Electroplating may be used in integrated circuit manufacturing processes to form electrically conductive structures. For example, in a copper damascene process, electroplating is used to form copper lines and vias within channels previously etched into a dielectric layer. In one example of such a process, an electrically conductive seed layer is first deposited into the channels and on the substrate surface, for example, via physical vapor deposition. Then, electroplating is used to deposit a thicker copper layer over the seed layer such that the channels are completely filled. Excess copper is then removed by chemical mechanical polishing, thereby forming the individual copper features.
As integrated circuit fabrication technologies advance, thinner and thinner seed layers are being used for electroplating processes. However, the use of thin seed layers may pose problems with the plating of a uniform film over the seed layer. For example, thinner seed layers can lead to a larger voltage drop between the electrical contacts that provide current to the seed layer and portions of the seed layer that are remote from the contacts. Because electrical contacts are generally made to a seed layer on a wafer at locations adjacent to an outer edge of the wafer, a significant voltage drop may exist between the edge of the wafer and the center of the wafer due to the thinness of the seed layer. This may cause higher film growth rates near the wafer perimeter than near the wafer center.
Various approaches have been employed to overcome such difficulties. For example, in one approach, segmented anodes comprising two or more anode sections with separately controllable potentials relative to the wafer surface (e.g. cathode) have been proposed to dynamically control plating rates on different regions of the wafer surface. Other approaches involve controlling the chemistry of the plating solution, for example, to increase a charge transfer resistance at the wafer-electrolyte interface via copper complexing agents or charge transfer inhibitors, to increase a resistance of the electrolyte surface by reducing an ionic conductivity of the plating solution, etc. These chemical approaches attempt to increase the resistance of other components of the plating circuit to reduce the effects of the seed layer resistance. However, the seed layer resistance of a thinly seeded wafer may be too high for such approaches to be effective. Further, various other factors may affect the uniformity of an electroplated film, including but not limited to electrolyte current uniformity, ionic current uniformity, the presence of bubbles in the electrolyte, etc.
Accordingly, various embodiments related to increasing a uniformity of an electroplated film are disclosed. For example, one disclosed embodiment provides an apparatus for electroplating a layer of metal onto a conductive seed layer on a work piece. The disclosed apparatus comprises a plating chamber configured to hold an electrolyte, a work piece holder configured to hold a work piece in the plating chamber during an electroplating process, a cathode contact associated with the work piece holder and configured to electrically contact a the work piece during plating, and an anode contact configured to electrically contact an anode disposed in the plating chamber. Further, a diffusing barrier is disposed between the cathode contact and the anode, an electrolyte delivery path is provided for delivering electrolyte to the plating chamber, and an electrolyte return path is provided for delivering electrolyte away from the plating chamber. Additionally, a vented electrolyte manifold is disposed in the electrolyte delivery path upstream from the plating chamber, the vented electrolyte manifold comprising one or more electrolyte delivery openings that open to the plating chamber and one or more vents that open to a location other than the plating chamber.
This Summary is provided to introduce a selection of concepts in a simplified form that are further described below in the Detailed Description. This Summary is not intended to identify key features or essential features of the claimed subject matter, nor is it intended to be used to limit the scope of the claimed subject matter. Furthermore, the claimed subject matter is not limited to implementations that solve any or all disadvantages noted in any part of this disclosure.
The cathode chamber 106 is configured to accommodate a work piece holder that comprises one or more electrical contacts configured to provide a flow of current to a work piece acting as a cathode. The cathode contacts, work piece holder, and work piece are collectively indicated schematically at 116. In one embodiment, the cathode may take the form of an electrically conductive seed layer on a semiconductor wafer.
