Abstract: An apparatus may include an electrostatic filter having a plurality of electrodes; a voltage supply assembly coupled to the plurality of electrodes; a cleaning ion source disposed between the electrostatic filter and a substrate position, the cleaning ion source generating a plasma during a cleaning mode, wherein a dose of ions exit the cleaning ion source; and a controller having a first component to generate a control signal for controlling the voltage supply assembly, wherein a negative voltage is applied to at least one of the plurality of electrodes when the plasma is generated.

Abstract: Provided herein are approaches for controlling particle trajectory from a beam-line electrostatic element. In an exemplary approach, a beam-line electrostatic element is disposed along a beam-line of an electrostatic filter (EF), and a voltage is supplied to the beam-line electrostatic element to generate an electrostatic field surrounding the beam-line electrostatic element, agitating a layer of contamination particles formed on the beam-line electrostatic element. A trajectory of a set of particles from the layer of contamination particles is then modified to direct the set of particles to a desired location within the EF. In one approach, the trajectory is controlled by providing an additional electrode adjacent the beam-line electrostatic element, and supplying a voltage to the additional electrode to control a local electrostatic field in proximity to the beam-line electrostatic element.

Abstract: The IHC ion source comprises an ion source chamber having a cathode and a repeller on opposite ends. The repeller is made of two discrete parts, each comprising a different material. The repeller includes a repeller head, which may be a disc shaped component, and a stem to support the head. The repeller head is made from a conductive material having a higher thermal conductivity than the stem. In this way, the temperature of the repeller head is maintained at a higher temperature than would otherwise be possible. The higher temperature limits the build-up of material on the repeller head, which improves the performance of the IHC ion source. In certain embodiments, the repeller head and the stem are connected using a press fit. Differences in the coefficient of thermal expansion of the repeller head and the stem may cause the press fit to become tighter at higher temperatures.

Abstract: An apparatus may include an ion source generating an ion beam, the ion source coupled to a first voltage. The apparatus may further include a stopping element disposed between the ion source and a substrate position; a stopping voltage supply coupled to the stopping element; and a control component to direct the stopping voltage supply to apply a stopping voltage to the stopping element, the stopping voltage being equal to or more positive than the first voltage when the ion beam comprises positive ions, and being equal to or more negative than the first voltage when the ion beam comprises negative ions, wherein at least a portion of the ion beam is deflected backwardly from an initial trajectory as deflected ions when the stopping voltage is applied to the stopping element.

Abstract: Provided herein are approaches for controlling a charged particle beam using a series of electrodes including a plurality of different shapes. In one approach, an electrostatic optical element includes a first set of electrodes having a first electrode shape for parallelizing and deflecting the charged particle beam using a first set of electrodes having a first electrode shape, such as a concave or convex profile. The electrostatic optical element further includes a second set of electrodes adjacent the first set of electrodes for accelerating or decelerating the charged particle beam along a beamline, wherein the second set of electrodes include a cylindrical shape. In one approach, a power supply is electrically connected to the first and second sets of electrodes, the power supply arranged to enable independent voltage/current control.

Abstract: An electrostatic clamp (ESC) has a clamping surface, and first and second pairs of electrodes. Each of the first pair of electrodes are associated with a respective third of the clamping surface, and each of the second pair of electrodes are associated with a respective sixth of the clamping surface. A peripheral region of each of the first and second pairs of electrodes spirals toward the periphery of the clamping surface. A DC mode connects one of each of the first and second pair of electrodes to a positive and the other one of the respective first and second pair of electrodes to a negative of a power supply. An AC mode electrically connects first, second, and third phase terminals of the power supply to one of the first pair of electrodes, the other one of the first pair of electrodes, and both of the second pair of electrodes, respectively.

Abstract: A platen having different grounding structures is disclosed. Different grounding structures, such as pins, flat-end posts and mushroom-shaped grounding structures, may be disposed on the surface of a platen. Each type of grounding structure may be advantageously used with a particular type of workpiece. In one embodiment, all of the different grounding structures are mechanically biased upward, such as by springs, from the surface of the platen such that all may contact the back surface of a workpiece disposed on the platen. In another embodiment, one or more actuators are used to lift and lower subsets of the grounding structures such that only a subset of the grounding structures contacts the back surface of the workpiece. These subsets may be all a single type of grounding structure, or may be associated with a particular type of workpiece.

