Abstract:
A method in a plasma processing system for etching a feature through a dielectric layer of a dual damascene stack on a semiconductor substrate is disclosed. The method includes placing the substrate in a plasma processing chamber of the plasma processing system. The method further includes flowing an etchant gas mixture into the plasma processing chamber, the etchant gas mixture being configured to etch the dielectric layer. The method additionally includes striking a plasma from the etchant source gas. The method also includes etching the feature through the dielectric layer while applying a bias RF signal to the substrate, the bias RF signal having a bias RF frequency of between about 27 MHz and about 90 MHz. The bias RF signal further has a bias RF power component that is configured to cause the feature to be etched in accordance to predefined etch rate parameters and etch profile parameters at the bias RF frequency.

Description:
BACKGROUND OF THE INVENTION  
       [0001]     The present invention relates in general to substrate manufacturing technologies and in particular to methods and apparatus for the optimization of ion energy control in a plasma processing system.  
         [0002]     In the processing of a substrate, e.g., a semiconductor wafer or a glass panel such as one used in flat panel display manufacturing, plasma is often employed. As part of the processing of a substrate (chemical vapor deposition, plasma enhanced chemical vapor deposition, physical vapor deposition, etc.) for example, the substrate is divided into a plurality of dies, or rectangular areas, each of which will become an integrated circuit. The substrate is then processed in a series of steps in which materials are selectively removed (etching) and deposited (deposition) in order to form electrical components thereon.  
         [0003]     Integrated circuits are sequentially created by forming conductive patterns on dielectric layers on a substrate. In an exemplary plasma process, a substrate is coated with a thin film of hardened emulsion (i.e., such as a photoresist mask) prior to etching. Areas of the hardened emulsion are then selectively removed, causing parts of the underlying layer to become exposed. The substrate is then placed in a plasma processing chamber on a substrate support structure comprising a mono-polar or bi-polar electrode, called a chuck. Appropriate etchant source gases (e.g., C 4 F 8 , C 4 F 6 , CHF 3 , CH 2 F 3 , CF 4 , CH 3 F, C 2 F 4 , N 2 , O 2 , Ar, Xe, He, H 2 , Nh 3 , SF 6 , BCl 3 , Cl 2 , etc.) are then flowed into the chamber and struck by a set of RF frequencies to form a plasma to etch exposed areas of the substrate. By controlling the amount of ion energy in the plasma through adjustments in a set of RF frequencies, the etch process is optimized.  
         [0004]     In a common substrate manufacturing method, known as dual damascene, dielectric layers are electrically connected by a conductive plug filling a via hole. Generally, an opening is formed in a dielectric layer, which is then filled with a conductive material (e.g., aluminum (Al), copper (Cu), etc.) that allows electrical contact between two sets of conductive patterns. This establishes electrical contact between two active regions on the substrate, such as a source/drain region. Excess conductive material on the surface of the dielectric layer is typically removed by chemical mechanical polishing (CMP).  
         [0005]     There are generally two approaches manufacture dual damascene substrates: Via-First and Trench-First. In one example of the Via-First methodology, the substrate is first coated with photoresist and then the vias are lithographically patterned. Next, an anisotropic etch cuts through the surface cap material and etches down through the low K layer of the substrate, and stops on a silicon nitride barrier, just above the underlying metal layer. Next, the via photoresist layer is stripped, and the trench photoresist is applied and lithographically patterned. Some of the photoresist will remain in the bottom of the via and prevent the lower portion via from being over-etched during the trench etch process. A second anisotropic etch then cuts through the surface cap material and etches the low K material down to a desired depth. This etch forms the trench. The photoresist is then stripped and the Silicon Nitride barrier at the bottom of the via is opened with a very soft, low-energy etch that will not cause the underlying copper to sputter into the via. As described above, the trench and via are filled with a conductive material (e.g., aluminum (Al), Copper (Cu), etc.) and polished by chemical mechanical polishing (CMP). And although the via-first approach has been widely adopted for small geometry devices because it avoids the photoresist pooling effect that occurs when the trenches are formed before the vias, it is also prone to photoresist poisoning.  
