidier directly dirough an appropriate matching or coupling network or by coupling to a wave adjustment circuit as described. Alternatively, a single power supply using power splitters and impedance matching networks can be coupled to each (or more d n two) of d e plasma applicators. Alternatively, more tiian one power supply can be used where at least one power supply is shared among more than one plasma applicator. Each power source is coupled to its respective wave adjustment circuits (WAC1, WAC2...WACn). Generally, each plasma applicator has an upper wave adjustment circuit (e.g., WAC la, WAC 2a...WACna) and a lower wave adjustment circuit (e.g., WAClb, WAC 2b...WACnb). The combination of upper and lower wave adjustment circuits are used to adjust die plasma source potential for each plasma source zone. Altemauvely, a single wave adjustment circuit can be used for each plasma applicator. Each wave adjustment circuit can provide substantially the same impedance characteristics, or substantially distinct impedance charactensucs. Of course, d e particular configurauon used will depend upon the application. For instance, multiple plasma applicators can be used to employ distinct excitation frequencies for selected zones in a variety of applications. These applications include film deposition using plasma enhanced chemical deposition, etching by way of ion enhanced etching or chemical dry etching and others. Plasma cleaning also can be performed by way of d e multiple plasma applicators. Specifically, at least one of d e plasma applicators will define a cleaning plasma used for cleaning purposes. In one embodiment, this cleaning plasma can have an oxygen containing species. This cleaning plasma is defined by using an oxygen discharge, which is sustained by microwave power to a cavity or resonant microwave chamber abutting or surrounding a conventional dielectric vessel. Of course, a variety of other processes also can be performed by way of diis multiple plasma applicator embodiment. This present application using multiple plasma applicators can provide a multi-zone (or multi-chamber) plasma source without die use of convenuonal mechanical separation means (e.g., baffles, separate process chambers, etc.). Alternatively, die degree of interaction between adjacent zones or chambers can be relaxed owing to the use of voltage potential control via wave adjustment circuits. This plasma source provides for multiple plasma source chambers, each widi its own control via its own plasma applicator. Accordingly, each plasma applicator provides a physical zone region (i.e., plasma source) with selected plasma characteristics (e.g., capaciuvely coupled current, inductively coupled current, etc.). These zones can be used alone or can be combined with odier zones. Of course, the particular configuration will depend upon the application. In die present embodiments, the wave adjustment circuit can be made from any suitable combination of element(s) such as various types of transmission lines, circuits, etc. These transmission lines include conventional solid or air dielectric coaxial cable, or ordinary, repeating inductor/ capacitor discrete approximauons to transmission iines, and others. These types of transmission iines are co-axial transmission lines, balanced parallel transmission lines, so called slow wave transmission lines widi a spiral inner conductor (e.g., selected portions of a helical resonator, etc.), and others. Individual lumped, fixed, or adjustable combinations of resistors, capacitors, and inductors (e.g. , matching networks, etc.) also can be used in place of transmission line secuons for d e wave adjustment circuit. These general types of wave adjustment circuits are frequency dependent, and can be termed frequency dependent wave adjustment circuits (or FDWACs). Frequency independent elements also can be used as the wave adjustment circuits. These wave adjustment circuits can be termed frequency independent WACs (or FTWACs). Frequency independent wave adjustment circuits include degenerate cases such as short-circuit connections to ground or an infinite impedance (i.e., open circuit), and odiers. Frequency independent wave adjustment circuits can be used alone, or in combination widi the frequency dependent wave adjustment circuits. Alternatively, die frequency dependent wave adjustment circuits can be used alone or in combinauon widi odier wave adjustment circuits. Other variations, alternative construcuons. and modificauons also may be possible depending upon the application. Wirh regard to operation of die wave adjustment circuits, various embodiments can be used, as illustrated by Fig. 2E. The wave adjustment circuits are used to seleα a wave lengtii portion to be applied in the plasma applicator. In some embodiments, d e average rf plasma potential is maintained close to ground potential by providing substantially equal phase 90, 81 and anti-phase 91, 82 capaciuvely coupled portions of the inductive applicator. This can occur in multi- wave embodiments 92, full-wave embodiments 93, half-wave multiple embodiments, quarter-wave multiple embodiments, or any other embodiments 94. In alternative embodiments, it is desirable to maintain an elevated source plasma voltage relative to ground potential to induce a controlled ion plasma flux (or ion bombardment) to the product substrate (or any other chamber bodies). These embodiments are provided by selecting distinct electncal lengths for each of d e wave adjustment circuit sections such diat the capacitive coupled current from a phase section of the inductive plasma applicator is in excess of capacitive coupled current from its anti-phase portion. In these embodiments, the wave adjustment circuit provides a deliberate imbalance between the phase and anti-phase of the coupled voltages. In some embodiments 97, this occurs by shifting d e zero voltage nodes along the process chamber axially, thereby achieving a bias