Abstract:
With a multi-beam type charged particle beam apparatus, and a projection charged particle beam apparatus, in the case of off-axial aberration corrector, there is the need for preparing a multitude of multipoles, and power supply sources in numbers corresponding to the number of the multipoles need be prepared. In order to solve this problem as described, a charged particle beam apparatus is provided with at least one aberration corrector wherein the number of the multipoles required in the past is decreased by about a half by disposing an electrostatic mirror in an electron optical system.
Abstract:
The present invention relates to e.g. a charged particle beam energy width reduction system for a charged particle beam with a z-axis along the optical axis and a first and a second plane, comprising, a first element acting in a focusing and dispersive manner, a second element acting in a focusing and dispersive manner, a first quadrupole element being positioned such that, in operation, a field of the first quadrupole element overlaps with a field of the first element acting in a focusing and dispersive manner, a second quadrupole element being positioned such that, in operation, a field of the second quadrupole element overlaps with a field of the second element acting in a focusing and dispersive manner, a first charged particle selection element being positioned, in beam direction, before the first element acting in a focusing and dispersive manner, and a second charged particle selection element being positioned, in beam direction, after the first element acting in a focusing and dispersive manner. Thereby, a virtually dispersive source-like location without an inherent dispersion limitation can be realized.
Abstract:
A charged particle beam apparatus for acquiring high-definition and highly contrasted observation images by detecting efficiently secondary signals without increasing aberration of the primary electron beam, detecting defects from observation images and thus increasing the inspection speed and enhancing the sensitivity of inspection. The desired area of the sample is scanned with a primary charged particle beam, and the secondary charged particles generated secondarily from the area by the irradiation of the primary charged particle beam are led to collide with the secondary electron conversing electrode, and then the secondary electrons generated by the first E×B deflector 31 arranged through an insulator on the surface of the secondary electron conversing electrode on the side of the sample is absorbed by the detector. At the same time, the deflection chromatic aberration that had been generated in the primary charged particle beam by the first E×B deflector is reduced by the second E×B deflector arranged on the first E×B deflector, to obtain high-definition and highly contrasted observation images free of shading.
Abstract:
A charged particle beam reflector device is configured to include at least two electrostatic mirrors arranged with a predetermined interval on a linear optical axis, each having a through hole through which a charged particle beam radiated from an electron gun along a linear optical axis passes, and having a function of reflecting the charged particle beam or allowing the charged particle beam to pass through the through hole in accordance with an applied voltage, and a controller controlling an applied voltage to the at least two electrostatic mirrors. The controller applies, to each of the electrostatic mirrors, a reflection voltage allowing the electrostatic mirrors to reflect the charged particle beam at a predetermined timing so that the charged particle beam from the electron gun is reflected by the at least two electrostatic mirrors a plurality of times.
Abstract:
The present invention aims to provide an axis alignment method, astigmatism correction method and SEM for implementing these methods, which can prevent an alignment or correction error attributable to conditions of a specimen. A first aspect is to obtain the difference between the optimal values acquired from an automatic axis alignment result on a standard sample and from each of automatic axis alignment results on a observation target sample, and to correct an optimal value adjusted using the standard sample by use of the difference thus obtained. A second aspect is to acquire an optimal stigmator value (astigmatism correction signal) by using the standard sample, to store the optimal stigmator value as a default value, to add the optimal stigmator value and the default value depending on the height of an observation target sample pattern, and to perform an astigmatism correction on the basis of the resultant stigmator value.
Abstract:
The present invention provides a charged particle beam device. The device comprises a first lens generating a crossover a second lens positioned after the crossover and an element acting in a focusing and dispersive manner in an x-z-plane with a center of the element having essentially same z-position as the crossover. Further, a multipole element, which acts in the x-z-plane and a y-z-plane is provided. A first charged particle selection element and a second charged particle selection element are used for selecting a portion of the charged particles. Thereby, e.g. the energy width of the charged particle beam can be reduced.
Abstract:
A corrective for eliminating the third-order aperture aberration and the first-order, first-degree axial chromatic aberration includes two correction pieces, which are arranged one behind the other in the direction of the optical axis, in which each correction piece has a plurality of quadrupole fields (QP) and at least one octupole field (OP.) Each correction piece is constructed such that it is symmetrical with respect to its central plane (S, S′) with each correction piece having an uneven number of at least five quadrupole fields (QP) and at least one octupole field (OP). Each correction piece is further constructed so that it is symmetrical with respect to its central plane. The central quadrupole field is arranged so that it is centered with respect to the central plane of the correction piece and is electromagnetic. The quadrupole fields of the two correction pieces are antisymmetrical and a transfer lens system is arranged such that it is symmetrical with respect to the central plane of the corrective between the correction pieces. The transfer lens system has two round lenses and the setting of the transfer lens system takes place so that the two round lenses image the central plane of the two correction pieces anamorphically onto one another, in which the enlargement in one main section is the reciprocal of the enlargement in the other main section and with an octupole field superimposed on the central quadrupole field.
Abstract:
The present invention relates to an orbit correction method for a charged particle beam, and aims to solve problems inherent in conventional aberration correction systems and to provide a low-cost, high-precision, high-resolution optical converging system for a charged particle beam. To this end, employed is a configuration in which a beam orbit is limited in ring zone form to form a distribution of electromagnetic field converging toward the center of a beam orbit axis. Consequently, a nonlinear action outwardly augmented, typified by spherical aberration of an electron lens, can be cancelled out. Specifically, this effect can be achieved by an electron disposed on the axis and subjected to a voltage to facilitate the occurrence of electrostatic focusing. For a magnetic field, this effect can be achieved by forming a coil radially distributed-wound on a surface equiangularly divided in the direction of rotation to control convergence of a magnetic flux density.
Abstract:
An electron beam apparatus with an aberration corrector using multipole lenses is provided. The electron beam apparatus has a scan mode for enabling the operation of the aberration corrector and a scan mode for disabling the operation of the aberration corrector and the operation of each of the aberration corrector, a condenser lens, and the like is controlled such that the object point of an objective lens does not change in either of the scan modes. If a comparison is made between the secondary electron images of a specimen in the two modes, the image scaling factor and the focus remain unchanged and evaluation and adjustment can be performed by distinctly recognizing only the effect of the aberration corrector. This reduces the time required to adjust an optical axis which has been long due to an axial alignment defect inherent in the aberration corrector and an axial alignment defect in a part other than the aberration corrector which are indistinguishably intermingled with each other.
Abstract:
There is disclosed a scanning electron microscope capable of removing the effects of vibrations on image information easily and reliably by detecting variations in the relative position between a specimen chamber holding a specimen therein and the specimen stage. The microscope has an image-processing portion that obtains information about the relative position between the specimen stage and the specimen chamber from a measurement unit when the beam is scanned. Based on the information about the relative position, a pixel position-correcting unit makes corrections to pixel positions indicated by the image information obtained by the scanning. An image creation unit creates image elements to eliminate pixel dropouts or pixel duplication produced by the aforementioned corrections. An image extraction unit extracts an image to be displayed.