Abstract:
An ion implantation system and method are provided where an ion beam is tuned to a first process recipe. The ion beam is scanned along a scan plane at a first frequency, defining a first scanned ion beam. A beam profiling apparatus is translated through the first scanned ion beam and one or more properties of the first scanned ion beam are measured across a width of the first scanned ion, thus defining a first beam profile associated with the first scanned ion beam. The ion beam is then scanned at a second frequency, thus defining a second scanned ion beam, wherein the second frequency is less than the first frequency. A second beam profile associated with the second scanned ion beam is determined based, at least in part, on the first beam profile. Ions are subsequently implanted into a workpiece via the second scanned ion beam.
Abstract:
An ion implantation system has an ion source forming an ion beam. An mass analyzer defines and varies a mass analyzed beam along a beam path. A moveable mass resolving aperture assembly has a resolving aperture whose position is selectively varied in response to the variation of the beam path by the mass analyzer. A deflecting deceleration element positioned selectively deflects the beam path and selectively decelerate the mass analyzed beam. A controller selectively operates the ion implantation system in both a drift mode and decel mode. The controller passes the mass analyzed beam along a first path through the resolving aperture without deflection or deceleration in the drift mode and deflects and decelerates the beam along a second path in the decel mode. The position of the resolving aperture is selectively varied based on the variation in the beam path through the mass analyzer and the deflecting deceleration element.
Abstract:
A method for improving the productivity of a hybrid scan implanter by determining an optimum scan width is provided. A method of tuning a scanned ion beam is provided, where a desired beam current is determined to implant a workpiece with desired properties. The scanned beam is tuned utilizing a setup Faraday cup. A scan width is adjusted to obtain an optimal scan width using setup Faraday time signals. Optics are tuned for a desired flux value corresponding to a desired dosage. Uniformity of a flux distribution is controlled when the desired flux value is obtained. An angular distribution of the ion beam is further measured.
Abstract:
A method comprising introducing an injected gas (e.g., Argon, Xenon) into a beam line region comprising a magnetic scanner is provided herein. The injected gas improves beam current by enhancing (e.g., increasing, decreasing) charge neutralization of the magnetic ion beam (e.g., the ion beam at regions where the scanning magnetic field is non-zero) thereby reducing the current loss due to the zero field effect (ZFE). By reducing the current loss in regions having a magnetic field, the magnetic beam current is increased (e.g., the beam current is increased in regions where the magnetic field is non-zero) raising the overall beam current in a uniform manner over an entire scan path and thereby reducing the effect of the ZFE. In other words, the ZFE is removed by effectively minimizing it through an increase in the magnetized beam current.
Abstract:
A system and method are provided for implanting ions at low energies into a workpiece. An ion source configured to generate an ion beam is provided, wherein a mass resolving magnet is configured to mass resolve the ion beam. The ion beam may be a ribbon beam or a scanned spot ion beam. A mass resolving aperture positioned downstream of the mass resolving magnet filters undesirable species from the ion beam. A combined electrostatic lens system is positioned downstream of the mass analyzer, wherein a path of the ion beam is deflected and contaminants are generally filtered out of the ion beam, while concurrently decelerating and parallelizing the ion beam. A workpiece scanning system is further positioned downstream of the combined electrostatic lens system, and is configured to selectively translate a workpiece in one or more directions through the ion beam, therein implanting ions into the workpiece.
Abstract:
An ion implantation system and method are provided where an ion beam is tuned to a first process recipe. The ion beam is scanned along a scan plane at a first frequency, defining a first scanned ion beam. A beam profiling apparatus is translated through the first scanned ion beam and one or more properties of the first scanned ion beam are measured across a width of the first scanned ion, thus defining a first beam profile associated with the first scanned ion beam. The ion beam is then scanned at a second frequency, thus defining a second scanned ion beam, wherein the second frequency is less than the first frequency. A second beam profile associated with the second scanned ion beam is determined based, at least in part, on the first beam profile. Ions are subsequently implanted into a workpiece via the second scanned ion beam.
Abstract:
A system and method are provided for implanting ions at low energies into a workpiece. An ion source configured to generate an ion beam is provided, wherein a mass resolving magnet is configured to mass resolve the ion beam. The ion beam may be a ribbon beam or a scanned spot ion beam. A mass resolving aperture positioned downstream of the mass resolving magnet filters undesirable species from the ion beam. A combined electrostatic lens system is positioned downstream of the mass analyzer, wherein a path of the ion beam is deflected and contaminants are generally filtered out of the ion beam, while concurrently decelerating and parallelizing the ion beam. A workpiece scanning system is further positioned downstream of the combined electrostatic lens system, and is configured to selectively translate a workpiece in one or more directions through the ion beam, therein implanting ions into the workpiece.
Abstract:
A method comprising introducing an injected gas (e.g., Argon, Xenon) into a beam line region comprising a magnetic scanner is provided herein. The injected gas improves beam current by enhancing (e.g., increasing, decreasing) charge neutralization of the magnetic ion beam (e.g., the ion beam at regions where the scanning magnetic field is non-zero) thereby reducing the current loss due to the zero field effect (ZFE). By reducing the current loss in regions having a magnetic field, the magnetic beam current is increased (e.g., the beam current is increased in regions where the magnetic field is non-zero) raising the overall beam current in a uniform manner over an entire scan path and thereby reducing the effect of the ZFE. In other words, the ZFE is removed by effectively minimizing it through an increase in the magnetized beam current.
Abstract:
A method for improving the productivity of a hybrid scan implanter by determining an optimum scan width is provided. A method of tuning a scanned ion beam is provided, where a desired beam current is determined to implant a workpiece with desired properties. The scanned beam is tuned utilizing a setup Faraday cup. A scan width is adjusted to obtain an optimal scan width using setup Faraday time signals. Optics are tuned for a desired flux value corresponding to a desired dosage. Uniformity of a flux distribution is controlled when the desired flux value is obtained. An angular distribution of the ion beam is further measured.
Abstract:
An ion implantation system employs a mass analyzer for both mass analysis and angle correction. An ion source generates an ion beam along a beam path. A mass analyzer is located downstream of the ion source that performs mass analysis and angle correction on the ion beam. A resolving aperture within an aperture assembly is located downstream of the mass analyzer component and along the beam path. The resolving aperture has a size and shape according to a selected mass resolution and a beam envelope of the ion beam. An angle measurement system is located downstream of the resolving aperture and obtains an angle of incidence value of the ion beam. A control system derives a magnetic field adjustment for the mass analyzer according to the angle of incidence value of the ion beam from the angle measurement system.