relative to the plasma discharge. As shown, the phase 95 is imbalanced relative to its anu-phase 96. In other embodiments 99, one phase portion 84 is imbalanced by way of a different period relative to its complementary phase portion 85. Odier embodiments are provided where the source plasma voltage is lower relative to ground potential. In die embodiments were imbalance is desirable, die potential difference between die phase and anti-phase potential portions is reduced (or minimized) when the amount of sputtering (e.g., wall sputtering, etc.) is reduced. The amount of sputtering, however, can be increased (or maximized) by increasing the potential difference between die phase and anti¬ phase potential portions. Sputtering is desirable in, for example, sputtering a quartz target, cleaning applications, and others. Of course, the type of operauon used will depend upon die application. Current maxima on an inductive applicator wid distributed capacitance (e.g., helical resonator transmission line, etc.) occur at voltage minima. In particular, conventional quarter-wave helical resonator current is substantially at a relative maximum at its grounded end of the coil, and to a lesser extend in d e nearby coil elements. Therefore, partial inductive coupling of power, if it occurs, will tend to be at this grounded end. In conventional half- wave helical resonators, inductive coupling tends to occur at each of de two grounded ends. In die present invention, substantially anti-symmetric phase and anti¬ phase inductive half-wave and odier fractional wave applicator sections suppon substantially more inductive coupling at a selected rf voltage node, e.g.. Fig. 2A reference numeral 00. This effect is caused by high current flow in die inductor applicator zones (or secuons) both directly above and below die node (conesponding to inductor elements in the phase and anu-phase secuons at and immediately adjacent to the rf voltage zero point). It should be noted dat convenuonal quarter and half-wave inductively coupled inducuve applicators have inducuve coupling which abruptly declines below d e grounded coil locauons because d e coil terminates and voltage extrema are present at these locauons. This generally produces convenuonal quaπer and half-wave helical resonators d at tend to operate in a capaciuve mode, or with a substanual fracuon of power which is capaciuvely coupled to the plasma, uniess d e plasma is shielded from coil voltages, as noted above. In a specific embodiment, die power system includes selected circuit elements for effecuve operauon. The power system includes an rf power source. This rf power source can be any suitable rf generator capable of providing a selected or continuously vanable frequency in a range from about 800 kHz to about 80 MHz. Many generators are useful. Preferably, generators capable of operating into shon and open-circuit loads without damage are used for industnai applicanons. One example of a suitable generator is a fixed frequency rf generator 28.12 MHz - 3 kW CX-3000 power supply made by Comdel. Inc. of Beverly, Massachusetts. A suitable vanable frequency power supply arrangement capable of the 3 kW output over an 800 kHz to 50 MHz range can be made by driving an IFI Model TCCX3500 High Power Wide Band Amplifier with a Hewlett Packard HP116A, 0-50 MHz Pulse/Function Generator. Other generators including those capable of higher or lower power also can be used depending upon the application. Power from die generator can be transmitted to the plasma source by convenuonal coaxial cable transmission line. An example of this transmission line is RG8/U and other higher temperature rated cable (e.g., RGIISIU, etc.) wiώ a coaxial TEFLON" dielectnc. In some embodiments, power is fed to convenuonal end-grounded half-wave helical resonators by positioning a movable tap on the helical coil and connecαng a power source between die tap and d e ground. In other embodiments, matching networks can be introduced between the coaxial cable power feed and die helical coil tap for flexibility. The matching • >"> network will depend on d e selected wave configuration and wave adjustment circuits. In a balanced half-wave helical resonator embodiment, for example, the ends of die resonator coil can be terminated with wave adjustment circuits which substanually have zero susceptance. In particular, die wave adjustment circuit is designed as an open circuit by making no electncal connecuons to the ends of the coil, or establishing an electncal equivalence thereof. Altemauvely, the ends of the coil are isolated by chokes senes resistance, -hereby DC coupled to a fixed reference potenuai. These types of wave adjustment circuits are frequency independent and are "degenerate" cases. In these embodiments, the rf power is provided such diat d e phase and anu-phase current flows above and below die electncal midpoint of die coil. This provides for substanually balanced phase and anti-phase current flow from the power source stabilizing desired operauon in coil voltages above the midpoint of die coil, and also provides substantially equal phase and anu-phase voltages. The embodiments descnbed above also can be applied to other plasma processing applicauons, e.g., PECVD, plasma immersion ion implantauon (PHI), stnpping, sputtering, etc. For instance. Fig. 3 is a simplified CVD apparatus 100 according to die present invenuon. The present CVD apparatus includes a chamber 112, a feed source 114, an exhaust 116, a pedestal 118, a power source 122, a ground 124, a helical resonator 126, and other elements. The helical resonator 126 has a coil 132, an outer shield 133, and odier elements. The chamber can be any suitable chamber capable of housing a product 119 such as a wafer for deposition, and for providing a plasma discharge therein. Preferably, die chamber is a right circular cylinder chamber for providing an uniform plasma species distribution over the product. But the chamber