The anode chamber 104 comprises an anolyte solution 109 and the diffuser chamber 114 and the cathode chamber 106 each comprise a catholyte solution. During electroplating, an electric field is established between the anode 110 and the cathode 116. This field drives positive ions from the separated anode chamber 104 through the selective transport barrier 108, through the diffuser chamber 114, the diffuser barrier 112, into the cathode chamber 106 and to the cathode 116. At the cathode, an electrochemical reaction takes place in which metal cations are reduced to form a solid layer of the metal on the surface of the cathode 116. An anodic potential is applied to the anode 110 via an anode electrical connection 118, and a cathodic potential is provided to the cathode 116 via a cathode electrical connection 120. In some embodiments, the cathode 116 may be rotated during plating. While the diffuser barrier 112 and selective transport barrier 108 are depicted as being between the anode 110 and cathode 116 along a straight-line path between the electrodes, it will be understood that the path between the anode and the cathode in other embodiments may not be a straight-line. The description of the diffuser barrier and selective transport barrier as being between the anode and the cathode refers to herein as being along an ionic pathway between the electrodes, and does not imply any specific pathway shape or geometry between the electrodes.
The anolyte in the anode chamber 104 may be stored in and replenished from an anolyte reservoir 122. The temperature and composition of the anolyte may be controlled in the anolyte reservoir 122. Anolyte may be circulated through the anolyte reservoir 122 and the anode chamber 104 via, for example, a combination of gravity and one or more pumps 124. Likewise, the catholyte may be circulated from a catholyte reservoir 126 into the diffuser chamber 114, then the cathode chamber 106, and back to the catholyte reservoir 126 via, for example, a combination of gravity and one or more pumps 128.
The selective transport barrier 108 allows a separate chemical and/or physical environment to be maintained within the SAC 109 compared to the cathode chamber 106 and the diffuser chamber 114. For example, the selective transport barrier 108 may be configured to prevent non-ionic organic species from crossing the barrier while allowing metal ions to cross the barrier. The catholyte may contain various organic additives, such as levelers, accelerators and suppressors, that aid in plating copper onto the cathode 116 but that may poison the anode 110 or otherwise harm anode performance. Therefore, the selective transport barrier 108 may be configured to prevent such organic additives in the catholyte from contaminating the anolyte while allowing copper from the anolyte to reach the catholyte.
The selective transport barrier 108 may be made from any suitable material or materials. In some embodiments, the selective transport barrier may be made from a material or material that is porous and that allows passage of both anions and cations. Examples of suitable materials include, but are not limited to, porous glasses, porous ceramics (e.g. alumina and zirconia), silica aerogels, organic aerogels, and porous polymeric materials such as polyvinylidene flouride, sintered polyethylene or sintered polypropylene. In one specific embodiment, the selective transport barrier 108 comprises Nafion, available from E.I. DuPont De Nemours and Company of Wilmington, Del. In yet other embodiments, a multi-layer structure comprising one or more layers of a material with smaller pores and one or more layers of a material with larger pores may be used.
The diffuser barrier 112 also may be made from any suitable material, and may have any suitable construction and location within the plating cell 102. As mentioned above, the diffuser barrier 112 is configured to create a uniform flow of electrolyte across the surface of a work piece during a plating process. Therefore, suitable materials include porous materials configured to allow passage of a desired flow rate of electrolyte. Examples of suitable materials include, but are not limited to, electrically insulating materials such as sintered plastics, porous ceramics, and sintered glasses.
In order for plating uniformity to benefit from the uniform flow emanating from the diffuser barrier 112, the surface of a work piece to be plated may be placed in close proximity to the diffuser barrier 112 during a plating process. In one specific embodiment, a wafer surface is placed within 5 mm or less of the diffuser barrier surface 112 during plating. In other embodiments, the diffuser barrier 112 may have any other suitable location.
In some embodiments, the diffuser barrier 112 may be configured to have a relatively low ionic resistance and low fluid resistance. In such embodiments, the diffuser barrier may have a void fraction of, for example, 10-70%. In other embodiments, the diffuser barrier 112 may be configured to have a relatively high fluid and ionic resistance. Where the diffuser barrier 112 is configured to have a higher ionic resistance, the diffuser barrier 112 may have either an interconnected network of pores or other internal passages (such that fluid and ionic current can flow in a radial direction relative to a surface of a work piece being plated), or may have non-interconnected pores or passages such that fluid and ionic current does not flow from pore to pore, but instead flows one-dimensionally through the diffuser barrier 112 in a direction defined by the direction of through-holed extending through the diffuser barrier 112. In some embodiments, such a diffuser barrier 112 may comprise a plate of an ionically resistive material, such as polyethylene, polypropylene, polyvinylidene difluoride (PVDF), polytetrafluoroethylne, polysulphone, etc.
