Abstract:
A beam control assembly to shape a ribbon beam of ions for ion implantation includes a first bar, second bar, first coil of windings of electrical wire, second coil of windings of electrical wire, first electrical power supply, and second electrical power supply. The first coil is disposed on the first bar. The first coil is the only coil disposed on the first bar. The second bar is disposed opposite the first bar with a gap defined between the first and second bars. The ribbon beam travels between the gap. The second coil is disposed on the second bar. The second coil is the only coil disposed on the second bar. The first electrical power supply is connected to the first coil without being electrically connected to any other coil. The second electrical power supply is connected to the second coil without being electrically connected to any other coil.
Abstract:
A finFET is formed having a fin with a source region, a drain region, and a channel region between the source and drain regions. The fin is etched on a semiconductor wafer. A gate stack is formed having an insulating layer in direct contact with the channel region and a conductive gate material in direct contact with the insulating layer. The source and drain regions are etched leaving the channel region of the fin. Epitaxial semiconductor is grown on the sides of the channel region that were adjacent the source and drain regions to form a source epitaxy region and a drain epitaxy region. The source and drain epitaxy regions are doped in-situ while growing the epitaxial semiconductor.
Abstract:
A variable aperture within an aperture device is used to shape the ion beam before the substrate is implanted by shaped ion beam, especially to finally shape the ion beam in a position right in front of the substrate. Hence, different portions of a substrate, or different substrates, can be implanted respectively by different shaped ion beams without going through using multiple fixed apertures or retuning the ion beam each time. In other words, different implantations may be achieved respectively by customized ion beams without high cost (use multiple fixed aperture devices) and complex operation (retuning the ion beam each time). Moreover, the beam tune process for acquiring a specific ion beam to be implanted may be accelerated, to be faster than using multiple fixed aperture(s) and/or retuning the ion beam each time, because the adjustment of the variable aperture may be achieved simply by mechanical operation.
Abstract:
A gas mixture method and apparatus of prolonging lifetime of an ion source for generating an ion beam particularly an ion beam containing carbon is proposed here. By mixing the dopant gas and the minor gas together to generate an ion beam, undesired reaction between the gas species and the ion source can be mitigated and thus lifetime of the ion source can be prolonged. Accordingly, quality of ion beam can be maintained.
Abstract:
A scan head assembled to a scan arm for an ion implanter and a scan arm using the same are provided, wherein the scan head is capable of micro tilting a work piece and comprises a case, a shaft assembly, an electrostatic chuck, a first driving mechanism and a micro-tilt mechanism. The shaft assembly passes through a first side of the case and has a twist axis. The electrostatic chuck is fastened on a first end of the shaft assembly outside the case for holding the work piece. The first driving mechanism is disposed within the case and capable of driving the shaft assembly and the ESC to rotate about the twist axis. The micro-tilt mechanism is disposed within the case and capable of driving the shaft assembly and the ESC to tilt relative to the case.
Abstract:
An ion implanter and an ion implant method are disclosed. Essentially, the wafer is moved along one direction and an aperture mechanism having an aperture is moved along another direction, so that the projected area of an ion beam filtered by the aperture is two-dimensionally scanned over the wafer. Thus, the required hardware and/or operation to move the wafer may be simplified. Further, when a ribbon ion beam is provided, the shape/size of the aperture may be similar to the size/shape of a traditional spot beam, so that a traditional two-dimensional scan may be achieved. Optionally, the ion beam path may be fixed without scanning the ion beam when the ion beam is to be implanted into the wafer, also the area of the aperture may be adjustable during a period of moving the aperture across the ion beam.
Abstract:
This invention discloses an ion implantation apparatus that has an ion source and an ion extraction means for extracting an ion beam therefrom. The ion implantation apparatus further includes an ion beam sweeping-and-deflecting means disposed immediately next to the ion extraction means. The ion implantation apparatus further includes a magnetic analyzer for guiding the ion beam passed through the deflecting-and-sweeping means. The mass analyzer is also used for selecting ions with specific mass-to-charge ratio to pass through a mass slit to project onto a substrate. The sweeping-and-deflecting means is applied to deflect the ion beam to project through the magnetic mass analyzer and the mass slit for sweeping the ion beam over a surface of the substrate to carry out an ion implantation. In a preferred embodiment, the ion implantation apparatus further includes a plasma electron flood system disposed between the mass slit and the substrate for projecting a plurality of electrons to the ion beam for preventing a space-charge and beam dispersion. In another preferred embodiment, the ion beam extraction and projecting system of this invention further includes a divergent ion-beam extracting optics for extracting an ion beam with a small divergent angle for projecting and diverging the ion beam as the ion beam is projected toward the target surface.
Abstract:
The present disclosure relates generally to ion implantation, and more particularly, to systems and processes for adjusting a ribbon beam angle of an ion implantation system. An exemplary ion implantation system includes an ion source configured to generate a ribbon beam, a wafer chuck configured to hold a wafer during implantation by the ribbon beam, a dipole magnet disposed between the ion source and the wafer chuck, and a controller. The dipole magnet includes at least two coils configured to adjust a ribbon beam angle of the ribbon beam at one or more locations along a path of the ribbon beam between the ion source and the wafer held in the wafer chuck. The controller is configured to control the ion source, the wafer chuck, and the dipole magnet.
Abstract:
The present disclosure relates generally to ion implantation, and more particularly, to systems and processes for measuring the temperature of a wafer within an ion implantation system. An exemplary ion implantation system may include a robotic arm, one or more load lock chambers, a pre-implantation station, an ion implanter, a post-implantation station, and a controller. The pre-implantation station is configured to heat or cool a wafer prior to the wafer being implanted with ions by the ion implanter. The post-implantation station is configured to heat or cool a wafer after the wafer is implanted with ions by the ion implanter. The pre-implantation station and/or post-implantation station are further configured to measure a current temperature of a wafer. The controller is configured to control the various components and processes described above, and to determine a current temperature of a wafer based on information received from the pre-implantation station and/or post-implantation station.
Abstract:
The disclosure provides a hybrid magnet structure which includes two dipole magnets assemblies arranged oppositely, and each dipole magnet assembly includes a permanent magnet, two iron cores, and a moveable magnetic field shunt element. The hybrid magnet structure is adapted to focus particle beams of different positions by applying an adjustable gradient magnetic field in the horizontal or vertical direction of the particle beam. By passing the charged particle beams through the gradient magnetic field established between the two dipole magnets, the aspect of focusing the charged particle beam is achieved. In addition, the intensity of the gradient magnetic field can be altered by adjusting the gap between the movable magnetic field shunt element and the permanent magnet, thereby controlling the particle beam size on a specific axis for different energies or masses of the charge particles.