can also be configured in die form of rectangular right cylinder, a truncated cone, and the like. The chamber and fixtures are constructed from aluminum and quaru, and odier suitable matenals. The plasma discharge is derived from a plasma source which is preferably a helical resonator discharge or other inducuve discharge using a wave adjustment circuit or odier techniques to selecuvely adjust phase-anti-phase potentials. The present CVD apparatus provides for deposition of a dielectnc mateπai. e.g., silicon dioxide or the like. The product 119 having an upper surface 130 is placed into the present CVD apparatus for deposiuon, e.g., plasma enhanced chemical vapor deposiuon (PECVD), and odiers. Examples of deposiuon matenals include a dielectnc material such as a silicon dioxide (SiOj), a phosphosilicate glass (PSG), a borophosphosilicate glass (BPSG), a silicon nitπde (Si 3 N 4 ), among others. In one embodiment, d e deposiuon occurs by introducing a mixture compnsing organic silane, oxygen, and an men gas such as helium or argon according to die present invenuon. The organic silane can be any suitable organic silicate matenal such TEOS, HMDS, OMCTS, and die like. Deposiuon is also conformal in selected instances. As for the oxygen, it includes a flow rate of about 1 liter/per minute and less. A relauve flow rate between die organic silane such as TEOS and oxygen ranges from about 1:40 to about 2: 1, and is preferably less than about 1:2 in certain applications. A deposiuon temperature of die organic silane-oxygen layer ranges from about 300 to about 500°C, and can also be at odier temperatures. Pressures in the range of 1 to 7 Torr are generally used. Of course, other concentraπons, temperatures, matenals, and flow rates can be used depending upon die particular applicauon. This chamber also includes a wave adjustment circuit 127. The wave adjustment circuit 127 is used to provide a helical coil operaung with capaciuve coupling to selected phase and anu-phase voltages. This portion 127 of die wave adjustment circuit coil also is shielded 140 to prevent rf from lnterfeπng with the plasma discharge or external elements, e.g., equipment, power, etc. The coil shield 140 is made of a conductive material such as copper, aluminum, or die like. In one embodiment, an operating frequency is selected and the wave adjustment circuit is adjusted to shon circuit die upper end of d e helical applicator coil to ground 124. This provides a helical coil operaung at approximately a full- wave multiple and has substanually equal phase and anu-phase secuons. This full- wave multiple operauon provides for balanced capacitance of phase 151 and anu- phase 153 voltages along die coil 132 adjacent to the plasma source. Full-wave muluple operauon reduces or even substanually eliminates the amount of capaciuvely coupled power from the plasma source to chamber bodies (e.g., pedestal, walls, wafer, etc.) at or close to ground potential. In the present embodiment, die wave adjustment circuit 127 is a variable coil portion 128 of a spiral transmission line, which is selecuvely placed outside the outer shield 133. Accordingly, when the wave adjustment circuit is adjusted to become a shon circuit, die plasma source "sees" only a selected full- wave multiple comprising substanually equal phase 151 and anu-phase 153 of the enure instantaneous AC voltages 134, 135. In this embodiment, stress of die deposited oxide film is often tensile, which can be undesirable. Altemauvely, die wave adjustment circuit 127 provides a helical resonator operating at selected phase and- anti-phase voltages that are not full-wave multiples. This wave adjustment circuit provides for a selected amount of capacitive coupling from die plasma source to die chamber bodies. Stress of die deposited oxide film in this embodiment can be made to be zero or slightly compressive. In some embodiments, die oxide films can be deposed widi an rf plasma potential of several hundred volts between die plasma source and die substrate to decrease the tendency of die oxide film to absorb moisture. This can occur by adjusαng die wave adjustment circuit to add in a small secuon of transmission line outside of die source and correspondingly shortening die applicator coil (by moving die lower point at which the applicator coil is shoπ- circuited and thereby decreasing d e inductance of die applicator coil and electrical length of the helical resonator 126 (e.g., spiral transmission line, etc.) ). Of course, the selected amount of capacitive coupling will depend upon the appiicauon. Fig. 4 is a simplified diagram of a resist stripper according to die present invention. The present snipping apparatus includes similar elements as the previous described CVD apparatus. The present stripping apparatus includes a chamber 112, a feed source 114, an exhaust 116, a pedestal 118, an rf power source 122, a ground 124, a helical resonator 126, and other elements. The helical resonator 126 includes a coil 132, an outer shield 133, a wave adjustment circuit 400, and other elements. The chamber can be any suitable chamber capable of housing a product 119 such as a photoresist coated wafer for stnpping, and for providing a plasma discharge dierein. The plasma discharge is denved from a plasma source, which is preferably a helical resonator discharge or odier inducuve discharge using a wave adjustment circuit or odier techniques to selecuvely adjust phase anu-phase potemials. The present stnpping apparatus provides for stπppmg or ashing photoresist, e.g., implant hardened, etc. Further examples of such a stnpping apparatus are descnbed in the expenments secuon below. In this embodiment, the wave adjustment circuits rely upon open circuits (i.e., zero susceptance). Power transfer can be occurred with a balanced feed such as an lnducuvely-coupled push-pull arrangement such as coupled inductors. Techniques for construcung tiiese coupled inductors are descnbed in. for