Abstract:
An energy contamination detection apparatus includes a membrane and a charge collection plate disposed at a distance from the membrane. The membrane is configured to receive an ion beam and allow a portion of the ion beam having energy levels above a desired energy level to pass therethrough toward the charge collection plate and absorb or reflect portions of the ion beam having energy levels at or below the desired energy level. A voltage source is electrically coupled to the charge collection plate for providing a bias voltage to the charge collection plate. A detection circuit is coupled to the charge collection plate and is configured to detect energy contamination based on an amount of charge collected on the charge collection plate.
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:
A multipurpose ion implanter beam line configuration comprising a mass analyzer magnet followed by a magnetic scanner and magnetic collimator combination that introduce bends to the beam path, the beam line constructed for enabling implantation of common monatomic dopant ion species cluster ions, the beam line configuration having a mass analyzer magnet defining a pole gap of substantial width between ferromagnetic poles of the magnet and a mass selection aperture, the analyzer magnet sized to accept an ion beam from a slot-form ion source extraction aperture of at least about 80 mm height and at least about 7 mm width, and to produce dispersion at the mass selection aperture in a plane corresponding to the width of the beam, the mass selection aperture capable of being set to a mass-selection width sized to select a beam of the cluster ions of the same dopant species but incrementally differing molecular weights, the mass selection aperture also capable of being set to a substantially narrower mass-selection width and the analyzer magnet having a resolution at the selection aperture sufficient to enable selection of a beam of monatomic dopant ions of substantially a single atomic or molecular weight, the magnetic scanner and magnetic collimator being constructed to successively bend the ion beam in the same sense, which is in the opposite sense to that of the bend introduced by the analyzer magnet of the beam line.
Abstract:
A method and apparatus satisfying growing demands for improving the precision of angle of incidence of implanting ions that impact a semiconductor wafer and the precision of ribbon ion beams for uniform doping of wafers as they pass under an ion beam. The method and apparatus are directed to the design and combination together of novel magnetic ion-optical transport elements for implantation purposes. The design of the optical elements makes possible: (1) Broad-range adjustment of the width of a ribbon beam at the work piece; (2) Correction of inaccuracies in the intensity distribution across the width of a ribbon beam; (3) Independent steering about both X and Y axes; (4) Angle of incidence correction at the work piece; and (5) Approximate compensation for the beam expansion effects arising from space charge. In a practical situation, combinations of the elements allow ribbon beam expansion between source and work piece to 350 millimeter, with good uniformity and angular accuracy. Also, the method and apparatus may be used for introducing quadrupole fields along a beam line.
Abstract:
Techniques for measuring energy contamination using time-of-flight (TOF) sensor are disclosed. In one particular exemplary embodiment, the techniques may be realized as a method for detecting energy contamination in an ion beam using time-of-flight comprising directing an ion beam towards an entrance of a sensor, wherein the ion beam may include charged particles and neutral particles, blocking the ion beam periodically from entering the sensor and allowing a pulse of the ion beam to enter the sensor periodically using a gate mechanism, separating the charged particles and the neutral particles of the ion beam pulse based at least in part upon different transit times over a distance caused by variations in at least one of mass and energy associated with the charged particles and the neutral particles, and detecting at least one of the charged particles and the neutral particles separately at a detector based at least in part upon the different transit times.
Abstract:
An apparatus and method for ion implantation that include destabilizing the ion beam as it passes through magnetic field, preferably a dipole magnetic field is disclosed. By introducing a bias voltage at certain points within the magnetic field, electrons from the plasma are drawn toward the magnet, thereby causing the ion beam to expand due to space charge effects. The bias voltage can be introduced into the magnet in a region where the magnetic field has only one component. Alternatively, the bias voltage can be in a region wherein the magnetic field has two components.
Abstract:
Non uniform ion implantations in a pendulum type of ion implantation are mitigated by adjusting movement of a wafer according to a corresponding non uniform function. More particularly, a non uniform ion implantation function is obtained by measuring and/or modeling ion implantations. Then, movement of a wafer along a second non arcuate scan path is adjusted according to the non uniform ion implantation function to facilitate uniform ion implantations.
Abstract:
An ion implantation system and associated method includes a scanner configured to scan a pencil shaped ion beam into a ribbon shaped ion beam, and a beam bending element configured to receive the ribbon shaped ion beam having a first direction, and bend the ribbon shaped ion beam to travel in a second direction. The system further includes an end station positioned downstream of the beam bending element, wherein the end station is configured to receive the ribbon shaped ion beam traveling in the second direction, and secure a workpiece for implantation thereof. In addition, the system includes a beam current measurement system located at an exit opening of the beam bending element that is configured to measure a beam current of the ribbon shaped ion beam at the exit opening of the beam bending element.
Abstract:
Ion implantation with high brightness, ion beam by ionizing gas or vapor, e.g. of dimers, or decaborane, by direct electron impact ionization adjacent the outlet aperture (46, 176) of the ionization chamber (80; 175)). Preferably: conditions are maintained that produce a substantial ion density and limit the transverse kinetic energy of the ions to less than 0.7 eV; width of the ionization volume adjacent the aperture is limited to width less than about three times the width of the aperture; the aperture is extremely elongated; magnetic fields are avoided or limited; low ion beam noise is maintained; conditions within the ionization chamber are maintained that prevent formation of an arc discharge. With ion beam optics, such as the batch implanter of FIG. (20), or in serial implanters, ions from the ion source are transported to a target surface and implanted; advantageously, in some cases, in conjunction with acceleration-deceleration beam lines employing cluster ion beams. Also disclosed are electron gun constructions, ribbon sources for electrons and ionization chamber configurations. Forming features of semiconductor devices, e.g. drain extensions of CMOS devices, and doping of flat panels are shown.
Abstract:
An ion implantation method is provided. The method, before ion implanting, is to rotate the substrate by an angle and shift the scan path of the ion beam with an interlace pitch in the direction perpendicular to the scan direction and on the plane of the substrate. Therefore a plurality of interlaced and not overlapped ion implantation scan lines are formed on the surface of the substrate, so the method can enhance the uniformity of the dose of the ion implantation in the substrate.