Abstract:
In the semiconductor industry, microscopic samples are cut out of substrates for purposes of analysis. In the case of a known method, a sample to be cut loose out of a substrate is attached to a sample carrier connected to a manipulator and the sample is cut loose from the substrate. Subsequently, the sample is fixed to a TEM grid and completely separated from the sample carrier.According to the invention, the sample carrier 3 is left in connection with the sample 1 and the sample carrier 3 is separated from the manipulator 4. By making the sample carrier 3 connected to the sample 1 much bigger than the (microscopic) sample 1, and by manipulating the sample carrier 3, manipulation—with the aid of a (macroscopic) manipulator—of the microscopic sample 1 attached thereto becomes easier than manipulating the sample 1 without the sample carrier 3 attached thereto. In addition, a mechanical coupling between manipulator 4 and sample carrier 3 is shown, which enables a great degree of automation.
Abstract:
A charged-particle beam emitting device which includes the following configuration devices so that a lowering in the image resolution will be suppressed even if a primary beam is tilted relative to a sample: A device for causing orbit of the primary beam to pass through off-axes of a plurality of lenses, and controlling off-axis orbit of the primary beam. This device allows the aberration which occurs in the objective lens at the time of beam tilt to be cancelled out by the aberration which occurs in the other lens. Also, there is provided a device for simultaneously modulating excitations of the plurality of lenses including the objective lens.
Abstract:
An image noise removing method in an FIB/SEM complex apparatus of the invention prevents a secondary electron detection signal in an FIB blanking period from affecting pixels of an SEM image by, for example, synchronizing a scanning cycle of an SEM with that of an FIB and optimizes an SEM current with respect to an FIB current value to be used to thereby reduce an influence of a secondary electron excited by the FIB, which is to be superimposed, on the SEM image.
Abstract:
A magnetic pole of a magnetic field type lens is divided into a first magnetic pole section that is at ground potential, and a second magnetic pole section facing a sample and to which a negative high voltage is applied, the first magnetic pole section and the second magnetic pole section 212 being electrically insulated from each other, and an electric field type bi-potential lens is made up of an electrode attached to the first magnetic pole section so as to surround an electron beam path. High resolution observation with small chromatic aberration factor Cs, Cc is made possible without forming a positive high voltage section inside an electron beam path of a lens barrel.
Abstract:
An imaging and raster-mode scanning apparatus has a compensation device for compensating for ambient influences that may degrade the imaging, comprising an electrical filter, and at least one sensor for providing a first signal dependent on the ambient influences the first signal passes through the filter directly and drives an internal actuator and a internal control elements of the apparatus, which has an effect on the imaging and on the image display, in a calibrated state of the apparatus, which comprises a setting of a transfer characteristic of the filter, image degradations are greatly reduced or essentially compensated for. The filter for calibrating the apparatus, has a calibration input and a second signal is applied to the calibration input of the filter.
Abstract:
A particle-optical apparatus is proposed which comprises a particle-optical lens for deflecting a plurality of separate beam-charged particles which is provided by a plurality of finger electrodes provided along an opening of the lens.
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:
In an electron beam detector, a light guide optically couples a fluorescence emitting surface of the compound semiconductor substrate to a light incident surface of the photodetector, and physically connects the compound semiconductor substrate with the photodetector, thereby integrating the compound semiconductor substrate with the photodetector. When the compound semiconductor substrate converts incident electrons to fluorescent light, the light guide guides the fluorescent light to the photodetector, and the photodetector detects the fluorescent light, thereby detecting the incident electrons.
Abstract:
A particle-optical apparatus is proposed which comprises a particle-optical lens for deflecting a plurality of separate beam-charged particles which is provided by a plurality of finger electrodes provided along an opening of the lens.
Abstract:
An electron source for, for example, an electron microscope cannot exhibit a high brightness and a large beam current at the same time, because the virtual emitter dimension is enlarged by Coulomb repulsion in the electron beam in the case of a large beam current, thus reducing the brightness. In a conventional electron source switching-over could take place from a high brightness to a large beam current by varying the dimension of a beam-limiting diaphragm; however, this is objectionable because the location of such a diaphragm is not readily accessible. In accordance with the invention said switching-over can take place by arranging two lenses 26, 28 in the source, which lenses parallelize In the described circumstances the beam either directly behind the emitter 4 (large current) or directly in front of the diaphragm aperture 32 (high brightness).