example, The ARRL Antenna Book," R.D. Straw, Editor, The Ameπcan Radio Delay League, Newmgton, CT (1994) and The Radio Handbook," W.I. Orr, Editor, Engineeπng Ltd, Indiana (1962), which are both hereby incorporated by reference for all purposes. In one embodiment, a femte or powdered iron core "balun" (balanced-unbalanced) toroidal transformer (i.e., broadband transmission transformer, broadband transformer, etc.) 401 can be used to provide balanced matching from a convenuonal unbalanced coaxial transmission line. Techniques for construcung toroidal baluns are descnbed in, for example, Transmission Line Transformers," J. Sevick, 2nd Edition, Ameπcan Radio Relay League, Newmgton. CT (1990). The toroidal transformer is coupled between die rf power source 122 and the coil 132. The midpoint 406 between d e phase 405 and anu- phase voltage on the coil is effecuveiy rf grounded, hence it may be convenient to diiecdy ground this midpoint of die inducuve applicauon in some embodiments for stability. This permits alternate operauon in which power may be coupled into die inducuve applicator (e.g., coil, etc.) with a convenuonal unbalanced feed line tapped on one side of die center. Push-pull balanced coupling ignites the plasma more easily dian convenuonal unbalanced coil tap matching and generally is easier to adjust in selected applicauons. Refemng to the helical resonator embodiments operaung at substantially equal phase and anu-phase potentials. Fig. 5A is a simplified diagram 200 of an equivalent circuit diagram of some of diem. The diagram is merely an illustration and should not limit die scope of the claims herein. The equivalent circuit diagram includes a plurality of rf power supplies (V,, V,, V 3 ...V.) 203, representing for example, a single rf power source. These power supplies are connected in parallel to each odier. One end of the power supply is operably coupled to a ground connection 201. The other end of d e power supplies can be represented as being connected to a respective capacitor (C,. C : , C,...CJ. Each of these capacitors are connected in parallel to each odier. Dunng this mode of operation, substantially no voltage difference exists between any of these capacitors, as they are all connected to each other in parallel. Fig. 5B is a simplified diagram of instantaneous AC voltage and current along a helical resonator coil of Fig. 5A where each end of d e inductive applicator is shon circuited. The diagram is merely an illustration and should not limit the scope of die claims herein. This diagram includes die discharge tube 213 and an inductive plasma discharge (or plasma source) 501 dierein. As shown, d e plasma discharge includes an intensified "donut- shaped" glow region 501 diat occupies a limited range (R) of the discharge tube 213. The plasma discharge has an average voltage potential (V.- of substantially zero volt between d e ground potential (VJ and die high voltage potential (Vg). As can be seen, the plasma discharge 501 has capaciuvely coupling elements to V H and V α . But die average voltage potential of this plasma discharge is zero. This operation provides for balanced capacitance of phase 503 and anti-phase 505 voltages along the coil adjacent to the plasma, u ereby substantially preventing capaciuvely coupling from die plasma source to chamber bodies. As also shown, a current maxima 507 exists at V m , which corresponds to an inflection point between the phase 503 and die anti-phase 505. In an alternative operating mode, dim nngs of plasma caused by inductively coupled plasma current are visible near top and bottom extremes of the inductive applicauon, as illustrated by Fig. 5C. This operating mode is generally for a full-wave 517 inductive coupling coil operated at a very high power, e.g. , maximum power input to die inducuve applicator is often limited by thermal considerauons and breakdown. The rings 513, 515 of current in the plasma discharge are simulated by maximum coil current areas corresponding to voltage minima at the top and bottom shorted ends of d e coil. Under these high power conditions, subordinate current rings are detectable and some excitation is often visible in die intermediate regions. This excitation is partially caused by capaciϋvely driven currents widiin the discharge coupled to die voltage maximum and voltage minimum positions along the inducuve applicator. Alte auvely, subordinate inductive plasma current rings at the top and bottom ends 513 of the resonator do not appear with limited input power. The coil current and inductive flux fall beyond the ends of the inductive applicator so diat a single inductive ring 5 IS in the center portion is more stable, provided that die conductivity of the plasma is large enough to suppon a single current ring at a specified input power. In alternative applications using high power operation, no secondary plasma current rings may be desirable. These applications often have substantially minimum internal capacitive coupling. In diese applications, die inducuve applicator (e.g., coil) abutting the vacuum vessel may be shortened from a full wave to an appropriate length such d at only die central current maxima exists on die coil abutting d e plasma source and die potential difference between maximum and minimum voltage on the applicator is substantially reduced. The present application is achieved by stabilizing die desired waveform along the applicator by appropriate impedance wave adjustment circuits. Referring to die above embodiments, the present invention provides for processing with an inductively coupled plasma in which die plasma potential from coupling to a phase portion of d e inductive applicator is substanually not offset by capacitive coupling to anti-phase voltages on selective portions to the inductive coupling element. Conventional inductive sources (e.g., conventional helical resonators, etc.), however, have hidierto been operated in quarter-wave or half-wave