Abstract:
Embodiments of a process chamber are provided herein. In some embodiments, a process chamber includes a chamber body having an interior volume, a substrate support disposed in the interior volume, a target disposed within the interior volume and opposing the substrate support, a process shield disposed in the interior volume and having an upper portion surrounding the target and a lower portion surrounding the substrate support, the upper portion having an inner diameter that is greater than an outer diameter of the target to define a gap between the process shield and the target, and a gas inlet to provide a gas to the interior volume through the gap or across a front opening of the gap to substantially prevent particles from the interior volume from entering the gap during use.
Abstract:
Embodiments of process kits for process chambers and methods for processing a substrate are provided herein. In some embodiments, a process kit includes a non-conductive upper shield having an upper portion to surround a sputtering target and a lower portion extending downward from the upper portion; and a conductive lower shield disposed radially outward of the non-conductive upper shield and having a cylindrical body with an upper portion and a lower portion, a lower wall projecting radially inward from the lower portion, and a lip protruding upward from the lower wall. The cylindrical body is spaced apart from the non-conductive upper shield by a first gap. The lower wall is spaced apart from the lower portion of the non-conductive upper shield by a second gap to limit a direct line of sight between a volume within the non-conductive upper shield and the cylindrical body of the conductive lower shield.
Abstract:
Light wave separation lattices and methods of formation are provided herein. In some embodiments, a light wave separation lattice includes a first layer having the formula ROxNy, wherein the first layer has a first refractive index; and a second layer, different from the first layer, disposed atop the first layer, and having the formula R′OxNy, wherein the second layer has a second refractive index different from the first refractive index, and wherein R and R′ are each one of a metal or a dielectric material. In some embodiments, a method of forming a light wave separation lattice includes depositing a first layer having a predetermined desired refractive index atop a substrate by a physical vapor deposition process; and depositing a second layer, different from the first layer, atop the first layer, wherein the second layer has a predetermined second refractive index different from the first refractive index.
Abstract:
A movable substrate support with a top surface for holding a substrate, when present, is used in conjunction with a cover ring that is stationary to adjust for a shadow effect to control substrate edge uniformity during deposition processes. The cover ring is held stationary by an electrically isolated spacer that engages with a grounded shield in the process volume of a semiconductor process chamber. A controller adjusts the substrate support in response to deposition material on a top surface of the cover ring to maintain the shadow effect and substrate edge uniformity.
Abstract:
Methods for depositing a layer on a substrate are provided herein. In some embodiments, a method of depositing a metal-containing layer on a substrate in a physical vapor deposition (PVD) chamber may include applying RF power at a VHF frequency to a target comprising a metal disposed in the PVD chamber above the substrate to form a plasma from a plasma-forming gas; optionally applying DC power to the target; sputtering metal atoms from the target using the plasma while maintaining a first pressure in the PVD chamber sufficient to ionize a predominant portion of the sputtered metal atoms; and controlling the potential on the substrate to be the same polarity as the ionized metal atoms to deposit a metal-containing layer on the substrate.
Abstract:
Interconnect structures and methods of formation of such interconnect structures are provided herein. In some embodiments, a method of forming an interconnect includes: depositing a silicon-aluminum oxynitride (SiAlON) layer atop a first layer of a substrate, wherein the first layer comprises a first feature filled with a first conductive material; depositing a dielectric layer over the silicon-aluminum oxynitride (SiAlON) layer; and forming a second feature in the dielectric layer and the silicon-aluminum oxynitride (SiAlON) layer to expose the first conductive material.
Abstract:
The present disclosure generally relates to tin oxide films prepared by physical vapor deposition using a doped tin target. The semiconductor film may include tin and oxygen, and may be formed in a PVD chamber including a silicon doped tin target. Additionally, the semiconductor film may be smooth compared to similarly formed films without a doped target. The semiconductor film may be deposited by applying an electrical bias to a sputtering silicon doped tin target including the silicon in an amount of 0.5 to 5% by atomic weight of the total target. The semiconductor film has a smooth surface morphology compared to similarly formed tin oxide films formed without a doped target.
Abstract:
Light wave separation lattices and methods of formation are provided herein. In some embodiments, a light wave separation lattice includes a first layer having the formula ROXNY, wherein the first layer has a first refractive index; and a second layer, different from the first layer, disposed atop the first layer, and having the formula R′OXNY, wherein the second layer has a second refractive index different from the first refractive index, and wherein R and R′ are each one of a metal or a dielectric material. In some embodiments, a method of forming a light wave separation lattice includes depositing a first layer having a predetermined desired refractive index atop a substrate by a physical vapor deposition process; and depositing a second layer, different from the first layer, atop the first layer, wherein the second layer has a predetermined second refractive index different from the first refractive index.