Abstract:
Techniques for ion beam current measurement, especially for measuring low energy ion beam current, are disclosed. In one exemplary embodiment, the techniques may be realized as an ion beam current measurement apparatus has at least a planar Faraday cup and a magnet device. The planar Faraday cup is close to an inner surface of a chamber wall, and may be non-parallel to or parallel to the inner surface. The magnet device is located close to the planar Faraday cup. Therefore, by properly adjusting the magnetic field, secondary electrons, incoming electrons and low energy ions may be adequately suppressed. Further, the planar Faraday cup may surround an opening of an additional Faraday cup being any conventional Faraday cup. Therefore, the whole ion beam may be received and measured well by the larger cross-section area of at least the planar Faraday cup on the ion beam path.
Abstract:
Apparatus and method for adjusting an ion beam between a mass analyzer and a substrate holder. Herein, one or more bended, such as arch-shaped, curved or zigzag shaped, bar magnets are configured to apply one or more magnetic fields to adjust the shape or cross section of an ion beam passing through a space partially surrounded by the one or more bended bar magnets. At least one of the gap width between neighbor bended bar magnets, the curvature of each bended bar magnet and the current flowing through each bended bar magnet may be fixed or adjusted dependently or independently. Therefore, the Lorentz force applied on the ion beam along different directions may be changed in a desired manner, and then the ion beam may be flexibly elongated, compressed or shaped to meet the process requirement.
Abstract:
A deceleration apparatus capable of decelerating a short spot beam or a tall. ribbon beam is disclosed. In either case, effects tending to degrade the shape of the beam profile are controlled. Caps to shield the ion beam from external potentials are provided. Electrodes whose position and potentials are adjustable are provided, on opposite sides of the beam, to ensure that the shape of the decelerating and deflecting electric fields does not significantly deviate from the optimum shape, even in the presence of the significant space-charge of high current low-energy beams of heavy ions.
Abstract:
An ion implanter and method for adjusting the shape of an ion beam are disclosed. After an ion beam is outputted from an analyzer magnet unit, at least one set of bar magnets is used to adjust the shape of the ion beam when the ion beam passes through a space enclosed by the bar magnets. The set of bar magnets can apply a multi-stage magnetic field on the ion beam. Hence, different portions of the ion beam will have different deformations or alterations, because the multi-stage magnetic field will apply a non-uniform force to change the trajectory of ions. Moreover, each bar magnet of the set is powered by one and only one power source, such that the set of bar magnets essentially only can adjust the magnitude of the multi-stage magnetic field. Particular structures and techniques for achieving the multi-stage magnetic field are not limited.
Abstract:
A thin film deposition apparatus and method are disclosed in this invention. The apparatus includes a depositing thin-film particle source, a beam-defining aperture between the particle source and the deposited substrate(s), and a substrate holder to rotate the substrate(s) around its center and move the center along a lateral path so that the substrate(s) can scan across the particle beam from one substrate edge to the other edge. The method includes a step of providing a vacuum chamber for containing a thin-film particle source for generating thin-film particles to deposit a thin-film on the substrates. The method further includes a step of containing a substrate holder in the vacuum chamber for holding a plurality of substrates having a thin-film deposition surface of each substrate facing the beam of thin-film particles. The method further includes a step of providing a rotational means for rotating the substrate holder to rotate each of the substrates exposed to the thin-film particles for depositing a thin film thereon. And, the method further includes a step of providing a laterally reciprocal moving means for reciprocally moving said substrate holder for said beam traversing on said substrate holder from one side of the edge to the other side of the edge or at least passing through the central area of said substrate holder.
Abstract:
A deceleration apparatus capable of decelerating a short spot beam or a tall ribbon beam is disclosed. In either case, effects tending to degrade the shape of the beam profile are controlled. Caps to shield the ion beam from external potentials are provided. Electrodes whose position and potentials are adjustable are provided, on opposite sides of the beam, to ensure that the shape of the decelerating and deflecting electric fields does not significantly deviate from the optimum shape, even in the presence of the significant space-charge of high current low-energy beams of heavy ions.
Abstract:
To select a relative velocity profile to be used in scanning an actual work piece with an ion implant beam of an ion implantation tool, the implantation of a virtual work piece is simulated. A dose distribution is calculated across the virtual work piece based on an implant beam profile and a relative velocity profile. A new relative velocity profile is then determined based on the calculated dose distribution and the relative velocity profile used in calculating the dose distribution. A new dose distribution is then calculated using the new relative velocity profile. A new relative velocity profile is determined and a corresponding new dose distribution is calculated iteratively until the new dose distribution meets one or more predetermined criteria. The new relative velocity profile is stored as the selected relative velocity profile when the new dose distribution meets the one or more predetermined criteria.
Abstract:
Techniques for low temperature ion implantation are provided to improve the throughput. During a low temperature ion implantation, an implant process may be started before the substrate temperature is decreased to be about to a prescribed implant temperature by a cooling process, and a heating process may be started to increase the substrate temperature before the implant process is finished. Moreover, one or more temperature adjust process may be performed during one or more portion of the implant process, such that the substrate temperature may be controllably higher than the prescribe implant temperature during the implant process.
Abstract:
A system and a method for moving a wafer during scanning the wafer by an ion beam. The proposed system includes an extendable/retractable arm, a holding apparatus and a driving apparatus. At least a length of the extendable/retractable arm is adjustable. The holding apparatus is capable of holding a wafer and is fixed on a specific portion of the extendable/retractable arm. Furthermore, the driving apparatus is capable of extending and/or retracting the extendable/retractable arm, such that the holding apparatus is moved together with the specific portion. In addition, the proposed method includes the following steps. First, hold the wafer by a holding apparatus fixed on a specific portion of an extendable/retractable arm. After that, adjust a length of the extendable/retractable. Therefore, the holding apparatus, i.e. the wafer, can be moved by the extension/retraction of the extendable/retractable arm.
Abstract:
An ion implanter and a method for implanting a wafer are provided, wherein the method includes the following steps. First, a wafer has at least a first portion requiring a first doping density and a second portion requiring a second doping density is provided. The first doping density is larger than the second doping density. Thereafter, the first portion is scanned by an ion beam with a first scanning parameter value, and the second portion is scanned by the ion beam with a second scanning parameter value. The first scanning parameter value can be a first scan velocity, and the second scanning parameter value can be a second scan velocity different than the first scan velocity. Alternatively, the first scanning parameter value can be a first beam current, and the second scanning parameter value can be a second beam current different than the first beam current.