         [0006]     An alternate methodology is trench-first. In one example, the substrate is coated with photoresist and a trench lithographic pattern is applied. An anisotropic dry etch then cuts through the surface hard mask (again typically SiN, TiN or TaN) followed by stripping the photoresist. Another photoresist is applied over the trench hard mask and then the vias are lithographically patterned. A second anisotropic etch then cuts through cap layer and partially etches down into the low K material. This etch forms the partial vias. The photoresist is then stripped for trench etch over the vias with the hard mask. The trench etch then cuts through the cap layer and partially etches the low K material down to desired depth. This etch also clears via holes at the same time stopping on the final barrier located at the bottom of the via. The bottom barrier is then opened with a special etch. And unlike the via-first methodology, photoresist poisoning may be substantially less.  
         [0007]     However, escalating requirements for high circuit density on substrates may be difficult to satisfy using current plasma processing technologies where sub-micron via contacts and trenches have high aspect ratios. The utilization of new low-k films and complex film stacks present a new set of challenges for dielectric etch processes and equipment.  
         [0008]     To facilitate discussion,  FIG. 1A  illustrates an idealized cross-sectional view of a layer stack  100 , representing the layers of an exemplar semiconductor IC, prior to a lithographic step. In the discussions that follow, terms such as “above” and “below,” which may be employed herein to discuss the spatial relationship among the layers, may, but need not always, denote a direct contact between the layers involved. It should be noted that other additional layers above, below, or between the layers shown may be present. Further, not all of the shown layers need necessarily be present and some or all may be substituted by other different layers.  
         [0009]     At the bottom of layer stack  100 , there is shown a layer  108 , comprising SiO 2 . Above layer  108  is disposed a barrier layer  104 , typically comprising nitride or carbide (SiN or SiC). Dual damascene substrates further comprise a set of metal layers including M 1   109   a - b , typically comprising aluminum or copper. Above the barrier layer  104 , is disposed a intermediate dielectric (IMD) layer  106 , comprising a low K material (e.g., SiOC, etc.). Above the IMD layer  106 , there may be placed a cap layer  103 , typically comprising SiO 2 . Above cap layer  103 , there may be disposed a trench mask layer  102 , typically comprising TiN, SiN, or TaN.  
         [0010]      FIG. 1B  shows a somewhat idealized cross-sectional view of layer stack  100  of  FIG. 1A , after photoresist layer  110  and a BARC layer  112  is further added.  FIG. 1C  shows a somewhat idealized cross-sectional view of layer stack  100  of  FIG. 1B  after photoresist layer  110  and BARC layer  112  have been processed through lithography. In this example, a photoresist mask pattern is created with a set of trenches  114   a - b.    
         [0011]      FIG. 1D  shows the cross-sectional view of layer stack  100  of  FIG. 1C  after trench mask layer  101  has been processed in the plasma system, further extending trench  114   a - b  to cap layer  103 .  FIG. 1E  shows the cross-sectional view of layer stack  100  of  FIG. 1D , after photoresist layer  110  and a BARC layer  112  are removed.  
         [0012]      FIG. 1F  shows the cross-sectional view of layer stack  100  of  FIG. 1E  after a second photoresist layer  116  and a BARC layer  118  are disposed, in order to create a second metal layer and a via connecting it to the first metal layer  109   a - b .  FIG. 1G  shows the cross-sectional view of layer stack  100  of  FIG. 1F  after the photoresist layer has been opened and an etch has been performed to partially etch into IMD layer  106  to create a via.  FIG. 1H  shows the cross-sectional view of layer stack  100  of  FIG. 1G  after photoresist layer  110  and BARC layer  112  have been stripped, and an additional etch process has been performed to extend the trench to a desired depth and etch through a via stopping on barrier layer  104 . In  FIG. 1I , the barrier layer  104  is etched through using, for example CH 2 F 2 , CH 3 F, etc. In  FIG. 1J , a chemical mechanical polish process has been performed to polish layer stack  100  down to cap layer  103 , and a conductive material (e.g., aluminum (Al), Copper (Cu), etc.) has been deposited to contact the existing M 1  metal material.  