modes. These modes provide only phase capacitive coupling to the plasma, which raises die plasma potential toward die coil without compensation anu-phase coupling. Convenuonal inductive sources diat are longer than a half- wave have been generally considered cumbersome and impractical for plasma reactors. In paπicular, these inducuve sources are large in size, and have nodes along d e helical coil, which have been believed to create a non-uniform plasma. In order to operate a substanually inducuve plasma in a helical resonator, convenuonal inducuve sources relied upon shielding the plasma tube from electncal fields onginaung on d e coil. Shielding occurred, for example, by inserting a longitudinally split shield between die coil and plasma tube. The present invenuon provides for a substanually pure inducuve ly coupled power source. A benefit of this inducuveiy coupled power as a primary means to sustain plasma excitauon is that electnc field Iines produced by inducuve coupling are solenoidal (e.g. they close on themselves). Since soienoidal electnc field lines have zero divergence, they do not create or suppon a scalar potential field (e.g. a voltage difference) within die plasma volume. Thus, in an ideal case, inductively coupled power can be transfeπed into a plasma widiout no direct relationship between die plasma potential and die voltages on coupling elements (e.g. the voltage on the coil in a helical resonator) or voltages on rf matching networks, if such are used. Furthermore, when transferring power to die plasma by purely inducuve means, power transfer does not require any significant potential difference to be maintained between elements of the plasma and ground potential (e.g. die potential difference between die plasma and ground can be fixed by factors which are substantially independent of inductive excitation power). Although in theory, inductive power transfer does not require raising die AC or DC potential of die plasma widi respect to ground, in practice there has been substantial shift and harmful alterauon in the plasma potential found in unshielded current an inducuve sources. As previously noted, and furdier emphasized herein, die most effecuve conventional method employed to avoid plasma potential shift in conventional commercially available inducuve sources is to shield die plasma from the electncal fields on the inductive coupling element (commonly a multi-turn coil) by inserung a grounded conducuve member between the inducuve driving element and the plasma discharge tube. Shielding is, however, cumbersome and inconvement and has serious disadvantages in pracuce. Shields couple to inducuve applicator elements and can cause wide excursions in d e natural resonance frequency, which are not predicted by convenuonal design formulae. This often results in labonous trail and error and iterative mechanical designs to achieve a desired resonance. Another disadvantage of shielding is that shields often make it difficult to achieve initial ignition of the plasma since shields generally exclude capacitive electnc fields in d e plasma discharge tube. In parucular, ignition (known as plasma breakdown) of inducuve breakdown generally begins with a capacitive electnc field discharge, which is stable at lower currents and powers (See, for example, J. A orim, H.S. Maciel and J.P. Sudana, J. Vac. Sci. Technol. B9, pp. 362-365, 1991). Accordingly, shields tend to block capacitive electnc fields, which induce plasma ignition. Insertion of die shield close to high voltage RF point in a network (such as the voltage maximum points in a helical resonator or the high potential driven side of a TCP coil) also causes large displacement currents to flow through the capacitance between the shield and coil. This high potential difference is also a potential cause of damaging rf breakdown across die air gap, hence d e gap may require protection by inconvenient solid or liquid dielectnc insulation. The displacement current flow causes power loss and requires that higher power RF generating equipment be used to compensate for the power loss. Coupling loss in the plasma source structure is also undesirable from die standpoint of thermal control. These limitations are overcome by d e present invention using die wave adjustment circuits, an inductive applicator of selected phase length, and odier elements. Experiment To prove die principle and demonstrate die operation of d e present invention, a helical resonator plasma source was used in a photoresist stripper. Convenuonal helical resonators also were evaluated in these experiments. These experiments are merely examples, and should not limit die scope of die claims herein. One of ordinary skill in the an would easily recognize other expenments. uses, vaπations, and modificauons of the invenuons defined by these claims. I. Conventional Photoresist Stπooer In this experiment, d e conventional resist stnpper was a prototype made by MC Electronics, present assignee. Of course, other stnpper platforms also can be used depending upon die applicauon. A convenuonal quarter-wave helical resonator resist stnpper 600 was constructed widi a quarter-wave helical resonator source 602 upstream of a processing chamber 604, shown in Fig. 6. This quarter-wave helicai resonator 602 included a coil 608 and odier elements. Coil 608 consisted of 5. IS turns of 0.4 inch diameter copper tubing would with a pitch of 0.5 turns per inch with a mean radius of 6.4 inches and centered radially and vertically inside an outer copper shield 610. Coil 608 is operably coupled to a power source 612 and operated at about 13 MHz radio frequency. A 17 inch long, 9.25 inch diameter quaru tube 606 was centered inside of die copper coil 608. The shield 610 was 16 inches inside diameter, approximately 0.08 inches duck and 18 inches long. This shield 610 also was connected to a ground (V 0 ) connecuon on die aluminum process chamber body (except when making die