Abstract:
A field emission electron source (10) includes a conductive base (12), a carbon nanotube (14), and a film of metal (16). The conductive base includes a top (122). One end (142) of the carbon nanotube is electrically connected with the top of the conductive base. The other end (144) of the carbon nanotube extends outwardly away from the top of the conductive base. The film of metal is formed on the nearly entire surface of the carbon nanotube and at least on the portion of the top of the conductive base proximate the carbon nanotube. A method for manufacturing the described field emission electron source is also provided.
Abstract:
A charged particle beam apparatus is provided which can prevent the accuracy of positional shift detection from being degraded owing to differences in picture quality, so that even when the state of a charged particle beam is changed at the time that optical conditions are changed or the optical axis changes with time, an auto adjustment of the optical axis can be realized easily and highly accurately. In the charged particle beam apparatus, evaluation or adjustment of focusing is conducted before the deflection condition of an alignment deflector for optical axis adjustment is changed or a table of focus adjustment amounts in correspondence with deflection conditions of the alignment deflector is provided, whereby when the deflection condition of the alignment deflector is changed, a focus adjustment is carried out in accordance with the table.
Abstract:
There is disclosed a charged-particle beam system equipped with a higher-order aberration corrector capable of correcting fifth-order spherical aberration and third-order chromatic aberration such that the primary trajectory of an electron beam is not affected by the strength of a transfer lens. The corrector is so adjusted that the image point of the corrector is located at a position shifted a distance of L0 from the principal plane of an objective lens toward the electron source. The transfer lens is so disposed that the position of the principal plane is coincident with the image point of the corrector. Therefore, the primary trajectory of the electron beam passes through the center of the transfer lens. Consequently, the primary trajectory is not affected by the strength of the transfer lens.
Abstract:
An aberration for correcting higher-order aberrations with a relatively small number of components is by let N1 being the aberration order at a first location, S1 being the symmetry at the first location, N2 being the aberration order at a second location and S2 being the symmetry at the second location. The produced combination aberration satisfies the following condition set 1 as order=N1+N2−1 and symmetry=|S1+S2| or |S2−S1|. That is two aberration-correcting elements (aberration-introducing elements) corresponding to the first and second locations, respectively. An aberration satisfying the condition set 1 is corrected by making use of the produced combination aberration.
Abstract:
A structure of an electron beam apparatus having shielding properties for shielding against an environmental magnetic field is provided. The electron beam apparatus comprises a mirror barrel for housing a magnetic lens for converging an electron beam onto a specimen and a specimen chamber for housing the specimen, wherein a non-magnetic material having conductivity is used as a material for at least one of the mirror barrel and a main body of the specimen chamber. The material for the mirror barrel or the main body of the specimen chamber is an aluminum alloy and a thickness of a sidewall of the mirror barrel or the main body of the specimen chamber is 10 mm or more. A magnetic plate having a thickness smaller than that of the sidewall of the mirror barrel or the main body of the specimen chamber is provided on an inner sidewall of the mirror barrel or the main body of the specimen chamber.
Abstract:
The present invention relates to a charged particle device with improved detection scheme. The device has a charged particle source providing a beam of primary charged particles; a first unit for providing a potential; a second unit for providing a potential; and a center unit positioned between the first unit and the second unit. The center unit is capable of providing a potential different from the potential of the first and the second unit for decelerating the primary charged particles to a first low energy and for accelerating the primary charged particles to a second high energy. Therein, the first unit and/or the second unit is a detector for detecting secondary electrons released at a specimen.
Abstract:
The invention concerns a corrector (10) for chromatic and aperture aberration correction in a scanning electron microscope or a scanning transmission electron microscope, comprising four multipole elements (1, 2, 3, 4) which are consecutively disposed in the optical path (9), the first (1) and fourth (4) of which are used to generate quadrupole fields (5, 6) and the second (2) and third (3) of which are used to generate octupole fields (11, 12) and quadrupole fields (7, 7′, 8, 8′), wherein the latter are superposed magnetic (7, 8) and electric (7′, 8′) fields, and wherein the quadrupole fields (5, 6, 7, 8) of all four multipole elements (1, 2, 3, 4) are successively rotated with respect to one another through 90°. Elimination of errors up to fifth order can be realized with a corrector (10) of this type in that the second (2) and the third (3) multipole elements are designed as twelve-pole elements, and an additional twelve-pole element (13) is inserted between the second (2) and the third (3) multipole element, and is loaded with current and/or voltage, such that an octupole field (14) is generated that is superposed by a twelve-pole field (15).
Abstract:
An object of the present invention is to provide a suitable method of observing a wafer edge by using an electron microscope. The electron microscope includes a column which can take an image in being tilted, and thus allows a wafer edge to be observed from an oblique direction.
Abstract:
A method of adjusting a response of an energy measuring filter, such as an FIR filter, of a pulse processor based on a slope of a preamplifier signal having a plurality of step edges each corresponding to a respective photon is provided that includes receiving a digital version of the preamplifier signal comprising a plurality of successive digital samples each having a digital value, the preamplifier signal having a portion defined by a first one of the step edges and a second one of the step edges immediately following the first one of the step edges, using the digital values of each of the digital samples associated with the portion to determine an average slope of the portion normalized by a length of the portion, and using the average slope of the portion normalized by a length of the portion to correct the response of the energy measuring filter.
Abstract:
An apparatus capable of improving image quality by making it possible to suck specimens of different sizes electrostatically, and uniformalizing an electric field of a specimen edge portion, while suppressing increase in prime cost is provided. Specimen holding means is an electrostatic chuck, a master flat plane part surrounding a specimen of the largest size of specimen sizes, and an opening surrounding a specimen size except for the largest specimen size are included at an outer peripheral portion of the electrostatic chuck, a dummy specimen attachable to and detachable from the electrostatic chuck is included, and at a time of switching the specimen size, a dummy specimen is selected (or may be prevented from being used).