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Fumio Hosokawa

Publications and source records attributed to Fumio Hosokawa.

2 recordsLinked to original sources

Transfer doublet and an elaborated phase plate holder for 120 kV electron-phase microscope.

A Zernike-type phase plate, which consisted of an amorphous carbon film, was developed for a 120 kV transmission electron microscope (TEM). The thickness of the film causes the scattered electrons to experience a pi/2 phase shift. The axial electrons pass through the central hole of the phase plate. The TEM was modified with an additional lens doublet, which allowed more flexibility in applying the phase plates. The doublet transfers the image from the back focal plane to a plane below the objective lens where a special phase plate holder, anticontaminator, and other necessary devices could be employed. The diameter of the central hole in the phase plate was 1 microm. The same mechanical system as in the specimen stage is used to align the axial beam into the hole. The use of a heating holder to protect the phase plate from contamination and consequential charging was investigated. Comparative diffractograms of amorphous carbon are shown with and without using a phase plate, demonstrating the change in phase contrast modulation from a sine to a cosine function when a phase plate is used. Images of biological specimens acquired using a phase plate are presented and the contrast enhancement due to the cosine transfer function is clearly demonstrated.

Animals↗

A spherical aberration-corrected 200 kV TEM.

A spherical aberration (Cs)-corrected 200 kV TEM was newly developed. The column of the microscope was extended by 25 cm and the inner yoke of the objective lens was modified to insert some parts of the corrector elements. The corrector has two hexapole elements that play a main role in Cs correction and they are placed at a position equivalent to the coma-free point of the objective lens by using two transfer doublet lenses. The Cs correction was successfully carried out by means of the third-order aberration that was generated in the two extended hexapoles. The Cs can be corrected to the desired value and also can be overcompensated in order to produce a negative Cs, as with the corrected Cs of -23 microm shown in this work. The optical system of the corrector does not produce second- and fourth-order aberrations, and can correct residual aberrations up to the third order. All of the corrector elements are computer-controlled and the third-order aberrations are quite stable after they are properly corrected. The resolution of 0.135 nm was experimentally confirmed by the Young's fringe method. Image simulations of a silicon [110] single crystal were made with various Cs and defocus values to demonstrate the effectiveness of arbitral control of Cs.

Journal Article↗