         [0013]     In a typical plasma processing system, a first RF energy source may be employed to create a cloud of ions for the processing a substrate. Generally speaking, this first RF energy source may be said to be generating a source RF signal for dissociating the ions. In addition, there is another RF energy source for creating a bias with the plasma, and directing the plasma away from structures within the plasma processing system and toward the substrate. Generally speaking, this second RF energy source may be said to be generating a bias RF signal for controlling the ion energy.  
         [0014]     For example, a dual frequency triode configuration may have a source RF generator at the top of the chamber, and a bias RF generator coupled to provide the bias RF signal to the substrate. Referring now to  FIG. 2A , a simplified diagram of a dual frequency triode plasma processing system  200  is shown. A typical arrangement is to employ a substantially high frequency source RF generator  202  (e.g., 27 MHz, 60 MHz, or 100 MHz) to provide a corresponding source RF signal an upper electrode, and a substantially lower frequency bias RF generator  204  (e.g., 8 KHz, 2 MHz, or 3 MHz) to provide a corresponding bias RF signal to the lower electrode, which is coupled to a substrate.  
         [0015]     A dual frequency diode configuration may have both the source and bias RF generators coupled to provide both source and bias RF signals to the substrate. Referring now to  FIG. 2B , a simplified diagram of a dual frequency diode plasma processing system  250  is shown. A plasma  206  forms above the substrate, and is accelerated down into the substrate to physically bombard and etch silicon or other materials from the substrate by an electric field formed between the plasma and the negatively charged wafer. A typical arrangement is to provide both a substantially high frequency source RF generator  252  (e.g., 27 MHz, 60 MHz, or 100 MHz) and a substantially lower frequency bias RF generator  254  (e.g., 8 KHz, 2 MHz, or 3 MHz) to provide both the source RF signal and the bias RF signal to the lower electrode, which is coupled to a substrate.  
         [0016]     Single frequency diode configuration may have a single bias RF sources coupled to provide the bias RF signal to the substrate. Referring now to  FIG. 2C , a simplified diagram of a single frequency diode plasma processing system  270  is shown. A plasma  206  forms above the substrate, and is accelerated down into the substrate to physically bombard and etch silicon or other materials from the substrate by an electric field formed between the plasma and the negatively charged wafer. A typical arrangement is to provide a single frequency bias RF generator  252  (e.g., 13.56 MHz,) to provide a bias RF signal to the lower electrode, which is coupled to a substrate.  
         [0017]     While not wishing to be bound by theory, fast moving electrons in the plasma generally tend to be absorbed by walls or other boundaries. In order to maintain a charge balance in the plasma, a thin positive ion sheath may be formed near each wall or boundary such as those proximate the substrate. This creates an electric field which tends to accelerate ions in the plasma into the wall or boundary with a substantial amount of energy. If the plasma is not properly optimized, faceting or corner sputtering (or erosion) occurs on the substrate surface. A facet is the result of a non-linear profile in the substrate, such as in a trench sidewall. A corner sputtering is a result of an undesirable removal of additional material, particularly of the material at the upper corners of the feature to be etched.  
         [0018]     Accurate control of faceting and unwanted corner sputtering becomes critical in dual damascene etches, particularly in copper dual damascene etches in which no plugs or multiple hard masks are employed (e.g., in a trench-first dual damascene dielectric etch). Up to now, no attempts have been made to employ RF configuration, particularly RF configuration of the bias RF generator, to minimize faceting and unwanted corner sputtering, maximizing the process window, and obtaining the desired vertical etch profile.  
