Abstract:
Provided is a multifunctional charged particle beam device capable of inclining a beam with little aberration. The aberration is corrected by forming a local divergent field with a multipole, parallel current lines, or the like, matching the beam axis with the local divergent field via a conventional rotationally symmetric lens, deflector or astigmatism corrector, and counteracting an aberration occurring from another rotationally symmetric convex lens field.
Abstract:
The present invention relates to a lens-less Foucault method wherein a transmission electron microscope objective lens (5) is turned off, an electron beam crossover (11, 13) is matched with a selected area aperture (65), and the focal distance of a first imaging lens (61) can be changed to enable switching between a sample image observation mode and a sample diffraction pattern observation mode, characterized in that a deflector (81) is disposed in a stage following the first imaging lens (61), and conditions for an irradiating optical system (4) can be fixed after conditions for the imaging optical system have been determined. This allows a lens-less Foucault method to be implemented in a common general-use transmission electron microscope with no magnetic shielding lens equipped, without burdening the operator.
Abstract:
A multipole lens (100) which can produce static magnetic fields showing different strengths in the direction of travel of an electron beam has lens subasssemblies (10a, 10b, 10c) stacked on top of each other. The lens subassemblies (10a, 10b, 10c) have yokes (14a, 14b, 14c), respectively, and polar elements (12a, 12b, 12c), respectively. The polar elements (12a, 12b, 12c) have base portions (13a, 13b, 13c), respectively, magnetically coupled to the yokes (14a, 14b, 14c), respectively, and front end portions (11a, 11b, 11c), respectively, magnetically coupled to the base portions (13a, 13b, 13c), respectively. Magnetic field separators (20, 22) made of a nonmagnetic material are mounted between the front end portions (11a, 11b, 11c) which are successively adjacent to each other in the direction of stacking of the lens subassemblies (10a, 10b, 10c).
Abstract:
A particle-optical arrangement comprises a charged-particle source for generating a beam of charged particles; a multi-aperture plate arranged in a beam path of the beam of charged particles, wherein the multi-aperture plate has a plurality of apertures formed therein in a predetermined first array pattern, wherein a plurality of charged-particle beamlets is formed from the beam of charged particles downstream of the multi-aperture plate, and wherein a plurality of beam spots is formed in an image plane of the apparatus by the plurality of beamlets, the plurality of beam spots being arranged in a second array pattern; and a particle-optical element for manipulating the beam of charged particles and/or the plurality of beamlets; wherein the first array pattern has a first pattern regularity in a first direction, and the second array pattern has a second pattern regularity in a second direction electron-optically corresponding to the first direction, and wherein the second regularity is higher than the first regularity.
Abstract:
This charged particle beam device comprises: an electron beam source (1); a charged particle optical system that includes an object lens (9) and that irradiates a sample (10) with electrons emitted from the electron beam source (1) as an electron beam (2); an aberration corrector (6) that corrects aberrations in the charged particle optical system; and a control unit (24) that controls the components of the charged particle optical system and the aberration corrector (6). The charged particle beam device further comprises an automatic aberration-correcting device (17) that autonomously acquires, through leaning, optimum adjustment procedures in order to reduce the time required for correcting parasitic aberrations that arise in the aberration corrector (6).
Abstract:
In order to provide a charged particle beam apparatus enabling reduction of deflecting coma aberration in cases such as where wide field-of-view scanning is carried out, a charged particle beam apparatus is provided with an electromagnetic objective lens and a stage on which a sample is placed, wherein the electromagnetic objective lens is provided with the following: a plurality of magnetic paths; an objective lens coil; an opening disposed so as to face the sample; an inner lens deflector disposed more on the objective lens coil side than the end of the opening.
Abstract:
A combined round-multipole magnetic lens comprises a coil bracket, a first pole piece and a second pole piece. At least a first pole shoe of the first pole piece on the coil support and at least a second pole shoe of the second pole piece under the coil support respectively extend towards the central axis. The first pole shoe and the second pole shoe are symmetric according to the central axis, or the first pole shoes and the second pole shoes are respectively symmetrically arranged, and the angle difference between the first pole shoe and the adjacent second pole shoes is 360/2N degrees. A magnetic circuit gap is formed between the first pole shoe and the adjacent second pole shoe, for generating a magnetic field distribution of multi-poles and reducing the volume and the number of power supplies.
Abstract:
An aberration computing device (100) includes a fitting section (48) for fitting line profiles of a diffractogram taken in radial directions to a fitting function and finding fitting parameters of the fitting function and a computing section (49) for finding at least one of an amount of defocus and two-fold astigmatism, based on the fitting parameters.
Abstract:
A particle-optical arrangement comprises a charged-particle source for generating a beam of charged particles; a multi-aperture plate arranged in a beam path of the beam of charged particles, wherein the multi-aperture plate has a plurality of apertures formed therein in a predetermined first array pattern, wherein a plurality of charged-particle beamlets is formed from the beam of charged particles downstream of the multi-aperture plate, and wherein a plurality of beam spots is formed in an image plane of the apparatus by the plurality of beamlets, the plurality of beam spots being arranged in a second array pattern; and a particle-optical element for manipulating the beam of charged particles and/or the plurality of beamlets; wherein the first array pattern has a first pattern regularity in a first direction, and the second array pattern has a second pattern regularity in a second direction electron-optically corresponding to the first direction, and wherein the second regularity is higher than the first regularity.
Abstract:
The charged particle beam application device is provided with a charged particle source and an objective lens that converges charged particle beam generated by the charged particle source onto a sample. In this case, the charged particle beam application device is further provided with an aberration generating element installed between the charged particle beam source and the objective lens, a tilt-use deflector installed between the aberration generating element and the objective lens, a deflection aberration control unit for controlling the aberration generating element, a first electromagnetic field superposing multipole installed between the aberration generating element and the objective lens, and an electromagnetic field superposing multipole control unit for controlling the first electromagnetic field superposing multipole. The aberration generating element has such a function that when the charged particle beam is tilted relative to the sample by the tilt-use deflector, a plurality of resulting aberrations are cancelled with one another. Moreover, the first electromagnetic field superposing multipole has a function to change the orbit of a charged particle beam having energy different from that of the main charged particle beam in the charged particle beam.