current measurements descnbed below). The process chamber 604 was for a convenuonal resist stnpper. This resist stnpper included a wafer suppon 616 (or pedestal) and other elements. Process chamber 604 is operably coupled at an outer locauon 620 to ground via shield 610. Wafer suppon 616 has a wafer 618 disposed thereon. The wafer 618 is a 6-inch (250mm) < 100> type wafer widi approximately 1.25 microns of spin-coated Mitsubishi Kasei positive photoresist MPR-4000. This wafer was ashed on die grounded 10 inch diameter wafer suppon 616. This suppon was resistivity heated and die temperature of the substrate suppon was sensed with a thermocouple. After the helical resonator plasma was ignited, visible plasma filled die quaru plasma tube under all of the conditions used for processing. In addition, a strong plasma glow was always visible above die wafer tn die downstream processing chamber which was indicauve of secondary plasma discharge to the substrate suppon. This secondary plasma discharge was also accompanied by current flow from the resonator shield to the chamber of approximately 5-10 Amperes r s (and sometimes even more) which could be measured by elevating die shield on insulating blocks and monitoring d e current flow through a 2 inch long 1.5 inch wide strip of copper braid which was passed through a Pearson Current probe used to monitor the current. Fig. 7 is a simplified diagram 700 of the rf voltage distribution along die coil for die quarter-wave helical resonator of Fig. 6. This diagram includes the quaru tube 606 and a plasma discharge (or source) 701 dierein. As shown, the plasma discharge includes a glow region diat 701 occupies a large range (R) of the quaru tube 606. The plasma discharge has an average voltage potential (VJ between the ground potential (V,,) and the high voltage potential (VR). As can be seen, die plasma discharge 701 has capaciuvely coupling elements to V„ and V 0 due to its average voltage potential V m . In fact, as previously noted, d e current fiow from die resonator shield to die chamber was at least 5-10 Amperes rms. In high power applications, intense sparking was observed in the chamber from the capaciuvely coupled plasma source. II. Present Photoresist StriDPer To prove the principle and operation of die present inventions, experiments were performed. These experiments used a photoresist stripper apparatus. This resist stripper apparatus in a cluster tool arrangement used a helical resonator according to the present inventions. One of ordinary skill in the an, however, would recognize that odier implementations, modifications, and variations may be used. Accordingly, die experiments performed herein are not intended to limit the scope of the claims below. The photoresist stripper apparatus was configured widi multiple process chambers in a cluster tool arrangement, as illustrated by Figs. 8 and 9. Figs. 8 and 9 illustrate a simplified top-view diagram 800 and a simplified side- view diagram, respectively. Two process chambers, e.g., chamber 1 901 and chamber 2 903, were used. Chamber 1 901 was used for stnpping implant hardened resist crust (or skin). Chamber 2 903 was used for stnpping the remaining photoresist. Altemauvely, the chambers can be both used for stnpping implant hardened resist crust and stripping remaining photoresist. Of course, the particular use depends upon the application. These chambers also were made of aluminum widi ceramic inserts, which is highly resistant to chemical attack. The apparatus also used a microprocessor based controller to oversee process operauons. This microprocessor based controller can be accessed through a control panel 921. The present apparatus used a controller made from a 486DX processor PC made by EPSON, widi a color LCD touch panel display. This controller also is shielded and highly resistant to chemical attack. An automatic wafer handling system 910 was also provided. The automatic wafer handling system used standard cassettes 912 for transferring die photoresist coated wafers to and from the process chambers 901 , 903. The automatic wafer handling system included a robot 917, cassette chamber 1 905, cassette chamber 2 907, cassette stage 1 909, cassette stage 2 911 , and odier elements. The wafer handling system 910 used a conventional interlock system for providing die cassettes 912 from the cieanroom into the process chambers 901. 903. A main shuttle chamber 913 housed d e robot 917 in the cluster tool arrangement. The controller oversees die automatic wafer handling system operations. The present wafer handing system is made by JEL Co., LTD of Japan. A cooling plate 915 was included in the main chamber 913 housing die robot 917. The cooling plate 915 was of conventional design, and was capable of cooling the wafer after being stripped, which often occurs at elevated temperatures. Alternatively, the cooling plate can be used to thermally adjust die wafer temperature either before, after, or even between selected process operations. The process chambers 901, 903 were disposed downstream from respective plasma sources 923, 925. Each helical resonator included a coil 927 disposed around a quaru tube 929. The coil consisted of 11.5 turns of 0.4 inch copper tubing wound widi a pitch of 0.9 turns per inch with a mean radius of 9.4 inches and centered radially and vertically inside an outer copper shield 9 1. The coil is operably coupled to a power source (not shown). A 17 inch long, 9.25 inch diameter quaru rube was centered inside of the copper coil. The shield was 16 inches inside diameter, approximately 0.08 inches thick and 18 inches long. The shield is operably coupled to a lower portion of the coil. In one experiment, processes were used for stripping photoresist from wafers, e.g., See. Fig. 9 reference numeral 933. The processes involved the use of a multi-step stripping operauon to remove implanted photoresist from semiconductor wafers. Samples were prepared using