Atmospheric scanning electron microscope achieves a wide field of view at low magnifications in a broad range of gaseous pressure, acceleration voltage and image resolution. This is based on the use of a reduced size pressure limiting aperture together with a scanning beam pivot point located at the small aperture at the end of electron optics column. A second aperture is located at the principal plane of the objective lens. Double deflection elements scan and rock the beam at a pivot point first at or near the principal plane of the lens while post-lens deflection means scan and rock the beam at a second pivot point at or near aperture at the end of the optics column. The aperture at the first pivot may act also as beam limiting aperture. In the alternative, with no beam limiting aperture at the principal plane, maximum amount of beam rays passes through the lens and with no post-lens deflection means, the beam is formed (limited) by a very small aperture at or near-and-below the final lens while the aperture skims a shifting portion of the wide beam, which is physically rocked with a pivot on the principal plane but with an apparent pivot point close and above the aperture, all of which result in a wide field of view on the examined specimen.

Disclosed is a charged particle optical apparatus. The charged particle optical apparatus has a liner electrode in a first vacuum zone. The liner electrode is used to generate an electrostatic objective lens field. The apparatus has a second electrode which surrounds at least a section of the primary particle beam path. The section extends in the first vacuum zone and downstream of the liner electrode. A third electrode is provided having a differential pressure aperture through which the particle beam path exits from the first vacuum zone. A particle detector is configured for detecting emitted particles, which are emitted from the object and which pass through the differential pressure aperture of the third electrode. The liner electrode, the second and third electrodes are operable at different potentials relative to each other.

The present invention relates to a scanning electron microscope realized to observe a test sample by detecting back-scattered electrons scattered and emitted from a surface of the test sample in the air without a vacuum chamber which is allowed to observe the test sample in a vacuum state the scanning electron microscope can be useful in minimizing dispersion of electrons of the electron beam passing through the shielding film caused due to electron scattering by focusing the electron beam passing through the shielding film on a top surface of the first back-scattered electron detector disposed between the electron gun and the shielding film to pass an electron beam and configured to detect back-scattered electrons scattered from the test sample since the first back-scattered electron detector is provided with the first planar coil having a magnetic field formed thereon.

Disclosed is a charged particle optical apparatus. The charged particle optical apparatus has a liner electrode in a first vacuum zone. The liner electrode is used to generate an electrostatic objective lens field. The apparatus has a second electrode which surrounds at least a section of the primary particle beam path. The section extends in the first vacuum zone and downstream of the liner electrode. A third electrode is provided having a differential pressure aperture through which the particle beam path exits from the first vacuum zone. A particle detector is configured for detecting emitted particles, which are emitted from the object and which pass through the differential pressure aperture of the third electrode. The liner electrode, the second and third electrodes are operable at different potentials relative to each other.

Atmospheric scanning electron microscope achieves a wide field of view at low magnifications in a broad range of gaseous pressure, acceleration voltage and image resolution. This is based on the use of a reduced size pressure limiting aperture together with a scanning beam pivot point located at the small aperture at the end of electron optics column. A second aperture is located at the principal plane of the objective lens. Double deflection elements scan and rock the beam at a pivot point first at or near the principal plane of the lens while post-lens deflection means scan and rock the beam at a second pivot point at or near aperture at the end of the optics column. The aperture at the first pivot may act also as beam limiting aperture. In the alternative, with no beam limiting aperture at the principal plane, maximum amount of beam rays passes through the lens and with no post-lens deflection means, the beam is formed (limited) by a very small aperture at or near-and-below the final lens while the aperture skims a shifting portion of the wide beam, which is physically rocked with a pivot on the principal plane but with an apparent pivot point close and above the aperture, all of which result in a wide field of view on the examined specimen.

The system described herein relates to an imaging device for imaging an object in a particle beam apparatus and/or for imaging a structural unit of a particle beam apparatus, and to a particle beam apparatus having such an imaging device. The imaging device has an illumination unit having a first switching state and a second switching state for illuminating the object and/or the structural unit with illumination light, where, in the first switching state, the illumination light comprises only light of a first spectral range and where, in the second switching state, the illumination light comprises only light of a second spectral range. The imaging device has a control unit for switching the illumination unit into the first switching state or into the second switching state, and a camera unit for imaging the object and/or the structural unit.

A permanently sealed vacuum tube is used to provide the electrons for an electron microscope. This advantageously allows use of low vacuum at the sample, which greatly simplifies the overall design of the system. There are two main variations. In the first variation, imaging is provided by mechanically scanning the sample. In the second variation, imaging is provided by point projection. In both cases, the electron beam is fixed and does not need to be scanned during operation of the microscope. This also greatly simplifies the overall system.

An x-ray analysis apparatus comprises an electron beam assembly for generating a focused electron beam within a first gas pressure environment. A sample assembly is used for retaining a sample within a second gas pressure environment such that the sample receives the electron beam from the electron beam assembly and such that the gas pressure in the second gas pressure environment is greater than the gas pressure within the first gas pressure environment. An x-ray detector is positioned so as to have at least one x-ray sensor element within the first gas pressure environment. The sensor element is mounted to a part of the electron beam assembly which is proximal to the sample assembly and further arranged in use to receive x-rays generated by the interaction between the electron beam and the sample.

An x-ray analysis apparatus comprises an electron beam assembly for generating a focused electron beam within a first gas pressure environment. A sample assembly is used for retaining a sample within a second gas pressure environment such that the sample receives the electron beam from the electron beam assembly and such that the gas pressure in the second gas pressure environment is greater than the gas pressure within the first gas pressure environment. An x-ray detector is positioned so as to have at least one x-ray sensor element within the first gas pressure environment. The sensor element is mounted to a part of the electron beam assembly which is proximal to the sample assembly and further arranged in use to receive x-rays generated by the interaction between the electron beam and the sample.

The present invention relates to a scanning electron microscope realized to observe a test sample by detecting back-scattered electrons scattered and emitted from a surface of the test sample in the air without a vacuum chamber which is allowed to observe the test sample in a vacuum state the scanning electron microscope can be useful in minimizing dispersion of electrons of the electron beam passing through the shielding film caused due to electron scattering by focusing the electron beam passing through the shielding film on a top surface of the first back-scattered electron detector disposed between the electron gun and the shielding film to pass an electron beam and configured to detect back-scattered electrons scattered from the test sample since the first back-scattered electron detector is provided with the first planar coil having a magnetic field formed thereon.