Abstract: Embodiments of the present invention relate to the use of a particle accelerator beam to form thin films of material from a bulk substrate. In particular embodiments, a bulk substrate having a top surface is exposed to a beam of accelerated particles. Then, a thin film of material is separated from the bulk substrate by performing a controlled cleaving process along a cleave region formed by particles implanted from the beam. To improve uniformity of depth of implantation, channeling effects are reduced by one or more techniques. In one technique, a miscut bulk substrate is subjected to the implantation, such that the lattice of the substrate is offset at an angle relative to the impinging particle beam. According to another technique, the substrate is tilted at an angle relative to the impinging particle beam. In still another technique, the substrate is subjected to a dithering motion during the implantation. These techniques may be employed alone or in combination.

Abstract: Embodiments of the present invention relate to the use of a particle accelerator beam to form thin films of material from a bulk substrate. In particular embodiments, a bulk substrate having a top surface is exposed to a beam of accelerated particles. Then, a thin film of material is separated from the bulk substrate by performing a controlled cleaving process along a cleave region formed by particles implanted from the beam. To improve uniformity of depth of implantation, channeling effects are reduced by one or more techniques. In one technique, a miscut bulk substrate is subjected to the implantation, such that the lattice of the substrate is offset at an angle relative to the impinging particle beam. According to another technique, the substrate is tilted at an angle relative to the impinging particle beam. In still another technique, the substrate is subjected to a dithering motion during the implantation. These techniques may be employed alone or in combination.

Abstract: Apparatus characterizes the quality of microelectronic features using broadband white light. A highly collimated light source illuminates an area of a first wafer using broadband multi-spectral light. The angular distribution of the light scattered from the first wafer is then measured. Generally, the angle of the light source, detector, or both is altered and an angular distribution measurement taken at each angle, producing a scatter signature for the first wafer. Finally, the scatter signature of the first wafer is compared with a known scatter signature of a second wafer of good quality to determine the quality of the first wafer.

Abstract: Apparatus characterizes the quality of microelectronic features using broadband white light. A highly collimated light source illuminates an area of a first wafer using broadband multi-spectral light. The angular distribution of the light scattered from the first wafer is then measured. Generally, the angle of the light source, detector, or both is altered and an angular distribution measurement taken at each angle, producing a scatter signature for the first wafer. Finally, the scatter signature of the first wafer is compared with a known scatter signature of a second wafer of good quality to determine the quality of the first wafer.

Abstract: Disclosed is a method for characterizing the quality of microelectronic features using broadband white light. A highly collimated light source illuminates an area of a first wafer using broadband multi-spectral light. The angular distribution of the light scattered from the first wafer is then measured. Generally, the angle of the light source, detector, or both is altered and an angular distribution measurement taken at each angle, producing a scatter signature for the first wafer. Finally, the scatter signature of the first wafer is compared with a known scatter signature of a second wafer of good quality to determine the quality of the first wafer.

Abstract: A method and apparatus for controlling deposit build-up on an interior surface of a dielectric member of a plasma processing chamber. The deposit build-up is controlled by selective ion bombardment of the inner surface by shifting location of a peak voltage amplitude of a voltage standing wave on an antenna such as a flat spiral coil of the plasma processing chamber. A region of high ion bombardment on the interior surface of the dielectric member is displaced by controlling the value of a termination capacitance over a range of values causing regions of low and high ion bombardment to move over the dielectric member in order to effect cleaning thereof.

Abstract: A method and apparatus for controlling deposit build-up on an interior surface of a dielectric member of a plasma processing chamber. The deposit build-up is controlled by selective ion bombardment of the inner surface by shifting location of a peak voltage amplitude of a voltage standing wave on an antenna such as a flat spiral coil of the plasma processing chamber. A region of high ion bombardment on the interior surface of the dielectric member is displaced by controlling the value of a termination capacitance over a range of values causing regions of low and high ion bombardment to move over the dielectric member in order to effect cleaning thereof.

Abstract: A plasma processing chamber includes a substrate holder, a gas distribution member, and a shield for preventing lightup of plasma in gas distribution holes in the gas distribution member. The chamber can include an RF energy source such as an RF antenna which inductively couples RF energy through the gas distribution member to energize process gas into a plasma state. The shield can be arranged to allow capacitive coupling of RF energy into the processing chamber for lightup of plasma in the processing chamber and/or ion bombardment of the exposed surface of the gas distribution member for cleaning thereof during processing of the substrate.

Abstract: The laser (10) has a crystal modulator (22) located at one end (16) of the laser gain medium (12) opposite the end (14) to which the total reflector or grating (18) is attached. The outcoupler (28) is spaced a predetermined nonzero distance apart from the edge (30) of the crystal (22). The spacing (d) is selected to overcome and compensate for distortions caused by thermal lensing effects in the crystal (22).