       SUMMARY OF THE INVENTION  
       [0019]     The invention relates, in one embodiment, to a method in a plasma processing system for etching a feature through a dielectric layer of a dual damascene stack on a semiconductor substrate. The method includes placing the substrate in a plasma processing chamber of the plasma processing system. The method further includes flowing an etchant gas mixture into the plasma processing chamber, the etchant gas mixture being configured to etch the dielectric layer. The method additionally includes striking a plasma from the etchant source gas. The method also includes etching the feature through the dielectric layer while applying a bias RF signal to the substrate, the bias RF signal having a bias RF frequency of between about 27 MHz and about 90 MHz. The bias RF signal further has a bias RF power component that is configured to cause the feature to be etched in accordance to predefined etch rate parameters and etch profile parameters at the bias RF frequency.  
         [0020]     In yet another embodiment, the invention relates to a method in a plasma processing system for etching a feature through a dielectric layer of a dual damascene stack on a semiconductor substrate. The method includes placing the substrate in a plasma processing chamber of the plasma processing system. The method further includes flowing an etchant gas mixture into the plasma processing chamber, the etchant gas mixture being configured to etch the dielectric layer. The method additionally includes striking a plasma from the etchant source gas. There is also included etching the feature through the dielectric layer while applying a bias RF signal to the substrate, the bias RF signal having a bias RF frequency of between about 45 MHz and about 75 MHz. The bias RF signal further has a bias RF power component that is configured to cause the feature to be etched in accordance to predefined etch rate parameters and etch profile parameters at the bias RF frequency.  
         [0021]     In yet another embodiment, the invention relates to a method, in a single frequency source plasma processing system for etching a feature through a dielectric layer of a dual damascene stack on a semiconductor substrate. The method includes placing the substrate in a plasma processing chamber of the plasma processing system. The method further includes flowing an etchant gas mixture into the plasma processing chamber, the etchant gas mixture being configured to etch the dielectric layer. The method additionally includes striking a plasma from the etchant source gas. There is further included etching the feature through the dielectric layer while applying a bias RF signal to the substrate, the bias RF signal having a bias RF frequency of about 60 MHz, the bias RF signal having a bias RF power component that is between about 200 W and about 1,500 W.  
         [0022]     These and other features of the present invention will be described in more detail below in the detailed description of the invention and in conjunction with the following figures. 
     
    
     BRIEF DESCRIPTION OF THE DRAWINGS  
       [0023]     The present invention is illustrated by way of example, and not by way of limitation, in the figures of the accompanying drawings and in which like reference numerals refer to similar elements and in which:  
         [0024]     FIGS.  1 A-J illustrate a cross-sectional view of an exemplary layer stack  100  undergoing the dual damascene process;  
         [0025]      FIG. 2A  illustrates a simplified diagram of a dual frequency triode plasma processing system;  
         [0026]      FIG. 2B  illustrates a simplified diagram of a dual frequency diode plasma processing system;  
         [0027]      FIG. 2C  illustrates a simplified diagram of a single frequency triode plasma processing system;  
         [0028]      FIG. 3  illustrates a layer stack in which the etch profile is faceted due to inadequately optimized plasma.  
         [0029]      FIG. 4  illustrates a layer stack in which the etch is incomplete due to inadequately optimized plasma.  
         [0030]      FIG. 5  illustrates a simplified diagram comparing faceting and etch rate to RF frequency at a given power level, according to one embodiment of the invention. 
     
    
     DETAILED DESCRIPTION OF THE PREFERRED EMBODIMENTS  
       [0031]     The present invention will now be described in detail with reference to a few preferred embodiments thereof as illustrated in the accompanying drawings. In the following description, numerous specific details are set forth in order to provide a thorough understanding of the present invention. It will be apparent, however, to one skilled in the art, that the present invention may be practiced without some or all of these specific details. In other instances, well known process steps and/or structures have not been described in detail in order to not unnecessarily obscure the present invention.  
