Abstract:
When a signal electron is detected by energy selection by combining and controlling retarding and boosting for observation of a deep hole, etc., the only way for focus adjustment is to use a change in magnetic field of an objective lens. However, since responsiveness of the change in magnetic field is poor, throughput reduces. A charged particle beam device includes: an electron source configured to generate a primary electron beam; an objective lens configured to focus the primary electron beam; a deflector configured to deflect the primary electron beam; a detector configured to detect a secondary electron or a reflection electron generated from a sample by irradiation of the primary electron beam; an electrode having a hole through which the primary electron beam passes; a voltage control power supply configured to apply a negative voltage to the electrode; and a retarding voltage control power supply configured to generate an electric field, which decelerates the primary electron beam, on the sample by applying the negative voltage to the sample, wherein the charged particle beam device performs focus adjustment while an offset between the voltage applied to the electrode and the voltage applied to the sample is being kept constant.
Abstract:
The present invention is related to an apparatus for transporting a charged particle beam. The apparatus may include means for scanning the charged particle beam on a target, a dipole magnet arranged upstream of the means for scanning, at least three quadrupole lenses arranged between the dipole magnet and the means for scanning and means for adjusting the field strength of said at least three quadrupole lenses in function of the scanning angle of the charged particle beam. The apparatus can be made at least single achromatic.
Abstract:
In the case of a conventional gas field ionization ion source, it was not possible to carry out an analysis with a high S/N ratio and a high-speed machining process because the current amount of an ion beam is small. In view of these problems, the present invention has been devised, and its object is to obtain a large ion beam current, while suppressing a probability of damaging an emitter electrode. The present invention is characterized by a process in which an ion beam is emitted at least in two operation states including a first operation state in which, when a first extraction voltage is applied, with the gas pressure being set to a first gas pressure, ions are emitted from a first ion emission region at the apex of the emitter electrode, and a second operation state in which, when a second extraction voltage that is higher than the first extraction voltage is applied, with the gas pressure being set to a second gas pressure that is higher than the first gas pressure, ions are emitted from a second ion emission region that is larger than the first ion emission region.
Abstract:
An apparatus for transporting a charged particle beam is provided. The apparatus may include: means for scanning the charged particle beam on a target, a dipole magnet arranged upstream of the means for scanning, at least three quadrupole lenses arranged between the dipole magnet and the means for scanning, and means for adjusting the field strength of at least three quadrupole lenses in function of the scanning angle of the charged particle beam. The apparatus can be made at least single achromatic.
Abstract:
The present invention provides apparatuses to inspect small particles on the surface of a sample such as wafer and mask. The apparatuses provide both high detection efficiency and high throughput by forming Dark-field BSE images. The apparatuses can additionally inspect physical and electrical defects on the sample surface by form SE images and Bright-field BSE images simultaneously. The apparatuses can be designed to do single-beam or even multiple single-beam inspection for achieving a high throughput.
Abstract:
A diffraction aberration corrector formed by the multipole of the solenoid coil ring and having a function of adjusting the degree of orthogonality or axial shift of the vector potential with respect to the beam axis. In order to cause a phase difference, the diffraction aberration corrector that induces a vector potential, which is perpendicular to the beam axis and has a symmetrical distribution within the orthogonal plane with respect to the beam axis, is provided near the objective aperture and the objective lens. A diffracted wave traveling in a state of being inclined from the beam axis passes through the ring of the magnetic flux. Since the phase difference within the beam diameter is increased by the Aharonov-Bohm effect due to the vector potential, the intensity of the electron beam on the sample is suppressed.
Abstract:
There is provided both an electron beam apparatus and a lens array, capable of correcting a curvature of field aberration under various optical conditions. The electron beam apparatus comprises the lens array having a plurality of electrodes, and multiple openings are formed in the respective electrodes. An opening diameter distribution with respect to the respective opening diameters of the plural openings formed in the respective electrodes are individually set, and voltages applied to the respective electrodes are independently controlled to thereby independently adjust an image forming position of a reference beam, and a curvature of the lens array image surface.
Abstract:
A single column inductively coupled plasma source with user selectable configurations operates in ion-mode for FIB operations or electron mode for SEM operations. Equipped with an x-ray detector, energy dispersive x-ray spectroscopy analysis is possible. A user can selectively configure the ICP to prepare a sample in the ion-mode or FIB mode then essentially flip a switch selecting electron-mode or SEM mode and analyze the sample using EDS or other types of analysis.
Abstract:
An inspection device for inspecting a surface of an inspection object using a beam includes a beam generator capable of generating one of either charge particles or an electromagnetic wave as a beam, a primary optical system capable of guiding and irradiating the beam to the inspection object supported within a working chamber, a secondary optical system capable of including a first movable numerical aperture and a first detector which detects secondary charge particles generated from the inspection object, the secondary charge particles passing through the first movable numerical aperture, an image processing system capable of forming an image based on the secondary charge particles detected by the first detector; and a second detector arranged between the first movable numerical aperture and the first detector and which detects a location and shape at a cross over location of the secondary charge particles generated from the inspection object.
Abstract:
An apparatus for transporting a charged particle beam is provided. The apparatus may include: means for scanning the charged particle beam on a target, a dipole magnet arranged upstream of the means for scanning, at least three quadrupole lenses arranged between the dipole magnet and the means for scanning, and means for adjusting the field strength of at least three quadrupole lenses in function of the scanning angle of the charged particle beam. The apparatus can be made at least single achromatic.