In one example embodiment, a highly ionically resistive diffuser barrier 112 with one-dimensional through-holes for use in plating a 300 mm wafer comprises an ionically resistive disc having a thickness of 5-25 mm, with a shape and size co-extensive with the shape and size of the wafer. The disc comprises between 6,000 and 12,000 non-interconnected (i.e. “one-dimensional”) through-holes, each with a diameter of a millimeter or less, formed through the plate in a direction normal to the major faces of the plate. Such a high-resistance, one-dimensional diffuser barrier may have a void fraction, for example of 5% or less. An ionically resistive, low-void fraction diffuser barrier such as the described example may be referred to herein as a “high resistance virtual anode” (HRVA), as the structure exhibits high ionic and fluidic resistance, and ionic current flow density from such a diffuser barrier approximates that from a uniformly charged anode of similar dimensions placed in a similar location. It will be understood that this diffuser plate embodiment is described for the purpose of example, and that a diffuser plate may have any other suitable construction and configuration.
It will be understood that the embodiment of
The anode chamber 104 may include an anode (not shown in
The vented electrolyte manifold 210 is configured to vent bubbles out of the electrolyte before the electrolyte is introduced into the diffuser chamber 114. As described in more detail below, the introduction of bubbles into the diffuser chamber of a larger size than the through-holes in the diffuser barrier 112 may result in the bubbles being trapped beneath the diffuser barrier 112. These bubbles may block the flow of electrolyte through the diffuser barrier 112, and therefore may cause non-uniform plating to occur in the region of the work piece that is impacted by the blocked flow. Such problems may be particularly evident in the case of a one-dimensional HRVA, as the one-dimensional channels and the close proximity of a work piece to the HRVA during use prevent lateral electrolyte flow from compensating for the blocked electrolyte flow.
Bubbles may arise from various sources in an electroplating system. For example, bubbles can be formed by fluid returning from a plating cell agitating the surface of a reservoir/bath and being subsequently redirected back into the cell, air trapped in the electrolyte supply line and air trapped in the plating cell during the startup, small air leaks in the lines or cavitations on the negative pressure side of the pump that feed the electrolyte to the plating cell, release of gas from an electrolyte supersaturated under pressure at the pump, electrolytic gas generated at the anode, and various other mechanisms.
The vented electrolyte manifold 210 removes bubbles by establishing a suitably slow flow of electrolyte to allow any bubbles within a size range of concern to rise to the top of the manifold for removal via one or more vents located in the top of the manifold. The vented electrolyte manifold 210 may have any suitable configuration for removing bubbles in this manner. For example, the vented electrolyte manifold 210 may be configured to slow electrolyte flow and reduce turbulence in the electrolyte flow to thereby allow time for bubbles to rise out of the electrolyte and reach vents in the vented electrolyte manifold.
In the depicted embodiment, the vented manifold 210 comprises two fluid flow stages that are separated by a wall with one or more openings permitting electrolyte flow between the stages. As can be seen in
The conversion of turbulent flow from the electrolyte feed tubes 204 to laminar flow in the quiescent stage 220 of the vented manifold may help to improve bubble separation compared to the turbulent flow in the electrolyte feed tubes 204, as bubbles may be poorly separated in turbulent flow. This may allow bubbles some time to separate and rise to a top portion of the vented manifold for removal in the de-bubbler stage 222.
