H01J2237/05

Ion Source Gas Injection Beam Shaping
20230133101 · 2023-05-04 ·

An ion source for extracting a ribbon ion beam with improved height uniformity is disclosed. Gas nozzles are disposed in the chamber proximate the extraction aperture. The gas that is introduced near the extraction aperture serves to shape the ribbon ion beam as it is being extracted. For example, the height of the ribbon ion beam may be reduced by injecting gas above and below the ion beam so as to compress the extracted ion beam in the height direction. In some embodiments, the feedgas is introduced near the extraction aperture. In other embodiments, a shield gas, such as an inert gas, is introduced near the extraction aperture.

FLUORINE BASED MOLECULAR CO-GAS WHEN RUNNING DIMETHYLALUMINUM CHLORIDE AS A SOURCE MATERIAL TO GENERATE AN ALUMINUM ION BEAM
20230352265 · 2023-11-02 ·

An ion implantation system, ion source, and method are provided having a gaseous aluminum-based ion source material. The gaseous aluminum-based ion source material can be, or include, dimethylaluminum chloride (DMAC), where the DMAC is a liquid that transitions into vapor phase at room temperature. An ion source receives and ionizes the gaseous aluminum-based ion source material to form an ion beam. A low-pressure gas bottle supplies the DMAC as a gas to an arc chamber of the ion source by a primary gas line. A separate, secondary gas line supplies a co-gas, such as a fluorine-containing molecule, to the ion source, where the co-gas and DMAC reduce an energetic carbon cross-contamination and/or increase doubly charged aluminum.

Input lens and electron spectrometer
11404260 · 2022-08-02 · ·

An input lens is provided which has a large acceptance solid angle for electrons. The input lens is for use in an electron spectrometer and disposed between an electron source producing electrons and an electron analyzer in the electron spectrometer. The input lens has a reference electrode at a reference potential, a slit, first through nth electrodes, where n is an integer equal to or greater than three, arranged between the reference electrode and the slit, and a second mesh attached to the first electrode. The first through nth electrodes are arranged in this order along an optical axis. The second mesh is at a potential higher than the reference potential.

SYSTEM AND METHOD FOR PREPARATION AND DELIVERY OF BIOLOGICAL SAMPLES FOR CHARGED PARTICLE ANALYSIS

Systems and method for the preparation and delivery of biological samples for charged particle analysis are disclosed herein. An example system at least includes an ion filter coupled to select a sample ion from an ionized sample supply, the ion filter including a quadrupole filter to select the sample ion from the sample supply, an energy reduction cell coupled to receive the selected sample ion and reduce a kinetic energy of the sample ion, a validation unit coupled to receive the sample ion and determine whether the sample ion is a target sample ion, a substrate coupled to receive the sample, wherein the substrate is electron transparent, an ion transport module coupled to receive the sample ion from the ion filter and transport the sample ion to the substrate, and an imaging system arranged to image, with a low energy charged particle beam, the sample located on the substrate, wherein the substrate is arranged in an analysis location. The imaging system including a charge particle emitter coupled to direct coherent charged particles toward the sample; and a detector arranged to detect interference patterns formed from interaction of the coherent charged particles and the sample.

Spin polarimeter

A spin polarimeter includes: a particle beam source or a photon beam source that is a probe for a sample; a sample chamber in which the sample is accommodated; a spin detector that includes a target to be irradiated with an electron generated from the sample by a particle beam or a photon beam from the probe, and a target chamber in which the target is accommodated, and is configured to detect a spin of the sample by detecting an electron scattered on the target; a first exhaust system that is configured to exhaust the sample chamber; a second exhaust system that is configured to exhaust the target chamber; and an orifice that is disposed between the target chamber and the sample chamber.

Scanning magnet design with enhanced efficiency

A scanning magnet is positioned downstream of a mass resolving magnet of an ion implantation system and is configured to control a path of an ion beam downstream of the mass resolving magnet for a scanning or dithering of the ion beam. The scanning magnet has a yoke having a channel defined therein. The yoke is ferrous and has a first side and a second side defining a respective entrance and exit of the ion beam. The yoke has a plurality of laminations stacked from the first side to the second side, wherein at least a portion of the plurality of laminations associated with the first side and second side comprise one or more slotted laminations having plurality of slots defined therein.

Ion beam quality control using a movable mass resolving device

A system and method for optimizing a ribbon ion beam in a beam line implantation system is disclosed. The system includes a mass resolving apparatus having a resolving aperture, in which the resolving aperture may be moved in the X and Z directions. Additionally, a controller is able to manipulate the mass analyzer and quadrupole lenses so that the crossover point of desired ions can also be moved in the X and Z directions. By manipulating the crossover point and the resolving aperture, the parameters of the ribbon ion beam may be manipulated to achieve a desired result. Movement of the crossover point in the X direction may affect the mean horizontal angle of the beamlets, while movement of the crossover point in the Z direction may affect the horizontal angular spread and beam current.

Scan and corrector magnet designs for high throughput scanned beam ion implanter

An ion implantation system and method provide a non-uniform flux of a ribbon ion beam. A spot ion beam is formed and provided to a scanner, and a scan waveform having a time-varying potential is applied to the scanner. The ion beam is scanned by the scanner across a scan path, generally defining a scanned ion beam comprised of a plurality of beamlets. The scanned beam is then passed through a corrector apparatus. The corrector apparatus is configured to direct the scanned ion beam toward a workpiece at a generally constant angle of incidence across the workpiece. The corrector apparatus further comprises a plurality of magnetic poles configured to provide a non-uniform flux profile of the scanned ion beam at the workpiece.

Input Lens and Electron Spectrometer
20210098244 · 2021-04-01 ·

An input lens is provided which has a large acceptance solid angle for electrons. The input lens is for use in an electron spectrometer and disposed between an electron source producing electrons and an electron analyzer in the electron spectrometer. The input lens has a reference electrode at a reference potential, a slit, first through nth electrodes, where n is an integer equal to or greater than three, arranged between the reference electrode and the slit, and a second mesh attached to the first electrode. The first through nth electrodes are arranged in this order along an optical axis. The second mesh is at a potential higher than the reference potential.

SPIN POLARIMETER

A spin polarimeter includes: a particle beam source or a photon beam source that is a probe for a sample; a sample chamber in which the sample is accommodated; a spin detector that includes a target to be irradiated with an electron generated from the sample by a particle beam or a photon beam from the probe, and a target chamber in which the target is accommodated, and is configured to detect a spin of the sample by detecting an electron scattered on the target; a first exhaust system that is configured to exhaust the sample chamber; a second exhaust system that is configured to exhaust the target chamber; and an orifice that is disposed between the target chamber and the sample chamber.