eight-inch wafers. These wafers were spin coated widi Mitsubishi Kasei positive photoresist MPR-4000. Spin coating occurred at 1,200 rpm and 120 β C for 90 seconds. The resulting photoresist was about 1.2 microns in thickness in die sample wafers. These sample wafers were implanted to form a implanted hardened resist layer near the top of the photoresist. An implant resist stripping process was performed to remove the top implant hardened resist. This occurred by stripping using an "un-balanced" phase and anti-phase coupling relationship in a half-wave helical resonator. The half- wave helical resonator was configured in one of the process chambers. In this chamber, the pedestal had a temperature of about 40 °C to maintain a low wafer temperature. This low wafer temperature was maintained to reduce the possibility of "popping." Popping occurs when vapor in the underlying photoresist explodes through die implant hardened resist. After the top hardened layer was removed. The wafer was transferred into a chamber operating at a full-wave multiple. This chamber operated at a frequency of about 27.12 MHz at a full-wave multiple. The pedestal of this chamber was at 150 to 200 β C. The full wave structure provided for balanced phase and anti-phase coupled currents, diereby reducing the amount of capaciuvely coupled plasma, which can be detrimental to d e underlying substrate. In this step, overashing was performed to substantially remove all photoresist material from the wafer. No damage occurred to the underlying substrate during this overashing step. Once the photoresist has been stnpped. the wafer is cooled. In parucular, the wafer is removed from the full-wave muluple process chamber, and placed on the cooling stauon. This cooling station reduces the temperature of the wafer (which was heated). This wafer is then reloaded back into us wafer cassette. Once all wafers have been processed in die cassette, the cassette compπsing die stnpped wafers is removed from d e cluster tool apparatus. Charactensucs of this half-wave helical resonator were descnbed in detail above. In the present expenments, the following tests also were performed. Test 1: 6-inch wafers were ashed at a total pressure of 0.13 Ton using a gas flow of 0.2 standard liter per minute of pure oxygen, forward rf power of 2200 watts and a reflected power of 150 warts at an excitation frequency of 13.4 Mhz. The substrate was held at 60 °C and wafers were ashed and then the discharge was extinguished). The ashing rate across the wafer was determined to vary between approximately 3411 A/min and 3139 A min with the rates approximately symmetric about the center of each wafer and die maximum ashing rate at the center. The average etching rate was 3228 A/min and etching uniformity was approximately 4 percent. Test 2: 6-inch wafers were ashed at a total pressure of 1 Ton using a gas flow of 1 standard liter per minute, forward rf power of 2200 watts and a reflected power of 160 watts at an excitation frequency of 13.0 MHz. The substrate was held at 60 β C and the ashing rate was determined to very between approximately 3144 A/min and 3748 A/min depending on position on a wafer. The etching uniformity was approximately 9 percent. Test 3: Resist coated wafers were implanted wid a selected dose of S x 10" atoms/cm 2 at 40 kev arsenic (As). The wafers were cleaved into samples approximately 3 cenumeters square. Two samples were d en ashed on die substrate suppon simultaneously, under the vanous conditions listed in Table 1. TABLE 1: Expenmental Results for Ashing (I) Unimplanted resist was used in this test and ashing was terminated before endpoint was reached to test uniformity. The average ashing rate was S259 A min and uniformity was 7.5%. (II) Implanted resist was etched for 150 sec, but endpoint was visible at 100 seconds. Under conditions used for Run D. it was determined diat resist was cleared from the entire wafer after 3 minute and 15 seconds. Consequentiy, the ashing time in de table included approximately 100 sec. overetching. Under conditions where practical ashing rates were attained, a visible plasma discharge and sheatii could be observed over die wafer. Diagnostic measurements of current similar to those performed in die conventional stripping apparatus were performed. In these measurements, currents from the shield of die resonator to d e processing chamber gave values of at about 0.1 to 0.S Amperes rms and less. These measurements were limited by error using available instrumentation. Accordingly, these currents were at least an order of magnitude below those currents measured above in die conventional stripping apparatus. A visual inspection of the stnpped wafers shows extremely good results. That is, the wafers were stnpped at a sufficient rate for production operauon and no substanual damaged occuπed to the wafers. This provides for effective wafer turn-arouπd-time and substantially no damage caused by die plasma. In addition, current measured from die shield to die chamber by elevaung he shield on insulating blocks was less than about 0.5 Amperes rms and. in some instances, at or below measured error using available instrumentation. This current was substantially less than those measured in die conventional stripping apparatus. While the invenuon has been described with reference to specific embodiments, various alternatives, modifications, and equivalents may be used. In fact, the invention also can be applied to almost any type of plasma discharge apparatus. This discharge apparatus can include an apparatus for plasma immersion ion implantation or growing diamonds, TCPs. and others. This discharge apparatus can be used for d e manufacture of fiat panel displays, disks, integrated circuits, diamonds, semiconductor materials, bearings, raw materials, and the like. Therefore, die above description should not be taken as limiting the scope of die invention which is defined by the appended claims.