From the quiescent stage 220, electrolyte flows into the de-bubbler stage 222. The de-bubbler stage 222 comprises one or more electrolyte delivery openings 224 and/or flow distribution tubes 225 that open to the diffuser chamber to deliver electrolyte to the diffuser chamber. The de-bubbler stage 222 also comprises one or more vents 226 that open to the electrolyte return path to allow a smaller flow of electrolyte to carry any separated bubbles directly to the electrolyte return path, rather than to the diffuser chamber. The locations of the terminal openings of the electrolyte delivery openings 224 and the vents 226 are shown in more detail in
To facilitate bubble removal, the electrolyte delivery openings 224 may be located at a lower position in the vented electrolyte manifold than the vents 226. In the depicted embodiment, the electrolyte delivery openings 224 are located in or near a bottommost surface of the de-bubbler stage 222, while the vents 226 may be located in or near an uppermost surface of the de-bubbler stage 222. In this manner, bubbles that have risen in the electrolyte higher than a height of the electrolyte delivery openings 224 relative to the bottommost surface flow through the vents 226, rather than through the electrolyte delivery openings 224. As such, the vents 226 may be configured to pass a much smaller flow of electrolyte than the electrolyte delivery openings 224, yet a sufficient flow to assist with the venting of bubbles that collect and/or coalesce at the uppermost surface of the de-bubbler stage. Consideration of electrolyte flow rates, viscosity, manifold dimensions, etc. may allow the design of a vented electrolyte manifold 210 that provides sufficiently slow electrolyte flow to allow bubbles of specific sizes of concern to rise to the vents, and thereby avoid introduction into the diffuser chamber 114. Further, making the vented manifold integrated into the anode chamber and placing the de-bubbler stage immediately upstream of the diffuser chamber 114 (i.e. with no intermediary structures other than the outlets that pass electrolyte from the de-bubbler stage to the diffuser chamber through the wall of the vented manifold) decreases the likelihood that any new bubbles will form in the electrolyte as the electrolyte flows from the vented electrolyte manifold 112 to the diffuser barrier 112.
In the depicted embodiment, the de-bubbler stage 222 and the quiescent stage 220 each have a horizontally-oriented uppermost surface (i.e. parallel to the horizontal axis). However, in other embodiments, the uppermost surface of either or both of these sections may have a suitable incline or slope to direct bubbles toward the vents 226, or may have any other suitable configuration.
In the depicted embodiment, the quiescent stage 220 is separated from the de-bubbler stage 222 via a wall 232. The wall 232 slants at an angle outwardly as it rises up from the bottom to the top of the vented electrolyte manifold 210. In this manner, electrolyte flowing into the quiescent stage 220 from the electrolyte feed tubes 204 is deflected by the wall 232. This may help to slow the turbulent flow entering the quiescent state 220. The spatial relationship between an example electrolyte feed tube 204 and the wall 232 is shown in
In order to allow sufficient time for bubbles of the sizes of concern to rise to the top of the electrolyte solution for removal through vents (described below) in the de-bubbler stage 222, the vented electrolyte manifold 210 may be configured to cause electrolyte to flow horizontally in an azimuthal direction for a sufficient distance to allow a desired bubble rise time to pass. During horizontal azimuthal flow, bubbles may tend to rise to the uppermost surface of the vented electrolyte manifold 210. The bubbles may subsequently coalesce with other bubbles, and eventually displace a sufficient volume to cover the opening of a vent 226 and then be redirected out of the de-bubbler stage 222 through the vent 226.
The vented electrolyte manifold 210 may comprise any suitable structures configured to direct azimuthal electrolyte flow. For example, in the depicted embodiment, openings in the wall 224 between the quiescent stage 220 and the de-bubbler stage 222 are azimuthally spaced from the openings of the electrolyte feed tubes 204 into the quiescent stage 220.
Referring briefly back to
It will be understood that the depicted tabs are shown to illustrate one potential embodiment for separating electrolyte flow from the vents 226 and electrolyte flow over the weir wall 200, and are not intended to be limiting in any manner. For example, in another embodiment, spacers such as ribs or walls may be provided between vents 226 and the regions of the weir wall 200 over which electrolyte from the cathode chamber flows. Likewise, a tube or other structure may be provided to route flow from each vent 226 away from the flow of electrolyte over the weir wall 200. In any of these cases, the vents are spaced from the outer perimeter of the weir wall, thereby separating electrolyte flow out of the vents from flow over the weir wall.
