Abstract: A sputtering process and magnetron especially advantageous for low-pressure plasma sputtering or sustained self-sputtering, in which the magnetron has a reduced area but full target coverage. The magnetron includes an outer pole face surrounding an inner pole face with a gap therebetween. The outer pole of the magnetron of the invention is smaller than that of a circular magnetron similarly extending from the center to the periphery of the target and has a substantially larger total magnetic intensity. Thereby, sputtering at low pressure and high ionization fraction is enabled.

Abstract: A metal/metal nitride barrier layer for semiconductor device applications. The barrier layer is particularly useful in contact vias where high conductivity of the via is important, and a lower resistivity barrier layer provides improved overall via conductivity.

Abstract: A plasma cleaning method particularly useful for removing photoresist and oxide residue from a porous low-k dielectric with a high carbon content prior to sputter deposition. A remote plasma source produces a plasma primarily of hydrogen radicals. The hydrogen pressure may be kept relatively low, for example, at 30 milliTorr. Optionally, helium may be added to the processing gas with the hydrogen partial pressure held below 150 milliTorr. Superior results are obtained with 70% helium in 400 milliTorr of hydrogen and helium. Preferably, an ion filter, such as a magnetic filter, removes hydrogen and other ions from the output of the remote plasma source and a supply tube from the remote plasma source includes a removable dielectric liner in combination with dielectric showerhead and manifold liner.

Abstract: An apparatus and a method of cleaning a dielectric film are provided in the present invention. In one embodiment, an apparatus of cleaning a dielectric film the apparatus includes a chamber body adapted to support a substrate therein, a remote plasma source adapted to provide a plurality of reactive radicals to the chamber body, a passage coupling the remote plasma source to the chamber body, and at least one magnet disposed adjacent the passage. In another embodiment, a method of cleaning a dielectric film that includes providing a substrate having an at least partially exposed dielectric layer disposed in a process chamber, generating a plurality of reactive radicals in a remote plasma source, flowing the reactive radicals from the remote plasma source into the process chamber through a passage having at least one magnet disposed adjacent the passage, and magnetically filtering the reactive radicals passing through the passage.

Abstract: One aspect of the invention includes an auxiliary magnet ring positioned outside of the chamber wall of a plasma sputter reactor and being disposed at least partially radially outwardly of an RF coil used to inductively generate a plasma, particularly for sputter etching the substrate being sputter deposited. Thereby, a magnetic barrier prevents the plasma from leaking outwardly to the coil and improves the uniformity of sputter etching. The magnetic field also acts as a magnetron when the coil, when made of the same material as the primary target, is being used as a secondary target. Another aspect of the invention includes a one-piece inner shield extending from the target to the pedestal with a smooth inner surface and supported by an annular flange in a middle portion of the shield. The shield may be used to support the RF coil.

Abstract: A sputtering coil for a plasma chamber in a semiconductor fabrication system is provided. The sputtering coil couples energy into a plasma and also provides a source of sputtering material to be sputtered onto a workpiece from the coil to supplement material being sputtered from a target onto the workpiece. Alternatively a plurality of coils may be provided, one primarily for coupling energy into the plasma and the other primarily for providing a supplemental source of sputtering material to be sputtered on the workpiece.

Abstract: We have discovered a method of providing a thin approximately from about 2 ? to about 100 ? thick TaN seed layer, which can be used to induce the formation of alpha tantalum when tantalum is deposited over the TaN seed layer. Further, the TaN seed layer exhibits low resistivity, in the range of 30 ?? cm and can be used as a low resistivity barrier layer in the absence of an alpha tantalum layer. In one embodiment of the method, a TaN film is altered on its surface form the TaN seed layer. In another embodiment of the method, a Ta film is altered on its surface to form the TaN seed layer.

