The present invention relates to on-chip power inductor structures and to methods of making a controlled seam laminated magnetic core for high frequency on-chip power inductors.
Laminating a magnetic core is a well know technique that reduces the adverse effect of eddy currents on the performance of inductors and transformers. While being relatively straightforward to implement in the macro world, fabricating laminations presents challenges in the case of micro-fabricated and on-chip inductor structures.
One of the approaches to fabricating on-chip inductors is to deposit laminations horizontally, layer by layer, separated by thin dielectric films. Those skilled in the art will appreciate that this approach requires multiple deposition steps to build sufficient volume of magnetic material, which makes this approach prohibitively expensive. Therefore, all practical solutions of this type to date are limited to one or two laminations. See, for example, S. C. O. Mathuna et al., “Magnetics on Silicon: An Enabling Technology for Power Supply on Chip,” IEEE Transactions on Power Electronics, Vol. 20, No. 3, May 2005, pp. 585-592. In this case, the performance of the inductor is limited because of the low total amount of magnetic material.
Alternatively, laminations can be built vertically utilizing photolithography. These solutions are known for very thin film inductors that do not receive practical exposure for the same reasons set forth above with respect to the horizontal lamination approach. See, for example, D.S. Gardner et al., “Integrated On-Chip Inductors With Magnetic Films,” IEEE Transactions on Magnetics, Vol. 43, No. 6, June 2007. pp. 2615-2617.
Another type of known micro-fabricated inductor utilizes vertical laminations that are large (i.e., hundreds of microns in cross-section), which does little to help reduce eddy currents. See, for example, P. Galle et al., “Ultra-Compact Power Conversion Based on a CMOPS-Compatible Microfabricated Power Inductor with Minimized Core Losses,” 2007 Electronic Components Technology Conference, pp. 1889-1894. In addition, inductors of this type are prohibitively large.
Commonly-assigned and co-pending U.S. patent application Ser. No. 12/082,209, filed on Apr. 9, 2008, by Smeys et al., and titled “ MEMS Power Inductor and Method of Forming the MEMS Power Inductor,” discloses a scalable MEMS inductor formed on the top surface of a semiconductor die. The disclosed thick film magnetic inductors have vertically designed laminations that are built inside thick photoresistive films, thereby providing large volumes of magnetic material while the cross-sectional dimension of about 10 μm helps to make this high performance device within a few square millimeters. The aspect ratio of the lamination cross-section is in the range of 3:1 to 4:1, which reduces eddy currents. (See also, U.S. Pat. No. 7,705,411, which issued to Smeys et al. on Apr. 27, 2010, and is hereby incorporated by reference herein in its entirety to provide background information regarding the present invention.)
Each substrate region 110 includes a number of structures, such as resistors, transistors, capacitors, diodes and similar active devices, which are formed in and on the substrate region 110. Each metal interconnect structure 112, in turn, is a multi-layered structure that electrically interconnects the various devices that are formed in or on the substrate region 110 to realize an integrated electrical circuit.
As further shown in
In addition, a number of opening are formed in the layer of passivation material 116 to expose selected regions SR1 on the top surfaces of the conductive structures 114 in each metal interconnect structure 112. The selected regions SR1, in turn, form connection points for a copper-topped structure. (Only one selected region SR1 is shown for clarity.)
Further, openings are also formed in the layer of passivation material 116 to expose selected regions SR2 and SR3 on the top surfaces of the conductive structures 114 in each metal interconnect structure112. The selected regions SR2 and SR3 form first and second connection points for a MEMS inductor, described in detail below.
Semiconductor wafer 100 also includes a number of identical copper-topped structures 118 and a number of identical copper MEMS inductors 120 that are formed on the metal interconnect structures 112. Each copper-topped structure 118, which includes vias, traces and pads, touches the passivation layer 116 and the selected regions SR1 of a metal interconnect structure 112. In operation, each copper-topped structure 118 provides signal and power routing, and external electrical connection points for an integrated circuit. Thus, once packaged, bonding wires can be connected to the pad regions of each copper-topped structure 118.
Each copper MEMS inductor 120, in turn includes a conductive base plate 122 with a via extension 122A that touches the passivation layer 116 and the selected region SR2 of a metal interconnect structure 112, and a conductive plug 124 with a via extension 124A that touches the passivation layer 116 and the selected region SR3 of a metal interconnect structure 112.