         [0032]     While not wishing to be bound by theory, it is believed by the inventor herein that in a plasma processing system, that faceting and/or corner sputtering (generically, etch profile) is strongly influenced by ion energy. Ion energy, in turn, is strongly influenced by the RF configuration of the bias RF signal, particularly to the frequency component of the bias RF signal. The ion energy is also influenced by the power component of the bias RF signal. The invention thus addresses the use of bias RF signal configuration in plasma processing systems in order to minimize faceting and/or corner sputtering and/or improves the vertical etch profile in dielectric etches, particularly in dielectric etched through low-K layers.  
         [0033]     It is believed that plasma is generally comprised of weakly ionized plasma. Because the plasma discharge is RF driven and weakly ionized, electrons in the plasma are not in thermal equilibrium with ions. That is, while the heavier ions efficiently exchange energy by collisions with the background gas (e.g., argon, etc.), electrons absorb the thermal energy. Because electrons have substantially less mass than that of ions, electron thermal velocity is much greater than the ion thermal velocity. This tends to cause the faster moving electrons to be lost to surfaces within the plasma processing system, subsequently creating positively charged ion sheath between the plasma and the surface.  
         [0034]     Ions that enter the sheath are then accelerated into the surface. Lower bias RF frequencies tend to cause plasma ions to cross the sheath in less than one RF cycle. Generally speaking, lower bias RF frequencies tend to result in higher ion energy, which leads to faceting and/or corner sputtering if the RF bias signal not optimized. Likewise, higher bias RF frequencies tend to cause plasma ions take several RF cycles to cross the sheath. Generally speaking, the higher bias RF frequencies tend to result in lower ion energy, which results in inadequate etching or non-anisotropic etching if the RF bias signal is not optimized.  
         [0035]     It is believed that if the ion energy is not properly optimized, the etch is slowed down to the point where the etch rate becomes unduly slow for efficient production. Alternatively and/or additionally, faceting and/or corner sputtering occurs.  
         [0036]      FIG. 3  shows the situation wherein the ion energy is not optimized during the IMD trench etch that is employed to create a second metal layer and etch through a via hole to contact barrier layer  104 , resulting in cornering sputtering/faceting. In comparison to etch profile  118  in  FIG. 1H , etch profile  416  has been substantially corrupted due excessive ion energy (e.g., by using a bias RF signal with an unduly low frequency), causing severe faceting and/or corner sputtering. This corner sputtering can be clearly seen by the excessive material removed from the corner regions in mask layer  102  and IMD layer  106 .  
         [0037]      FIG. 4  shows the situation wherein the ion energy is not optimized during the IMD trench etch that is employed to create a second metal layer and etch through a via hole to contact barrier layer  104 , resulting in a taper trench profile and an incomplete via etch.  
         [0038]     Referring now to  FIG. 5 , a simplified diagram comparing faceting (represented by the dashed line and measured against axis  502 ), etch rate through the low-K layer (represented by the solid line and measured against axis  504 ) as a function of the bias RF frequency (shown on axis  506 ) at a given power level. Faceting may be measured using conventional faceting measurement methodology.  FIG. 5  intends to illustrate that as the bias RF frequency is increased, the etch rate increases and the amount of faceting/corner sputtering decreases (e.g., from about 2 MHz to about 60 MHz in our example). In particular, the increase in etch rate is rapid to about 30 MHz, and then increases less rapidly to about 60 MHz where the etch rate essentially flattens out until about 70 MHz. After about 70 MHz, the etch rate begins to slow down dramatically (e.g., from about 70 MHz to about 100 MHz), signifying that the ion energy level is now below what is necessary for an efficient etch.  