Claims: WHAT IS CLAIMED IS: 1. A process for fabncaung a product, said process compπsing die steps of subjecting a substrate to entiues, at least one of said enuties emanaung from a species generated by a gaseous discharge excited by a high frequency field in which die vector sum of phase portion and anu-phase ponton of capaciuve current coupled from die inducuve coupling structure balances. 2. The process of claim 1 wherein said product compnses a semiconductor device. 3. The process of claim 1 wherein said gaseous discharge is provided by a helical resonator. 4. The process of claim 1 wherein said gaseous discharge is provided by a helical resonator having an electncal length which is substanually a whole number multiple of one wavelengtii. 5. The process of claim 1 wherein said gaseous discharge is provided by a helical resonator structure, said helical resonator structure having an electncal length which is substanually free from any muluple of one quarter wavelengtii. 6. The process of claim 1 wherein said one of said enuties is provided in chemical vapor deposition. 7. The process of claim 1 wherein said one of said eπαoes is provided in plasma etching. 8. The process of claim 1 wherein said inducuve coupling structure is selecuvely balanced using a wave adjustment circuit. 9. A process for fabncaung a product comprising the steps of subjecung a substrate to a composition of entities and employing the resulting substrate for completion of said product, at least one of said enuties emanaung from a species generated by a gaseous discharge provided by a helical resonator. said helical resonator having an integral current driven by capacitive coupling of plasma column to elements with a selected potential greater than a surrounding shield potential is substantially equal to capacitive coupling of the plasma column to substantially equal elements with a potential below shield potential. 10. The process of claim 9 wherein said helicai resonator is characterized in that the capacitive current flow from the surrounding coil into the plasma column is substantially equal to die capacitive current from die plasma column to the surrounding coil. 11. The process of claim 9 wherein said helical resonator is in which the average potential of the plasma column is substantially equal to that of die shield. 12. Apparatus for fabricating a product, said apparatus comprising: an enclosure comprising an outer surface and an inner surface, said enclosure housing a gaseous discharge; a plasma applicator disposed adjacent to said outer surface; a high frequency power source operably coupled to said plasma applicator, said high frequency power source exciting said gaseous discharge to provide at least one entity from a high frequency field in which die vector sum of phase and anti-phase capacitive current coupled from die inductive coupling structure substantially balances. 13. Apparatus of claim 12 wherein said enclosure is a chamber. 14. Apparatus of claim 12 wherein said enclosure is a rube. 15. Apparatus of claim 14 wherein said rube is made of a matenal selected from quaπz, glass, diamond, polymer, sapphire, and alumina. 16. Apparatus of claim 12 wherein said apparatus further compπses a wave adjustment circuit, said wave adjustment circuit operably coupled to said plasma applicator to selectively provide balancing of said inducuve coupling strucmre. 17. Apparatus of claim 12 wherein apparatus is provided for chemical vapor deposition. 18. Apparatus of claim 12 wherein apparatus is provided for plasma etching. 19. Apparatus of claim 12 wherein said enclosure, said plasma applicator, and said high frequency power source define a helical resonator structure, said helical resonator structure having an electrical length which is substantially a whole number multiple of one wavelength. 20. Apparatus of claim 12 wherein said enclosure, said plasma applicator, and said high frequency power source define a helical resonator structure, said helical resonator structure having an electrical lengdi which is substantially free from any multiple of one quarter wavelengtii. AMENDED CLAIMS [received by the International Bureau on 30 April 1997 (30.04.97); original claims 1-20 replaced by amended claims 1-18 (2 pages)] 1. A process for fabricating a product comprising the steps of subjecting a substrate to entities, at least one of which emanates from a species generated by a gaseous discharge excited by a high frequency field, in which phase and anti-phase capacitive currents, coupled to the gaseous discharge from an inductive coupling structure, are substantially balanced. 2. The process of claim 1 wherein the product comprises a semiconductor device. 3. The process of claim 1 wherein the high frequency field is provided by a helical resonator. 4. The process of claim 3 wherein the helical resonator has an electrical length which is substantially an integer number of wavelengths . 5. The process of claim 1 wherein one of the entities is for chemical vapor deposition. 6. The process of claim 1 wherein one of the entities is for plasma etching. 7. The process of claim 1 wherein the inductive coupling structure is selectively balanced using external circuitry. 8. A process for fabricating a product comprising the steps of subjecting a substrate to a composition of entities and employing the resulting substrate for completion of the product, at least one of the entities emanating from a species generated by a gaseous discharge provided by a helical resonator having a coil, the integral of the current driven by the capacitive coupling of plasma to elements of the coil which have a potential greater than a surrounding shield potential being substantially equal to the integral of the current driven by the capacitive coupling of the plasma to other elements of the coil which have a potential below the surrounding shield potential. 9. The process of claim 8 wherein capacitive current flow from the coil into the plasma is substantially equal to capacitive current flow from the plasma into the coil . 10 The process of claim 8 wnerein the plasma nas an average potential substantially equal to that of the shield. 11. Apparatus for fabricating a product comprising - an enclosure comprising an outer surface and an inner surface and housing a gaseous discnarge, an inductive coupling structure; a h gh frequency power source operably coupled to the inductive coupling structure for exciting the gaseous discharge to provide at least one entity from a high frequency field m which the phase and antl-phase currents coupled from the inductive coupling structure are substantially balanced. 12. The apparatus of claim 11 wherein the enclosure is a chamber. 13. The apparatus of claim 11 wherein the enclosure 1 . The apparatus of claim 13 wherein the tube is made of a material selected from quartz, glass, diamond, polymer, sapphire and alumina. 15. The apparatus of claim 11 further comprising matching circuitry operably coupled to the inductive coupling structure to selectively balance the inductive coupling structure . 16. The apparatus of claim 11 adapted for chemical vapor deposition. 17. The apparatus of claim 11 adapted for plasma etching. 18. The apparatus of claim 11 wherein the enclosure, the inductive coupling structure and the high frequency power source define a helical resonator structure having an electrical length which is substantially an integer number of wavelengths .

Inventors: VINOGRADOV GEORGY, YONEYAMA SHIMAO, VINOGRADOV, GEORGY, YONEYAMA, SHIMAO
Applicants: MC ELECTRONICS CO LTD, MC ELECTRONICS CO., LTD.
Application year: 1996
Main classification: H05H1
IPC codes: C23C16, H01J37, H01L21, H05H1