Abstract:
In one embodiment, an aperture member producing method includes applying a charged particle beam to a plurality of chip areas on a first substrate while changing a writing condition to write a first pattern corresponding to an aperture opening, processing the first substrate based on the written first pattern to form a second pattern, cutting out a chip area provided with the second pattern having desired accuracy from the first substrate to produce a template, allowing the template to come into contact with a resist overlying a front surface of a second substrate, separating the template from the hardened resist to pattern the resist with a transfer pattern, processing the second substrate using the transfer pattern as a mask to form a first recess, and etching a rear surface of the second substrate to form a second recess communicating with the first recess.
Abstract:
Provided is a charged particle beam apparatus (111) to and from which a diaphragm (101) can be easily attached and detached, and in which a sample (6) can be arranged under vacuum and under high pressure. The charged particle beam apparatus includes: a lens barrel (3) holding a charged particle source (110) and an electron optical system (1,2,7); a first housing (4) connected to the lens barrel (3); a second housing (100) recessed to inside the first housing (4); a first diaphragm (10) separating the space inside the lens barrel (3) and the space inside the first housing (4), and through which the charged particle beam passes; a second diaphragm (101) separating the spaces inside and outside the recessed section (100a) in the second housing (100), and through which the charged particle beam passes; and a pipe (23) connected to a third housing (22) accommodating the charged particle source (110). The first diaphragm (10) is attached to the pipe (23), and the pipe (23) and the third housing (22) can be attached to and detached from the lens barrel (3) in the direction of the optical axis (30). A space (105) surrounded by the first housing (4) and the second housing (100) is depressurized, and the sample (6) arranged inside the recessed section (100a) is irradiated with a charged particle beam.
Abstract:
Provided is a charged particle beam apparatus (111) to and from which a diaphragm (101) can be easily attached and detached, and in which a sample (6) can be arranged under vacuum and under high pressure. The charged particle beam apparatus includes: a lens barrel (3) holding a charged particle source (110) and an electron optical system (1,2,7); a first housing (4) connected to the lens barrel (3); a second housing (100) recessed to inside the first housing (4); a first diaphragm (10) separating the space inside the lens barrel (3) and the space inside the first housing (4), and through which the charged particle beam passes; a second diaphragm (101) separating the spaces inside and outside the recessed section (100a) in the second housing (100), and through which the charged particle beam passes; and a pipe (23) connected to a third housing (22) accommodating the charged particle source (110). The first diaphragm (10) is attached to the pipe (23), and the pipe (23) and the third housing (22) can be attached to and detached from the lens barrel (3) in the direction of the optical axis (30). A space (105) surrounded by the first housing (4) and the second housing (100) is depressurized, and the sample (6) arranged inside the recessed section (100a) is irradiated with a charged particle beam.
Abstract:
Aimed at providing an ion implantation apparatus elongated in period over which failure of a target work, due to deposition and release of ion species typically to and from the inner surface of a through-hole shaping a beam shape of ion beam, may be avoidable, reduced in frequency of exchange of an aperture component, and consequently improved in productivity, an aperture component shaping a beam shape has a taper opposed to the ion beam, in at least a part of inner surface of at least the through-hole, and has a thick thermal-sprayed film formed so as to cover the inner surface and therearound of the through-hole.
Abstract:
An ion source includes an arc chamber having an extraction aperture, and a plasma sheath modulator. The plasma sheath modulator is configured to control a shape of a boundary between plasma and a plasma sheath proximate the extraction aperture. The plasma sheath modulator may include a pair of insulators positioned in the arc chamber and spaced apart by a gap positioned proximate the extraction aperture. A well focused ion beam having a high current density can be generated by the ion source. A high current density ion beam can improve the throughput of an associated process. The emittance of the ion beam can also be controlled.
Abstract:
A method and system of location specific processing on a substrate is described. The method comprises acquiring metrology data for a substrate, and computing correction data for adjusting a first region of the metrology data on the substrate. Thereafter, a first gas cluster ion beam (GCIB) for treating the high gradient regions is established, and the first GCIB is applied to the substrate according to the correction data. The method further comprises optionally acquiring second metrology data following the applying of the first GCIB, and computing second correction data for adjusting a second region of the metrology data, or the second metrology data, or both on the substrate. Thereafter, a second gas cluster ion beam (GCIB) for treating the second region is established, and the second GCIB is applied to the substrate according to the second correction data.
Abstract:
This invention relates to shaped apertures in an ion implanter that may act to clip an ion beam and so adversely affect uniformity of an implant. In particular, the present invention finds application in ion implanters that employ scanning of a substrate to be implanted relative to the ion beam such that the ion beam traces a raster pattern over the substrate. An ion implanter is provided comprising: a substrate scanner arranged to scan a substrate repeatedly through an ion beam in a scanning direction substantially transverse to the ion beam path, thereby forming a series of scan lines across the substrate; and an aperture plate having provided therein an aperture positioned on the ion beam path upstream of the substrate scanner, and wherein the aperture is defined in part by an inwardly-facing projection.
Abstract:
In one embodiment, a beam detector includes a first aperture plate including a first passage hole, a second aperture plate including a second passage hole that allows a single detection target beam passing through the first passage hole to pass therethrough, and a sensor detecting a beam current of the detection target beam passing through the second passage hole. The second aperture plate includes an electrically conductive material, a plurality of third passage holes are formed around the second passage hole, and the plurality of third passage holes allow light to pass therethrough.
Abstract:
A method of producing a corrected beam of charged particles for use in a charged-particle microscope, comprising the following steps: Providing a non-monoenergetic input beam of charged particles; Passing said input beam through an optical module comprising a series arrangement of: A stigmator, thereby producing an astigmatism-compensated, energy-dispersed intermediate beam with a particular monoenergetic line focus direction; A beam selector, comprising a slit that is rotationally oriented so as to match a direction of the slit to said line focus direction, thereby producing an output beam comprising an energy-discriminated portion of said intermediate beam.
Abstract:
A method of producing a corrected beam of charged particles for use in a charged-particle microscope, comprising the following steps: Providing a non-monoenergetic input beam of charged particles; Passing said input beam through an optical module comprising a series arrangement of: A stigmator, thereby producing an astigmatism-compensated, energy-dispersed intermediate beam with a particular monoenergetic line focus direction; A beam selector, comprising a slit that is rotationally oriented so as to match a direction of the slit to said line focus direction, thereby producing an output beam comprising an energy-discriminated portion of said intermediate beam.