Abstract:
Provided is a method for forming a flying body using optical vortex laser, the method including irradiating an opposite surface of a base to a surface of the base, on which a light-absorbing material is disposed, with an optical vortex laser beam to generate a liquid column or liquid droplet having a diameter smaller than an irradiation diameter of the optical vortex laser beam from the light-absorbing material in an irradiation direction of the optical vortex laser beam.
Abstract:
An image forming method includes exposing a surface of an image bearer with light according to an image pattern including an image portion and a non-image portion, the image portion constituted of a plurality of pixels, to form an electrostatic latent image correspondent to the image pattern, comparing the image pattern adjacent to each of the pixels with a comparison pattern constituted of a plurality of pixels to specify at least a group of pixels existing at a boundary with respect to the non-image portion as a group of non-exposure pixels among the pixels constituting the image portion, and executing determination of specifying at least a group of pixels adjacent to the group of non-exposure pixels as a group of high power exposure pixels exposed with light of a higher light power than a predetermined light power required for exposing the image portion among the pixels constituting the image portion.
Abstract:
A surface charge measuring distribution method includes the steps of irradiating a sample with a charged particle beam and charging a sample surface in a spot-like manner, irradiating the charged sample with the charged particle beam to measure a potential at a potential saddle point formed above the sample, selecting one of preset multiple structure models and a tentative space charge distribution associated with the selected structure model, calculating a space potential at the potential saddle point by electromagnetic field analysis using the selected structure model and tentative space charge distribution, comparing the calculated space potential and measured value to determine the tentative space charge distribution as a space charge distribution of the sample when an error between the space potential and the measured value is within a predetermined range, and calculating a surface charge distribution of the sample by electromagnetic field analysis based on the determined space charge distribution.
Abstract:
A light scanning apparatus is provided in which a light source is controlled so that the total exposure energy density of when light beams are emitted to an image carrying member across light deflection scanning of a plurality of times becomes constant on the image carrying member, thereby high image quality, long lasting output images are obtained. Exposure energy density necessary when exposure is completed by light deflection scanning of one time is set to Ex1, the latent image electrical potential deepness of a latent image formed thereof is set to Vs1, total exposure energy density across light deflection scanning of a plurality of times is set to Ex_n, the latent image electrical potential deepness thereof is set to Vs_n, wherein Ex_n=Ex1−ΔEx and {(Vs_n/Vs1)^3−1.05}×Ex1
Abstract:
A latent-image measuring device that measures the state of a photoconductor. The latent-image measuring device emits a charged-particle beam to the photoconductor to detects a charged-particle signal obtained through the emission of the charged-particle beam. The latent-image measuring device then exposes the photoconductor a plurality of times to form electrostatic latent images on the photoconductor, and measures an amount of change in latent-image depth while changing a time interval between a plurality of exposures.
Abstract:
A surface-potential distribution measuring apparatus includes an electron gun, an electron-beam optical system, an electron-emission panel, a detector, and a control system. The electron-beam optical system is located between the electron gun and a sample, and focuses a beam of electrons emitted from the electron gun to the surface of the sample. The electron-emission panel is located near the sample to be collided with at least part of the electrons via the sample, and emits secondary electrons corresponding to the number of collided electrons. The detector detects at least part of the secondary electrons. The control system obtains potential distribution on the surface of the sample based on a detection result obtained by the detector.
Abstract:
In a surface potential distribution measurement method and device, a sample having a surface with a surface potential distribution is scanned using a charged particle beam in a two-dimensional manner. A detection signal caused by the two-dimensional scanning is obtained to measure the surface potential distribution. Charged particles, other than charged particles of the charged particle beam incident to the sample surface by the two-dimensional scanning, with which components of an incidence velocity vector of the charged particles in a direction perpendicular to the sample surface are reversed, are detected so that a detection signal indicating an intensity according to the detected charged particles is obtained in correspondence with a position on the sample surface.
Abstract:
An optical scanning lens used in a scanning and imaging optical system in which a beam deflected by a light deflector is condensed on or in the vicinity of a surface to be scanned. The optical scanning lens is formed through plastic mold, and a distribution of the refractive indexes Δn(x) inside of the optical scanning lens has a local maximum within a range through which the beam passes through the lens.
Abstract:
An apparatus configured to fly a light-absorbing material, includes a unit configured to irradiate a light-absorbing material absorbing light with a laser beam corresponding to a light absorption wavelength of the light-absorbing material to fly the light-absorbing material. When a preceding beam radiation region and a following beam radiation region overlap, the following beam radiation region is irradiated with the laser beam such that a beam centroid position is outside the preceding beam radiation region.
Abstract:
An optical processing apparatus includes a light source, a condensing optical system, and a shaping optical system. The light source emits light. The condensing optical system condenses the light emitted from the light source onto a processing target position on a surface of an object to be processed. The shaping optical system shapes a spot shape of the condensed light, such that a ratio of a major axis diameter of the spot shape to a minor axis diameter of the spot shape, in a cross section orthogonal to an optical axis of the condensed light on the object to be processed, is a minimum at or adjacent to a focal position of the shaping optical system. A method for optically processing an object is also provided.