         [0039]     At the bias RF frequency of 60 MHz  512 , it is observed by the inventors that the etch rate is at its maximum while the faceting is near its minimum. However, an advantageous process window exists when the bias RF signal is between about 30 MHz and about 80 MHz, and even an even more advantageous process window exists when the bias RF signal is between about 45 MHz and abut 75 MHz where the etch rate is high and the faceting/corner sputtering is low.  
         [0040]     Generally speaking, increasing the bias RF power at a given bias RF frequency setting will cause an increase in both the etch rate and the amount of faceting/corner sputtering. Too much bias RF power will cause an excessive amount of faceting/corner sputtering while too little bias RF power will unduly decrease the etch rate. Thus, power setting is another knob for controlling the process to stay within the desired etch rate vs. faceting/corner sputtering parameters.  
         [0041]     In accordance with one embodiment of the invention, in order to optimize the plasma etch rate while also minimizing faceting in a plasma processing system, a bias RF signal of between about 27 MHz and about 90 MHz in frequency may be employed for a dual damascene trench etch through the low-K dielectric layer. Bias frequency is important as it controls the ion energy distribution. At a higher bias frequency, the ion energy distribution is narrow and contributes to the reduction of the corner sputtering/faceting problem. The bias RF signal is preferably selected with an optimal combination of bias RF frequency/bias RF power such that the ion energy is optimized and minimal and/or commercially acceptable faceting and corner sputtering is achieved while maintaining a commercially acceptable vertical profile. As the term is employed herein, commercially acceptability denotes that the result falls within specification for satisfactory operation of the final semiconductor product under fabrication. The optimal bias frequency/bias power combination may be empirically determined for a test substrate and the optimal parameters found may be employed during production. Of course the optimal bias frequency/bias power combination varies depending on the chemistry employed and the composition of the layer being etched.  
         [0042]     For example, at about 27 MHz of bias frequency, the RF power setting may be between about 100 W and about 1500 W, more preferably between about 200 W and 1,200 W, and preferably at about 400 W. For example, at about 90 MHz of bias frequency, the RF power setting may be between about 200 W and about 2,000 W, more preferably between about 400 W and 1,500 W, and preferably at about 1,000 W.  
         [0043]     In accordance with another embodiment of the invention, in order to optimize the plasma etch rate while also minimizing faceting in a dual frequency triode plasma processing system, a bias RF signal of between about 30 MHz and about 80 MHz in frequency may be employed. The bias RF signal is preferably selected with an optimal combination of bias RF frequency/bias RF power such that the ion energy is controlled and minimal and/or commercially acceptable faceting and corner sputtering is achieved while maintaining a commercially acceptable vertical profile. For example, at about 30 MHz of bias frequency, the RF power setting may be between about 100 W and about 1500 W, more preferably between about 200 W and 1,200 W, and preferably at about 400 W. For example, at about 80 MHz of bias frequency, the RF power setting may be between about 200 W and about 1,800 W, more preferably between about 400 W and 1,200 W, and preferably at about 800 W.  
         [0044]     In accordance with another embodiment of the invention, in order to optimize the plasma etch rate while also minimizing faceting in a dual frequency triode plasma processing system, a bias RF signal of between about 45 MHz and about 75 MHz in frequency may be employed. The bias RF signal is preferably selected with an optimal combination of bias RF frequency/bias RF power such that the ion energy is controlled and minimal and/or commercially acceptable faceting and corner sputtering is achieved while maintaining a commercially acceptable vertical profile. For example, at about 45 MHz of bias frequency, the RF power setting may be between about 100 W and about 1500 W, more preferably between about 200 W and 1,200 W, and preferably at about 400 W. For example, at about 75 MHz of bias frequency, the RF power setting may be between about 200 W and about 1,800 W, more preferably between about 400 W and 1,200 W, and preferably at about 800 W.  
