Abstract:
There is disclosed a method of fabricating a smaller-sized multipole lens having polar elements that can be formed with high accuracy. The method starts with forming a first member (10) having a first yoke (14) formed integrally with first polar elements (12). A second member (20) having a second yoke (24) formed integrally with second polar elements (22) is formed. The first yoke (14) is made to overlap with the second yoke (24). The first member (10) and the second member (20) are held.
Abstract:
There is provided an image processing method capable of generating an image representative of a magnetic field distribution. The method starts with acquiring phase images providing visualization of electromagnetic fields respectively in a plurality of columns. Then, each of the electromagnetic fields in the columns within the phase images is separated into magnetic field and electric field components. An image representative of a magnetic field distribution is created based on the separated magnetic field components. The step of separating each electromagnetic field includes separating the electromagnetic field in a first one of the columns into magnetic field and electric field components based on the electromagnetic field in a second one of the columns, the latter electromagnetic field having an electric field component oriented in the same direction as that in the first column.
Abstract:
There is provided an image processing method capable of generating an image representative of a magnetic field distribution. The method starts with acquiring phase images providing visualization of electromagnetic fields respectively in a plurality of columns. Then, each of the electromagnetic fields in the columns within the phase images is separated into magnetic field and electric field components. An image representative of a magnetic field distribution is created based on the separated magnetic field components. The step of separating each electromagnetic field includes separating the electromagnetic field in a first one of the columns into magnetic field and electric field components based on the electromagnetic field in a second one of the columns, the latter electromagnetic field having an electric field component oriented in the same direction as that in the first column.
Abstract:
A method of acquiring a dark-field image for a scanning transmission electron microscope is provided. The scanning transmission electron microscope includes a dark-field detector having an annular detection region which is capable of detecting electrons scattered at a specimen in a predetermined angular range, an objective lens, and an imaging lens group disposed at a stage following the objective lens. The method includes reducing an influence of a geometrical aberration on the electrons scattered in the predetermined angular range by shifting a focus of the imaging lens group from a diffraction plane of the objective lens.
Abstract:
There is provided a method of aberration measurement capable of reducing the effects of image drift. The novel method of aberration measurement is for use in an electron microscope. The method comprises the steps of: acquiring a first image that is a TEM (transmission electron microscope) image of a sample; scanning the illumination angle of an electron beam impinging on the sample and acquiring a second image by multiple exposure of a plurality of TEM images generated at different illumination angles; and calculating aberrations from the first and second images.
Abstract:
There is provided a deflector that produces only a weak resulting combined hexapole field. The deflector (100) has first to sixth coils (11-16). The first to third coils (11-13) are equal in direction of energization. The fourth to sixth coils (14-16) are equal in direction of energization. The first coil (11) and fourth coil (14) are opposite in direction of energization. The first, third, fourth, and sixth coils (11, 13, 14, 16) are equal in electromotive force. The second coil (12) is equal in electromotive force to the fifth coil (15) and twice the electromotive force of the first coil (11).
Abstract:
A measurement method capable of easily measuring the directions of detector segments of a segmented detector relative to a scanning transmission electron microscope (STEM) image is provided. The measurement method is for use in an electron microscope equipped with the segmented detector having a detection surface divided into the detector segments. The measurement method is used to measure the directions of the detector segments relative to the STEM image. The method involves defocusing the STEM image to thereby cause a deviation of the STEM image and measuring the directions of the detector segments relative to the STEM image from the direction of the deviation of the STEM image (step S11).
Abstract:
An electron microscope is provided which can measure, with high sensitivity and high positional resolution, an amount of deflection of an electron beam occurring when it is transmitted through a sample. The electron microscope (100) is adapted to measure the amount of deflection of the electron beam (EB) when it is transmitted through the sample (S), and has an electron beam source (10) producing the electron beam (EB), an illumination lens system for focusing the electron beam (EB) onto the sample (S), an aperture (30) having an electron beam blocking portion (32) for providing a shield between a central portion (EB1) and an outer peripheral portion (EB2) of the cross section of the beam (EB) impinging on the sample (S), and a segmented detector (20) having a detection surface (22) for detecting the electron beam (EB) transmitted through the sample (S). The detection surface (22) is divided into a plurality of detector segments (D1-D4).
Abstract:
An electron microscope capable of measuring aberrations accurately is provided. The microscope is adapted to obtain scanning transmission electron (STEM) images by detecting electrons transmitted through a sample (S). The microscope (100) includes a segmented detector (20) having a detection surface (23) for detecting the electrons transmitted through the sample (S). The detection surface (23) is divided into detector segments (D1-D16) for detecting the electrons transmitted through the sample (S). The microscope (100) further includes an aperture plate (30) for limiting the active areas of the detector segments (D1-D16) on which the electrons impinge.
Abstract:
A method of acquiring a dark-field image for a scanning transmission electron microscope is provided. The scanning transmission electron microscope includes a dark-field detector having an annular detection region which is capable of detecting electrons scattered at a specimen in a predetermined angular range, an objective lens, and an imaging lens group disposed at a stage following the objective lens. The method includes reducing an influence of a geometrical aberration on the electrons scattered in the predetermined angular range by shifting a focus of the imaging lens group from a diffraction plane of the objective lens.