Abstract:
A method is provided for making a FET device in which a nitride layer overlies the PFET gate structure, where the nitride layer has a compressive stress with a magnitude greater than about 2.8 GPa. This compressive stress permits improved device performance in the PFET. The nitride layer is deposited using a high-density plasma (HDP) process, wherein the substrate is disposed on an electrode to which a bias power in the range of about 50 W to about 500 W is supplied. The bias power is characterized as high-frequency power (supplied by an RF generator at 13.56 MHz). The FET device may also include NFET gate structures. A blocking layer is deposited over the NFET gate structures so that the nitride layer overlies the blocking layer; after the blocking layer is removed, the nitride layer is not in contact with the NFET gate structures. The nitride layer has a thickness in the range of about 300-2000 Å.
Abstract:
A method of processing wafers within a high density plasma chemical vapor deposition chamber comprises setting a plasma charge level within the chamber at a zero power level and, while the plasma charge level within the chamber is at the zero power level, moving a wafer into the chamber. Then, the method sets the plasma charge level to a second power level higher than zero after the wafer is moved into the chamber and performs a chemical vapor deposition process on the wafer within the chamber. After performing the chemical vapor deposition process, the method moves the wafer to a non-plasma region within the chamber. Then, after moving the wafer to the non-plasma region within the chamber, the method again sets the plasma charge level within the chamber at the zero power level. Next, after setting the plasma charge level within the chamber at the zero power level, the method opens the door of the chamber and, while the plasma charge level within the chamber is at the zero power level, the method removes the wafer from the chamber through the door of the chamber.
Abstract:
The present invention relates to a bilayer cap structure for interconnect structures that comprise copper metallization or other conductive metallization. Such bilayer cap structure includes a first cap layer formed by an unbiased high density plasma (HDP) chemical vapor deposition process, and a second cap layer over the first cap layer, where the second cap layer is formed by a biased high density plasma (bHDP) chemical vapor deposition process. During the bHDP chemical vapor deposition process, a low AC bias power is applied to the substrate to increase the ion bombardment on the substrate surface and to induce resputtering of the capping material, thereby forming a seamless second cap layer with excellent reactive ion etching (RIE) selectivity.
Abstract:
An HDP process for high aspect ratio gap filling comprises contacting a semiconductor substrate with an oxide precursor under high density plasma conditions at a first pressure less than about 10 millitorr, wherein said gaps are partially filled with oxide; and further contacting the substrate with an oxide precursor under high density plasma conditions at a second pressure greater than about 10 millitorr, wherein said gaps are further filled with oxide.
Abstract:
A method for formation of a shallow trench isolation (STI) in an active region of a device comprising trench capacitive elements, the trench capacitive elements comprising a metal plate and a high-k dielectric includes etching a STI trench in the active region of the device, wherein the STI trench is directly adjacent to at least one of the metal plate or high-k dielectric of the trench capacitive elements; and forming an oxide liner in the STI trench, wherein the oxide liner is formed selectively to the metal plate or high-k dielectric, wherein forming the oxide liner is performed at a temperature of about 600° C. or less.
Abstract:
Methods for controlling the height of semiconductor structures are disclosed. Amorphous carbon is used as a stopping layer for controlling height variability. In one embodiment, the height of replacement metal gates for transistors is controlled. In another embodiment, the step height of a shallow trench isolation region is controlled.
Abstract:
Methods for controlling the height of semiconductor structures are disclosed. Amorphous carbon is used as a stopping layer for controlling height variability. In one embodiment, the height of replacement metal gates for transistors is controlled. In another embodiment, the step height of a shallow trench isolation region is controlled.
Abstract:
Forming a shallow trench capacitor in conjunction with an FET by forming a plurality of STI trenches; for the FET, implanting a first cell well having a first polarity between a first and a second of the STI trenches; for the capacitor, implanting a second cell well having a second polarity in an area of a third of the STI trenches; removing dielectric material from the third STI trench; forming a gate stack having a first portion located between the first and the second of the STI trenches and a second portion located over and extending into the third trench; and performing a source/drain implant of the same polarity as the second cell well, thereby forming a FET in the first cell well, and a capacitor in the second cell well. The second polarity may be opposite from the first polarity. An additional implant may reduce ESR in the second cell well.
Abstract:
Embodiments of the invention provide a method of forming a compressive stress nitride film overlying a plurality of p-type field effect transistor gate structures produced on a substrate through a high-density plasma deposition process. Embodiments include generating an environment filled with high-density plasma using source gases of at least silane, argon and nitrogen; biasing the substrate to a high frequency power of varying density, in a range between 0.8 W/cm2 and 5.0 W/cm2; and depositing the high-density plasma to the plurality of gate structures to form the compressive stress nitride film.
Abstract translation:本发明的实施例提供一种通过高密度等离子体沉积工艺形成在衬底上产生的多个p型场效应晶体管栅极结构的压应力氮化物膜的形成方法。 实施例包括使用至少硅烷,氩和氮的源气体产生填充有高密度等离子体的环境; 在0.8W / cm 2至5.0W / cm 2之间的范围内将衬底偏置为变化密度的高频功率; 以及将所述高密度等离子体沉积到所述多个栅极结构以形成所述压应力氮化物膜。
Abstract:
A structure comprises at least one transistor on a substrate, an insulator layer over the transistor, and an ion stopping layer over the insulator layer. The ion stopping layer comprises a portion of the insulator layer that is damaged and has either argon ion damage or nitrogen ion damage.