Abstract: A multi-step process performed in a plasma sputter chamber including sputter deposition from the target and argon sputter etching of the substrate. The chamber includes a quadruple electromagnetic coil array coaxially arranged in a rectangular array about a chamber axis outside the sidewalls of a plasma sputter reactor in back of an RF coil within the chamber. The coil currents can be separately controlled to produce different magnetic field distributions, for example, between a sputter deposition mode in which the sputter target is powered to sputter target material onto a wafer and a sputter etch mode in which the RF coil supports the argon sputtering plasma. A TaN/Ta barrier is first sputter deposited with high target power and wafer bias. Argon etching is performed with even higher wafer bias. A flash step is applied with reduced target power and wafer bias.

Abstract: A magnetron sputter reactor for sputtering deposition materials such as tantalum, tantalum nitride and copper, for example, and its method of use, in which self-ionized plasma (SIP) sputtering and inductively coupled plasma (ICP) sputtering are promoted, either together or alternately, in the same or different chambers. Also, bottom coverage may be thinned or eliminated by ICP resputtering in one chamber and SIP in another. SIP is promoted by a small magnetron having poles of unequal magnetic strength and a high power applied to the target during sputtering. ICP is provided by one or more RF coils which inductively couple RF energy into a plasma. The combined SIP-ICP layers can act as a liner or barrier or seed or nucleation layer for hole. In addition, an RF coil may be sputtered to provide protective material during ICP resputtering. In another chamber an array of auxiliary magnets positioned along sidewalls of a magnetron sputter reactor on a side towards the wafer from the target.

Abstract: A first method is provided for forming a barrier layer on a substrate by sputter-depositing a tantalum nitride layer on a substrate having (1) a metal feature formed on the substrate; (2) a dielectric layer formed over the metal feature; and (3) a via formed in the dielectric layer so as to expose the metal feature. The via has side walls and a bottom, and a width of about 0.18 microns or less. The tantalum nitride layer is deposited on the side walls and bottom of the via and on a field region of the dielectric layer; and has a thickness of at least about 200 angstroms on the field region. The first method also includes sputter-depositing a tantalum layer on the substrate, in the same chamber. The tantalum layer having a thickness of less than about 100 angstroms on the field region. Other aspects are provided.

Abstract: A magnetron sputter reactor for sputtering deposition materials such as nickel and cobalt, for example, and its method of use, in which self-ionized plasma (SIP) sputtering is promoted. SIP is promoted by a small magnetron having poles of unequal magnetic strength and a high power applied to the target during sputtering. One embodiment of the present inventions is directed to sputter depositing a metal layer by biasing a sputter target with pulsed power in which the power applied to the target alternates between low and high levels. The high levels are, in one embodiment, sufficiently high to maintain a plasma for ionizing deposition material. The low levels are, in one embodiment, sufficiently low such that the power applied to the target during the high and low levels is, on average, low enough to facilitate deposition of thin layers if desired.

Abstract: We have discovered a method of providing a thin, approximately from about 2 ? to about 100 ? thick TaN seed layer, which can be used to induce the formation of alpha tantalum when tantalum is deposited over the TaN seed layer. Further, the TaN seed layer exhibits low resistivity, in the range of 30 ??cm and can be used as a low resistivity barrier layer in the absence of an alpha tantalum layer. In one embodiment of the method, a TaN film is altered on its surface to form the TaN seed layer. In another embodiment of the method, a Ta film is altered on its surface to form the TaN seed layer.

Abstract: A one-piece inner shield usable in a plasma sputter reactor and extending from the target to the pedestal with a smooth inner surface and supported by an annular flange in a middle portion of the shield. The shield may be used to support the RF coil used in exciting the plasma. An outer shield includes an outwardly extending flange on its end alignable with the inner shield flange, holes in correspondence to recesses in the inner shield for standoffs for the RF coil, and circumferentially arranged gas flow holes.