Each MEMS inductor 120 further includes a top conductive plate 126 that lies over the base conductive plate 122. In the illustrated example, the widths and thicknesses of the plates 122 and 126 are substantially identical. Each top conductive plate 126 has a first via extension 126A that touches a base conductive plate 122 of a metal interconnect structure 112, and a second via extension 126B that touches a conductive plug 124 of a metal interconnect structure 112. In addition, base conductive plate 122, top conductive plate 126, and the via extensions 126A and 126B, define an enclosed region 130 that lies only between the base and top conductive plates 122 and 126, and the via extensions 126A and 126B.
In the
As further shown in
In operation, a current I1 can flow into a MEMS inductor 120 through base conductive plate 122 by way of via extension 122A and selected region SR2, and flow out of conductive plug 124 via selected region SR3. A current 12 can also flow in the opposite direction, flowing into MEMS inductor 120 through conductive plug 124 by way of selected region SR3, and out along via extension 122A of base conductive plate 122 and selected region SR2. A current flowing through an inductor generates a magnetic field that produces a magnetic flux density. The magnetic flux density, in turn, is a measure of the total magnetic effect that is produced by the current flowing through the inductor.
One problem with the formation of a MEMS inductor is that it is difficult to form a MEMS inductor that is scalable to frequencies of operation that are greater than 10 MHz at currents that are greater than a few 100 mA.
As shown in
In addition, the top section of each metal interconnect structure 212 includes a number of conductive structures 214, such as aluminum traces, and a layer of passivation material 216, such as silicon nitride, silicon oxide, or a combination of the two, that touches and isolates the conductive structures 214. The conductive structures 214, in turn, include a pair of MEMS-supporting conductive structures 214A and 214B, For example, the pair of MEMS-supporting conductive structures 214A and 214B can represent the input and the output nodes of a MEMS inductor.
Further, in the illustrated embodiment, semiconductor wafer 200 includes a stress relief layer 220 that lies on passivation layer 216. Stress relief layer 220 is able to laterally deform enough to absorb dimensional changes from the materials used to form a MEMS inductor, and prevent stress from being transmitted to the underlying metal interconnect structures 212 and substrate regions 210.
Stress relief layer 220 is implemented with a material that has a maximum bulk elongation that is substantially greater than the maximum bulk elongation of the material used to form passivation layer 216, such as silicon oxide and silicon nitride, and the maximum bulk elongation of the material used to form the MEMS devices such as oxide, SU-8 epoxy, permalloy and copper. Bulk elongation is a well-known measure of the amount a structure can stretch before it breaks.
For example, stress relief layer 220 can be implemented with a spin-on benzocyclobutene (BCB) or photoimagible elastomer, such as photoimagible silicone WL-5150 manufactured by Dow Corning®. The adhesion properties of these two materials are excellent, and provide a suitable base layer for subsequent MEMS processing.
BCB has a maximum bulk elongation of approximately 8%, while the Dow Corning material has a maximum bulk elongation of approximately 30%. Alternately, other formulations of isolating films with large maximum bulk elongation values would work equally as well. By contrast, silicon oxide and silicon nitride have a very small maximum bulk elongation of, for example, 2%. Similarly, copper, permalloy, silicon dioxide and SU-8 epoxy have a very small maximum bulk elongation of, for example, 2%. Thus, the maximum bulk elongation of the stress relief layer 220 is substantially greater than the maximum bulk elongations of passivation layer 216 and the materials that are used to form a MEMS device, ranging from 4× to 15× greater.
In addition, stress relief layer 220 can also be implemented with a material that can be fully cured (hardened) at a temperature, such as 250° C., that is greater than the highest subsequent processing temperature. Curing the stress relief layer 220 at a temperature that is higher than the highest subsequent process temperature ensures stability of the film.
As shown in
In the illustrated embodiment, the lower mold 224 is implemented utilizing SU-8 which, as noted above, has a very low maximum bulk elongation when compared to the maximum bulk elongation of stress relief layer 220. In addition, the controlled seam magnetic core lower laminations, which function as a lower magnetic core structure, can be implemented with, for example, laminated permalloy (Ni—Fe) or other magnetic materials, as discussed in greater detail below. The thickness of the laminations must be thin enough to minimize eddy currents. Further, the controlled magnetic lower laminations 226 are totally electrically isolated from each other and from all other conductive structures.
In addition, MEMS inductor 222 includes a nonconductive isolation layer, for example, a magnetic gap dielectric layer 230, that is formed on mold 224 and the controlled seam magnetic lower laminations 226. The magnetic gap dielectric layer 230 can be implemented utilizing, for example, SU-8 epoxy. Lower mold 224 and magnetic gap isolation layer 230 electrically isolate each of the controlled seam magnetic lower laminations 226.