The use of vented electrolyte manifold 210 may offer advantages in any plating cell. For example, in plating cells without a diffuser barrier 112, bubbles that reach the cathode surface may cause the formation of plating defects at that location on the surface, as the bubble prevents ionic current from reaching the cathode area beneath the bubble. Further, as mentioned above, bubbles that become trapped beneath the diffuser barrier 112 may block fluid flow and ionic current through a portion the diffuser barrier 112. Such problems may be more apparent where a one-dimensional HRVA is used as a diffuser barrier 112, as the close proximity of the work piece to the HRVA during plating may prevent lateral plating fluid flow from adjacent HRVA through-holes from compensating for the lack of flow through the blocked holes.
Next,
It will be appreciated that not all bubbles pose the problems illustrated in
Bubbles larger than this may be sufficiently stable such that removal by separation is more efficient than removal by dissolution. However, referring next to
On the other hand, bubbles larger than the HRVA through-holes may be stable enough that the bubbles do not dissolve into the electrolyte at an appreciable rate, and also may become trapped beneath the HRVA. Therefore, the vented electrolyte manifold may be configured to remove these bubbles from the electrolyte. In order to separate such bubbles from the electrolyte prior to delivery of the electrolyte into the plating chamber, the bubbles need sufficient time to rise higher in the electrolyte flow than the height of the electrolyte delivery openings that deliver electrolyte from the vented manifold into the plating chamber. In the specific embodiment shown in
In this example, it is desired for a bubble large enough to block the HRVA to rise more than the electrolyte delivery opening height in 7.5 seconds so that it can be removed and vented out through outlet 226 rather than the HRVA chamber inlet 224. From
In some embodiments, such as embodiments with relatively smaller diffuser barrier through-holes, it may be desired to separate smaller bubbles with slower rise times from the electrolyte that may rise too slowly for removal by the vented electrolyte manifold. In such embodiments, an additional bubble removal structure may be included in the vented electrolyte manifold. For example, one embodiment may provide a two-part de-bubbler stage. In such an embodiment, a first de-bubbler stage may remove larger bubbles via buoyancy, as described above. Then, a second de-bubbler stage may comprise a bubble removal filter configured to remove any bubbles that are not removed in the buoyancy separation stage, and/or to break up larger bubbles into smaller bubbles that can pass through the diffuser barrier without being trapped.
Any suitable structure may be used for such bubble removal filter. For example, in some embodiments, the bubble removal filter may comprise a porous material with a pore size that is equal to or smaller than the diameter of the diffuser barrier through-holes. In some embodiments, the filter may be made from a hydrophilic material that is wet by the electrolyte, thereby causing the electrolyte to reject gas bubbles. In embodiments, the filter may be made from a material that is hydrophobic but that adsorbs bubble gases to allow bubbles to coalesce, and therefore to rise more quickly to a vent opening. In one more specific embodiment, the bubble removal filter comprises a polysulphone filter with a pore size less than the size of the diffuser barrier through-holes and that is placed over the electrolyte delivery openings in the vented manifold. In this manner, the bubble removal filter is the last structure that the electrolyte passes through prior to entering the plating chamber. Because the filter pores are smaller than the diffuser barrier through-holes, only bubbles smaller than the diffuser barrier through-holes pass through the bubble removal filter. Such bubbles do not accumulate in front of or block diffuser barrier through-holes, but instead tend to travel through the diffuser barrier and then radially outwardly through the space between the diffuser barrier and the substrate above.
It be understood that the configurations and/or approaches described herein are exemplary in nature, and that these specific embodiments or examples are not to be considered in a limiting sense, because numerous variations are possible. The subject matter of the present disclosure includes all novel and nonobvious combinations and subcombinations of the various processes, systems and configurations, and other features, functions, acts, and/or properties disclosed herein, as well as any and all equivalents thereof.
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