Abstract:
Provided is a charged particle beam apparatus, which can emit a stable electron beam, having high brightness and a narrow energy width. The charged particle beam apparatus comprises a field emission electron source, electrodes for applying an electric field to the field emission electron source, and a vacuum exhaust unit for keeping the pressure around the field emission electron source at 1×10−8 Pa or less. The apparatus is so constituted as to use such one of the electron beams emitted as has an electron-beam-center radiation angle of 1×10−2sr or less, and to use the electric current thereof, the second order differentiation of which is negative or zero with respect to the time, and which reduces at a rate of 10% or less per hour. The charged particle beam apparatus further comprises a heating unit for the field emission electron source, and a detection unit for the electric current of the electron beam. The field emission electron source is repeatedly heated to keep the electric current of the electron beam to be emitted, at a predetermined value or higher.
Abstract:
System that focuses electron beams in an electro-static area to a laminar flow of electrons with uniform distribution of current density and extraordinary demagnification includes a housing having a first interior portion and a second interior portion electrically insulated from the first interior portion. The second interior portion has an electric field-free space. An electrode system is disposed in the first interior portion and includes a cathode assembly and at least one anode assembly. The cathode assembly generates an electron beam that passes through each anode assembly and then into the electric field-free space in the second interior portion. A position of a crossover point on a longitudinal axis maybe regulated by varying dimensions of a substantially cylindrical portion of the anode assembly and a substantially cylindrical portion of a near-cathode electrode assembly.
Abstract:
A method determines ion beam emittance, i.e., the beam current density based on position and angle, in a charged particle transport system. The emittance is determined from variations in the current measured in a slot Faraday or sample cup as a straight-edged mechanism traverses the beam upstream of the sample cup in a direction perpendicular to the orientation of the slot Faraday and the straight-edged mechanism, which also can be the direction in which the emittance is determined. An expression in terms of the beam current density can be determined for the derivative of the sample current with respect to position of the mechanism. Depending on the angular spread of the beam reaching the sample cup, the density can be determined directly from the derivative, or can be determined using a least squares analysis of the derivative over a range of mechanism positions.
Abstract:
Non-elliptical ion beams (508) and plumes (510) of sputtered material can yield a relatively uniform wear pattern on a destination target (504) and a uniform deposition of sputtered material on a substrate assembly (506). The non-elliptical ion beams (508) and plumes (510) of sputtered material impinge on rotating destination targets (504) and substrate assemblies (506). A first example ion beam grid (302) and a second example ion beam grid (304) each have patterns of holes with an offset between corresponding holes. The quantity and direction of offset determines the quantity and direction of steering individual beamlets passing through corresponding holes in the first and second ion beam grids (302, 304). The beamlet steering as a whole creates a non-elliptical current density distribution within a cross- section of an ion beam (508) and generates a sputtered material plume (510) that deposits a uniform distribution of sputtered material onto a rotating substrate assembly (506).
Abstract:
System that focuses electron beams in an electro-static area to a laminar flow of electrons with uniform distribution of current density and extraordinary demagnification includes a housing having a first interior portion and a second interior portion electrically insulated from the first interior portion. The second interior portion has an electric field-free space. An electrode system is disposed in the first interior portion and includes a cathode assembly and at least one anode assembly. The cathode assembly generates an electron beam that passes through each anode assembly and then into the electric field-free space in the second interior portion. The system parameters may be calculated and created due to the CGMR conceptual method.
Abstract:
Provided may include an electron beam generator, an image apparatus including the same, and an optical apparatus. The optical apparatus includes a first and second laser apparatuses providing a first and second laser beams on a substrate, and a first optical system provided between the first and second laser apparatuses and the substrate to focus the first and second laser beams. The first and second laser beams overlap with each other generating an interference beam, thereby decreasing a spot size of the interference beam to be smaller than a wavelength of each of the first and second laser beams at a focal point.
Abstract:
A charged particle beam apparatus includes a field emission electron source, electrodes for applying an electric field to the field emission electron source, and a vacuum exhaust unit for keeping the pressure around the field emission electron source at 1×10−8 Pa or less. The apparatus uses electron beams emitted to have an electron-beam-center radiation angle of 1×10−2 sr or less, and uses the electric current thereof, the second order differentiation of which is negative or zero with respect to time, and which reduces at a rate of 10% or less per hour. A heating unit is provided for the field emission electron source, and a detection unit is provided for the electric current of the electron beam. The field emission electron source is repeatedly heated to keep the electric current of the electron beam to be emitted, at a predetermined value or higher.
Abstract:
Problems to be solved: To obtain higher brightness than Langmuir limit. Adjust brightness to the optimum value.Method of resolution: To obtain such beams, the following means and methods are effective. A charged particles beam apparatus consisting of a charged particle source, a beam drawing electrode, and a beam control electrode, wherein; after the charged particles beam source a condenser lens is designed, and brightness of the charged particles beam is adjusted by adjusting a magnification factor of said condenser lens.
Abstract:
System that focuses electron beams in an electro-static area to a laminar flow of electrons with uniform distribution of current density and extraordinary demagnification includes a housing having a first interior portion and a second interior portion electrically insulated from the first interior portion. The second interior portion has an electric field-free space. An electrode system is disposed in the first interior portion and includes a cathode assembly and at least one anode assembly. The cathode assembly generates an electron beam that passes through each anode assembly and then into the electric field-free space in the second interior portion. The system parameters may be calculated and created due to the CGMR conceptual method.
Abstract:
Provided is a charged particle beam apparatus, which can emit a stable electron beam, having high brightness and a narrow energy width. The charged particle beam apparatus comprises a field emission electron source, electrodes for applying an electric field to the field emission electron source, and a vaccume exhaust unit for keeping the pressure around the field emission electron source at 1 10−8 Pa or less. The apparatus is so constituted as to use such one of the electron beams emitted as has an electron-beam-center radiation angle of 1 10−2 str or less, and to use the electric current thereof, the second order differentiation of which is negative or zero with respect to the time, and which reduces at a rate of 10% or less per hour. The charged particle beam apparatus further comprises a heating unit for the field emission electron source, and a detection unit for the electric current of the electron beam. The field emission electron source is repeatedly heated to keep the electric current of the electron beam to be emitted, at a predetermined value or higher.