MEMS inductor 222 further includes a (square) circular copper trace 232 that touches the magnetic gap isolation layer 230 and a pair of copper plugs 234 that touch the pair MEMS-supporting conductive structures 214A and 214B. Copper trace 232, which lies directly over each of the controlled seam magnetic lower laminations 226, ids illustrated in
As further shown in
In addition, MEMS inductor 222 includes a number of controlled seam magnetic upper laminations 244 that touch molds 240 and 242 (the upper mold) directly over each metal interconnect structure 212. The controlled seam magnetic upper laminations, which function as an upper magnetic core structure, can be implemented utilizing, for example, laminated permalloy (Ni—Fe) or other magnetic materials, as discussed in greater detail below. The thickness of the laminations must be thin enough to minimize eddy currents. Further, the magnetic upper laminations 244 are totally electrically isolated from each other and from all other conductive structures.
As shown in
MEMS inductor 222 also includes a passivation layer 246 that is formed on mold 242 and the controlled seam magnetic upper laminations 244. Molds 240 and 242 (the upper mold) and passivation layer 246 electrically isolate each of the controlled seam magnetic upper laminations 244. Passivation layer 246 can be implemented utilizing, for example, benzocyclobutene (BCB). In addition, openings 248 are formed in passivation layer 246 to expose the copper plugs 234.
Thus, in the illustrated embodiment, wafer bow is prevented by utilizing a stress relief layer 220 that laterally deforms enough to absorb dimensional changes from the materials that are used to form the MEMS inductors, and thereby prevents stress from being transmitted to the underlying metal interconnect structures 212 and substrate regions 210.
As shown in
Each substrate region 310 includes a number of structures, such as resistors, transistors, capacitors, diodes and similar devices, which are formed in and on the substrate region 310. Each metal interconnect structure 312, in turn, is a multi-layered structure that electrically interconnects the various devices that are formed in a substrate region 310 to realize an integrated electrical circuit.
As further shown in
The method begins by forming a stress relief layer 320 on the top surface of the passivation layer 316. In the illustrated embodiment, stress relief layer 320 is implemented with a material that has a maximum bulk elongation that is substantially greater than the maximum bulk elongation of the material used to form passivation layer 316. For example, a 5 μm thick film of BCB or WL-5150 on top of passivation layer 316 can effectively absorb the lateral stress from a MEMS structure (e.g., SU-8/copper/permalloy) which has thickness of 5-100 μm. In addition, stress relief layer 320 can be implemented with a material that can be cured at a temperature that is higher than the highest subsequent process temperature.
Referring back to
After mask 322 has been removed, as shown in
Following this, the soft baked epoxy is again baked, and then developed, such as by using immersion development at room temperature. After the development, the unexposed regions of the soft baked epoxy are rinsed away and removed. Once the unexposed regions of the soft baked epoxy have been removed, the developed epoxy is cured to form mold 324. As shown in
Referring to
In contrast, while the method of the present invention utilizes damascene ECD, the process stops prior to pinch off. That is, the controlled seam lamination includes a horizontal base and spaced-apart sidewalls that extend substantially vertically upward from the base. A cross-section of the resulting controlled seam lamination is shown in
Thus, in accordance with the concepts of the present invention, as shown in
Following the formation of mask 330, as shown in
As shown in
Next, as shown in
After a magnetic gap dielectric layer 336 has been formed, a copper seed layer 340 is formed on magnetic gap dielectric layer 336 and copper seed layer 326. Copper seed layer 340 can be implemented utilizing, for example, 330 Å of titanium, 3000 Å of copper and 300 Å of titanium. After copper seed layer 340 has been formed, a non-conductive mold 342 is formed on copper seed layer 340. Mold 342 can be formed, for example, by forming and patterning a photoresist layer, such as AZ or NR2, to have a thickness of approximately 55 μm.
As shown in
After mold 342 and the exposed regions of copper seed layer 340 have been removed, as shown in
After base mold 350 has been formed, as show in
As shown in
Next, as shown in
Next, as shown in
It should be understood that the above describes exemplary embodiments of the present invention and that various alternatives of the embodiments described herein may be employed in practicing the invention. Therefore, it is intended that the following claims define the scope of the invention and that structures and methods within the scope of these claims and their equivalents be covered thereby.
This application is related to co-pending and commonly-assigned application Ser. No. 12/082,209, filed on Apr. 9, 2008, and published on Oct. 15, 2009, as Publication No. U.S. 2009/0256667 A1. Application Ser. No. 12/082,209 is hereby incorporated by reference herein in its entirety.