Abstract: Provided herein are approaches for in-situ plasma cleaning of one or more components of an ion implantation system. In one approach, the component may include a beam-line component having a conductive beam optic, the beam optic having a varied geometry configured to generate a concentrated electric field proximate the beam optic. The system further includes a power supply for supplying a first voltage and first current to the component during a processing mode and a second voltage and second current to the component during a cleaning mode. The second voltage and current may be applied to the one or more beam optics, in parallel, to selectively (e.g., individually) generate plasma in an area corresponding to the concentrated electric field. By providing custom-shaped ion beam optics, plasma density is strategically enhanced in areas where surface contamination is most prevalent, thus improving cleaning efficiency and minimizing tool down time.

Abstract: Methods for processing of a workpiece are disclosed. A fluid that contains a desired dopant is prepared. The workpiece is immersed in this fluid, such that the dopant is able to contact all surfaces of the workpiece. The fluid is then evacuated, leaving behind the dopant on the workpiece. The dopant is then subjected to a thermal treatment to drive the dopant into the surfaces of the workpiece. In certain embodiments, a selective doping process may be performed by applying a mask to certain surfaces prior to immersing the workpiece in the fluid. In certain embodiments, the fluid may be in a super-critical state to maximize the contact between the dopant and the workpiece.

Abstract: An apparatus, referred to as a light bath, is disposed in a beamline ion implantation system and is used to photoionize particles in the ion beam into positively charged particles. Once positively charged, these particles can be manipulated by the various components in the beamline ion implantation system. In certain embodiments, a positively biased electrode is disposed downstream from the light bath to repel the formerly non-positively charged particles away from the workpiece. In certain embodiments, the light bath is disposed within an existing component in the beamline ion implantation system, such as a deceleration stage or a Vertical Electrostatic Energy Filter. The light source emits light at a wavelength sufficiently short so as to ionize the non-positively charged particles. In certain embodiments, the wavelength is less than 250 nm.

Abstract: An apparatus, referred to as a light bath, is disposed in a beamline ion implantation system and is used to photoionize particles in the ion beam into positively charged particles. Once positively charged, these particles can be manipulated by the various components in the beamline ion implantation system. In certain embodiments, a positively biased electrode is disposed downstream from the light bath to repel the formerly non-positively charged particles away from the workpiece. In certain embodiments, the light bath is disposed within an existing component in the beamline ion implantation system, such as a deceleration stage or a Vertical Electrostatic Energy Filter. The light source emits light at a wavelength sufficiently short so as to ionize the non-positively charged particles. In certain embodiments, the wavelength is less than 250 nm.

Abstract: Provided herein are approaches for controlling particle trajectory from a beam-line electrostatic element. In an exemplary approach, a beam-line electrostatic element is disposed along a beam-line of an electrostatic filter (EF), and a voltage is supplied to the beam-line electrostatic element to generate an electrostatic field surrounding the beam-line electrostatic element, agitating a layer of contamination particles formed on the beam-line electrostatic element. A trajectory of a set of particles from the layer of contamination particles is then modified to direct the set of particles to a desired location within the EF. In one approach, the trajectory is controlled by providing an additional electrode adjacent the beam-line electrostatic element, and supplying a voltage to the additional electrode to control a local electrostatic field in proximity to the beam-line electrostatic element.

Abstract: Systems and methods for the selective processing of a particular portion of a workpiece are disclosed. For example, the outer portion may be processed by directing an ion beam toward a first position on the workpiece, where the ion beam extends beyond the outer edge of the workpiece at two first locations. The workpiece is then rotated relative to the ion beam about its center so that certain regions of the outer portion are exposed to the ion beam. The workpiece is then moved relative to the ion beam to a second position and rotated in the opposite direction so that all regions of the outer portion are exposed to the ion beam. This process may be repeated a plurality of times. The ion beam may perform any process, such as ion implantation, etching or deposition.

