The invention discloses a sub-nanoscale high-precision lithography writing field stitching method. A photosensitive resist layer is coated on the surface of the wafer to be exposed; after the surface of the photosensitive resist layer is exposed, the exposed pattern will generate a tiny concave-convex structure; the concave-convex structure patterns are identified with a nano contact sensor and can be used as in-situ alignment coordinate markers; by comparing the position coordinates of the writing field before and after exposure and wafer moving, the deviations of stitching can be calculated, and an high-precision lithography stitching of the wafer is performed in a negative feedback control mode, so that the disadvantages of the existing non-in-situ, far-from-writing field and the poor performance of stitching precision in blind type open-loop lithography technology due to the influence of mechanical motion precision of a wafer workbench and long-time drift of an electron beam are overcome.

In corner sections of first to fourth quadrants whose origin point is a center of an upper surface of a stage, three each of two-dimensional heads are provided. The three each of two-dimensional heads include one first head and two second heads. The stage is driven, while measuring a position of the stage using three first heads that face a two-dimensional grating of a scale plate provided above the stage from the four first heads, and during the driving, difference data of measurement values of the two second heads with respect to the first head in a measurement direction are taken in for head groups to which the three first heads belong, respectively, and using the difference data, grid errors are calibrated.

Aspects of the disclosure relate to apparatus for the fabrication of waveguides. In one example, an angled ion source is utilized to project ions toward a substrate to form a waveguide which includes angled gratings. In another example, an angled electron beam source is utilized to project electrons toward a substrate to form a waveguide which includes angled gratings. Further aspects of the disclosure provide for methods of forming angled gratings on waveguides utilizing an angled ion beam source and an angled electron beam source.

Aspects of the disclosure relate to apparatus for the fabrication of waveguides. In one example, an angled ion source is utilized to project ions toward a substrate to form a waveguide which includes angled gratings. In another example, an angled electron beam source is utilized to project electrons toward a substrate to form a waveguide which includes angled gratings. Further aspects of the disclosure provide for methods of forming angled gratings on waveguides utilizing an angled ion beam source and an angled electron beam source.

A multi-column metrology tool may include two or more measurement columns distributed along a column direction, where the two or more measurement columns simultaneously probe two or more measurement regions on a sample including metrology targets. A measurement column may include an illumination sub-system to direct illumination to the sample, a collection sub-system including a collection lens to collect measurement signals from the sample and direct it to one or more detectors, and a column-positioning sub-system to adjust a position of the collection lens. A measurement region of a measurement column may be defined by a field of view of the collection lens and a range of the positioning system in the lateral plane. The tool may further include a sample-positioning sub-system to scan the sample along a scan path different than the column direction to position metrology targets within the measurement regions of the measurement columns for measurements.

A system and method for optimizing a ribbon ion beam in a beam line implantation system is disclosed. The system includes a calibration sensor disposed in the beam line after the mass analyzer. The calibration sensor is able to measure both the total current of the ribbon ion beam, as well as provide information about its vertical position. Information from the calibration sensor can then be utilized by a controller to adjust various parameters to improve the density as well as the vertical position. In some embodiments, the calibration sensor may include a plurality of Faraday sensors, where, both the total current and the vertical position of the ion beam can be determined. Furthermore, the focus of the ion beam can be estimated based on the distribution of the current in the height direction.

In a charged particle beam writing method according to one embodiment, a deflector is caused to deflect a charged particle beam and a pattern is written by irradiating a substrate with the charged particle beam. The charged particle beam writing method includes calculating a charge amount distribution based on a charge amount of a beam irradiation region on the substrate immediately after irradiation with the charged particle beam and a diffusion coefficient for electric charge of the substrate, calculating a position shift distribution of the charged particle beam on the substrate based on the charge amount distribution, and correcting an irradiation position of the charged particle beam based on the position shift distribution.

A multi-beamlet charged particle beamlet lithography system for transferring a pattern to a surface of a substrate. The system comprises a projection system (311) for projecting a plurality of charged particle beamlets (7) onto the surface of the substrate; a chuck (313) moveable with respect to the projection system; a beamlet measurement sensor (.[.i.a..]. .Iadd.i.e., .Iaddend.505, 511) for determining one or more characteristics of one or more of the charged particle beamlets, the beamlet measurement sensor having a surface (501) for receiving one or more of the charged particle beamlets; and a position mark measurement system for measuring a position of a position mark (610, 620, 635), the position mark measurement system comprising an alignment sensor (361, 362). The chuck comprises a substrate support portion for supporting the substrate, a beamlet measurement sensor portion (460) for accommodating the surface of the beamlet measurement sensor, and a position mark portion (470) for accommodating the position mark.

Provided herein are approaches for optimizing a full horizontal scanned beam distance of an accelerator beam. In one approach, a method may include positioning a first Faraday cup along a first side of an intended beam-scan area, positioning a second Faraday cup along a second side of the intended beam-scan area, scanning an ion beam along the first and second sides of the intended beam-scan area, measuring a first beam current of the ion beam at the first Faraday cup and measuring a second beam current of the ion beam at the second Faraday cup, and determining an optimal scan distance of the ion beam across the intended beam-scan area based on the first beam current and the second beam current.

A method for controlling operation of an electron emission source includes acquiring, while varying an emission current of an electron beam, a characteristic between a surface current of a target object at a position on the surface of the target object irradiated with the electron beam, and the emission current, calculating, based on the characteristic, first gradient values each obtained by dividing the surface current of the target object by the emission current, in a predetermined range of the emission current in the characteristic, calculating a second gradient value by dividing a surface current of the target object by an emission current in a state where the electron beam has been adjusted, and adjusting a cathode temperature to make the second gradient value in the state where the electron beam has been adjusted be in the range of the first gradient values in the predetermined range of the emission current.