Abstract: A first method is provided for forming a barrier layer on a substrate by sputter-depositing a tantalum nitride layer on a substrate having (1) a metal feature formed on the substrate; (2) a dielectric layer formed over the metal feature; and (3) a via formed in the dielectric layer so as to expose the metal feature. The via has side walls and a bottom, and a width of about 0.18 microns or less. The tantalum nitride layer is deposited on the side walls and bottom of the via and on a field region of the dielectric layer; and has a thickness of at least about 200 angstroms on the field region. The first method also includes sputter-depositing a tantalum layer on the substrate, in the same chamber. The tantalum layer having a thickness of less than about 100 angstroms on the field region. Other aspects are provided.

Abstract: Plasma etching or resputtering of a layer of sputtered materials including opaque metal conductor materials may be controlled in a sputter reactor system. In one embodiment, resputtering of a sputter deposited layer is performed after material has been sputtered deposited and while additional material is being sputter deposited onto a substrate. A path positioned within a chamber of the system directs light or other radiation emitted by the plasma to a chamber window or other optical view-port which is protected by a shield against deposition by the conductor material. In one embodiment, the radiation path is folded to reflect plasma light around the chamber shield and through the window to a detector positioned outside the chamber window.

Abstract: A sputtering process and magnetron especially advantageous for low-pressure plasma sputtering or sustained self-sputtering, in which the magnetron has a reduced area but full target coverage. The magnetron includes an outer pole face surrounding an inner pole face with a gap therebetween. The outer pole of the magnetron of the invention is smaller than that of a circular magnetron similarly extending from the center to the periphery of the target and has a substantially larger total magnetic intensity. Thereby, sputtering at low pressure and high ionization fraction is enabled.

Abstract: A magnetron sputter reactor (410) and its method of use, in which SIP sputtering and ICP sputtering are promoted is disclosed. In another chamber (412) an array of auxiliary magnets positioned along sidewalls (414) of a magnetron sputter reactor on a side towards the wafer from the target is disclosed. The magnetron (436) preferably is a small one having a stronger outer pole (442) of a first polarity surrounding a weaker inner pole (440) of a second polarity all on a yoke (444) and rotates about the axis (438) of the chamber using rotation means (446, 448, 450). The auxiliary magnets (462) preferably have the first polarity to draw the unbalanced magnetic field (460) towards the wafer (424), which is on a pedestal (422) supplied with power (454). Argon (426) is supplied through a valve (428). The target (416) is supplied with power (434).

Abstract: A sputtering coil for a plasma chamber in a semiconductor fabrication system is provided. The sputtering coil couples energy into a plasma and also provides a source of sputtering material to be sputtered onto a workpiece from the coil to supplement material being sputtered from a target onto the workpiece. Alternatively a plurality of coils may be provided, one primarily for coupling energy into the plasma and the other primarily for providing a supplemental source of sputtering material to be sputtered on the workpiece.

Abstract: A sputtering coil for a plasma chamber in a semiconductor fabrication system is provided. The sputtering coil couples energy into a plasma and also provides a source of sputtering material to be sputtered onto a workpiece from the coil to supplement material being sputtered from a target onto the workpiece. Alternatively a plurality of coils may be provided, one primarily for coupling energy into the plasma and the other primarily for providing a supplemental source of sputtering material to be sputtered on the workpiece.

Abstract: One aspect of the invention includes an auxiliary magnet ring positioned outside of the chamber wall of a plasma sputter reactor and being disposed at least partially radially outwardly of an RF coil used to inductively generate a plasma, particularly for sputter etching the substrate being sputter deposited. Thereby, a magnetic barrier prevents the plasma from leaking outwardly to the coil and improves the uniformity of sputter etching. The magnetic field also acts as a magnetron when the coil, when made of the same material as the primary target, is being used as a secondary target. Another aspect of the invention includes a one-piece inner shield extending from the target to the pedestal with a smooth inner surface and supported by an annular flange in a middle portion of the shield. The shield may be used to support the RF coil.