Abstract: Provided herein are approaches for in-situ plasma cleaning of one or more components of an ion implantation system. In one approach, the component may include a beam-line component having one or more conductive beam optics. The system further includes a power supply for supplying a first voltage and first current to the component during a processing mode and a second voltage and second current to the component during a cleaning mode. The second voltage and current may be applied to the conductive beam optics of the component, in parallel, to selectively (e.g., individually) generate plasma around one or more of the one or more conductive beam optics. The system may further include a flow controller for adjusting an injection rate of an etchant gas supplied to the component, and a vacuum pump for adjusting pressure of an environment of the component.

Abstract: An apparatus may include an extraction assembly comprising at least a first extraction aperture and second extraction aperture, the extraction assembly configured to extract at least a first ion beam and second ion beam from a plasma; a target assembly disposed adjacent the extraction assembly and including at least a first target portion comprising a first material and a second target portion comprising a second material, the first target portion and second target portion being disposed to intercept the first ion beam and second ion beam, respectively; and a substrate stage disposed adjacent the target assembly and configured to scan a substrate along a scan axis between a first point and a second point, wherein the first target portion and second target portion are separated from the first point by a first distance and second distance, respectively, the first distance being less than the second distance.

Abstract: An apparatus for creating an angled ion beam for implanting into a substrate is disclosed. The apparatus includes a plasma chamber in which plasma is created. The extraction aperture includes a plurality of rotatable plates. Ion beamlets are extracted through apertures defined by the plurality of rotatable plates. The degree to which these plates are rotated determines the angle of extraction for the extracted ion beam. These plates may be formed in a plurality of different shapes, which may increase the maximum extraction angle that is achievable. Additionally, electrodes may be disposed near the plates to affect the extraction angle.

Abstract: Methods for the selective processing of the outer portion of a workpiece are disclosed. The outer portion is processed by directing an ion beam toward the workpiece, where the ion beam extends beyond the outer edge of the workpiece at two locations. The workpiece is then rotated relative to the ion beam about the center so that all regions of the outer portion are exposed to the ion beam. The workpiece may be rotated an integral number of rotations. The ion beam may perform any process, such as ion implantation, etching or deposition. The outer portion may be an annular ring having an outer diameter equal to that of the workpiece and having a width of 1 to 30 millimeters. The rotation of the workpiece may be aligned with a notch on the outer edge of the workpiece.

Abstract: An apparatus for creating an angled ion beam for implanting into a substrate is disclosed. The apparatus includes a plasma chamber in which plasma is created. The extraction aperture includes a plurality of rotatable plates. Ion beamlets are extracted through apertures defined by the plurality of rotatable plates. The degree to which these plates are rotated determines the angle of extraction for the extracted ion beam. These plates may be formed in a plurality of different shapes, which may increase the maximum extraction angle that is achievable. Additionally, electrodes may be disposed near the plates to affect the extraction angle.

Abstract: An improved method of etching a metal substrate is described. After a mask layer is applied to the metal substrate, an ion implantation process is performed which implants ions, such as oxygen ions, into the exposed regions of the metal substrate. This implantation creates regions of metal oxide, which may be more susceptible to etching. Afterwards, the exposed regions of metal oxide are subjected to an etching process. This process may be through vaporization or may be a wet etch process. In some embodiments, the etchant is selected so that the metal oxide binds with the etchant to form a volatile compound, which stays in the vapor or gaseous state. This may reduce the unwanted deposition of the metal to other surfaces. These ion implantation and etching processes may be repeated a plurality of times to create a recessed feature of the desired depth.

Abstract: Systems and methods for the production of laser induced high mass molecular borane is disclosed for an ion implantation system. The system comprises a laser, a diborane gas source, a heated interaction chamber for generating a high mass molecular borane, a transport system for transferring the high mass molecular borane, and an ion source chamber for generating an ion beam in an ion beam path for implantation of a workpiece. The transport system comprises at least a first and a second flow control component at least a first heated chamber, wherein the first heated chamber is disposed between the first and second flow control components, and wherein the first heated chamber is configured to condense the high mass molecular borane. The laser comprises a CO2 laser configured to irradiate the diborane source gas at a wavelength of about 10.6 ?m at a R-16 (973 cm?1) line of excitation.