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.

A method of observing a liquid specimen in an electron microscope includes: housing the liquid specimen in a space formed by a specimen stage and a lid member; and observing the liquid specimen, wherein the lid member includes a water retaining material, and a supporting member for supporting the water retaining material, and the water retaining material is provided with a through-hole that enables passage of an electron beam with which the liquid specimen is irradiated.

A vacuum condition controlling apparatus, the top of which is connected with an electron beam generating instrument. The apparatus is rotationally symmetric, comprises the following parts deployed outward from the central axis: the central channel, the first pumping channel, the gas supplying chamber and the at least one pumping chamber. A pressure limiting aperture is deployed near the outlet of the central channel, for keeping the pressure difference between the central channel and the outside environment, and allow the electron beam to go through the central channel; the first pumping channel is connected to the central channel to pump the central channel; the top of the gas supplying chamber is connected to the gas supplying channel to supply gas to the area between the specimen and the apparatus; the top of the second pumping channel is connected to the second pumping channel, to pump the area.

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.

In an atom probe having a vacuum chamber containing a specimen mount and a detector for receiving ions emitted from the specimen, a high vacuum subchamber is provided about the specimen mount, with an aperture in the subchamber allowing passage of emitted ions to the detector. The high vacuum subchamber may be pumped to higher vacuum (lower pressure) than the vacuum chamber, and so long as the pressure in the vacuum chamber is below about 10.sup.1 Pa, very little gas diffusion takes place through the aperture, allowing higher vacuum to be maintained in the subchamber despite the aperture opening to the chamber. The higher vacuum in the subchamber about the specimen assists in reducing noise in atom probe image data. The aperture may conveniently be provided by the aperture in a counter electrode, such as a local electrode, as commonly used in atom probes.

A vacuum condition controlling apparatus, the top of which is connected with an electron beam generating instrument. The apparatus is rotationally symmetric, comprises the following parts deployed outward from the central axis: the central channel, the first pumping channel, the gas supplying chamber and the at least one pumping chamber. A pressure limiting aperture is deployed near the outlet of the central channel, for keeping the pressure difference between the central channel and the outside environment, and allow the electron beam to go through the central channel; the first pumping channel is connected to the central channel to pump the central channel; the top of the gas supplying chamber is connected to the gas supplying channel to supply gas to the area between the specimen and the apparatus; the top of the second pumping channel is connected to the second pumping channel, to pump the area.

A vacuum condition processing apparatus is provided, the top of which is connected to an external charged particle beam generating device, and the apparatus includes: a suction cup in contact with the specimen to be observed or the stage holding the specimen, a first gas controlling device connected to an external gas supplying system, and a second gas controlling device connected to an external pumping system; a window is deployed at the top of the apparatus, through which the particle beam can go into the apparatus; the first gas controlling device is arranged to connect the gas supplying system and the suction cup; the second gas controlling device is arranged to connect the gas pumping system and the suction cup. Also disclosed is a specimen observation system and method.

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.

An aperture device (31) is described, which is attachable to a lens system (13). The lens system (13) is arranged to form a particle beam of charged particles, emitted from a sample surface (Ss). The aperture device (31) comprises an end surface (S) which is to be arranged facing the sample surface (Ss), at least one aperture (38) arranged in the end surface (S), a length axis (32) which extends through the centre of said at least one aperture (38), and at least one gas outlet (10), which is arranged at a transverse distance (T) perpendicular from the length axis (32), and is arranged to direct gas into a volume between at least one aperture (38) and the sample surface (Ss). The end surface (S) within a distance, equal to ? of the transverse distance (T), perpendicular from the length axis (32) has a variation along the length axis (32) being smaller than ? of the transverse distance (T).

A large current electron beam is stably emitted from an electron gun of a charged particle beam device. The electron gun of the charged particle beam device includes: a SE tip 202; a suppressor 303 disposed rearward of a distal end of the SE tip; a cup-shaped extraction electrode 204 including a bottom surface and a cylindrical portion and enclosing the SE tip and the suppressor; and an insulator 208 holding the suppressor and the extraction electrode. A shield electrode 301 of a conductive metal having a cylindrical portion 302 is provided between the suppressor and the cylindrical portion of the extraction electrode. A voltage lower than a voltage of the SE tip is applied to the shield electrode.