         [0045]     In accordance with another embodiment of the invention, in order to optimize the plasma etch rate while also minimizing faceting in a dual frequency triode plasma processing system, a bias RF signal of about 60 MHz is found to be particularly suitable. The bias RF signal is preferably selected with an optimal combination of bias RF frequency/bias RF power such that the ion energy is controlled and minimal and/or commercially acceptable faceting and corner sputtering is achieved while maintaining a commercially acceptable vertical profile. For example, at about 60 MHz of bias frequency, the RF power setting may be between about 200 W and about 1,500 W, more preferably between about 400 W and 1,000 W, and preferably at about 600 W.  
         [0046]     In conjunction with the guidelines discussed above, a graph similar to  FIG. 5  also furnishes a way for a process engineer to tune a particular dielectric etch process to a particular plasma processing chamber configuration. If a set of data for etch rate vs. faceting/corner sputtering is empirically obtained for a range of bias RF frequencies of interest and/or a range of RF power settings of interest, the process engineer can more accurately obtain the desired process window with the bias RF frequency knob and the bias RF power knob for a particular dielectric etch process and/or a particular plasma processing system while still achieving the desired parameters (i.e., at particular values or within an acceptable range of values) with respect to the etch rate and faceting/corner sputtering (generically, etch profile).  
         [0047]     With respect to the discussion above, it is noted that the plasma processing chamber may be of a dual frequency design, i.e., one having a separate source RF signal and a separate bias RF signal. The source RF signal and the bias RF signal may be provided in a dual-frequency diode configuration (wherein both the source RF signal and the bias RF signal are applied to the substrate such as in an Excelan™ series machine by Lam Research Corporation of Fremont, Calif.), a dual-frequency triode configuration (wherein only the RF bias signal is applied to the substrate).  
         [0048]     Additionally, the plasma processing chamber may be of a single frequency design, i.e., only RF bias signal with no separate source RF signal. Since the bias RF signal controls the ion energy, proper control of the bias RF signal results in the desired minimization of faceting and corner sputtering while maintaining a commercially acceptable vertical profile. It has been found that with a single-frequency design, a bias RF frequency signal of between about 45 MHz and about 75 MHz is particularly useful for minimizing faceting and/or corner sputtering while maintaining the aforementioned commercially acceptable vertical etch profile. In particular, it has been found that the single frequency design, when operated at a bias RF signal of about 60 MHz is particularly well-suited to for minimizing faceting and/or corner sputtering while maintaining the aforementioned commercially acceptable vertical etch profile for a dual-damascene trench etch.  
         [0049]     Furthermore, it is not necessary that the plasma processing chamber be of a capacitively coupled plasma design. For example, the top RF source may be an inductive coil (such as those in TCP™ plasma etchers available from Lam Research Corporation of Fremont, Calif.), and the bias RF signal may still be provided to the substrate and controlled during etching. Likewise, the top RF source may be an ECR (Electron Cyclotron Resonance) source, and the bias RF signal may still be provided to the substrate and controlled during etching. In fact, it is contemplated that the source RF signal may be furnished using any RF signal generation arrangement since the invention deals with controlling the bias RF frequency and/or bias RF power to achieve the desired etch rate and low faceting/corner sputtering parameters.  
         [0050]     While this invention has been described in terms of several preferred embodiments, there are alterations, permutations, and equivalents which fall within the scope of this invention. For example, although the present invention has been described in connection with Lam Research plasma processing systems (e.g., Exelan™, Exelan HP™, Exelan HPT™, Exelan 2300™, etc.), other plasma processing systems may be used. It should also be noted that there are many alternative ways of implementing the methods of the present invention.  
         [0051]     Advantages of the invention include the optimization of RF configurations in a plasma processing system, in which an optimum set of frequencies and an optimum set of power settings are employed to substantially control faceting. Additional advantages include optimizing RF configurations in dual damascene plasma processing applications in order to substantially control faceting.  
         [0052]     Having disclosed exemplary embodiments and the best mode, modifications and variations may be made to the disclosed embodiments while remaining within the subject and spirit of the invention as defined by the following claims.