Abstract: An amount of pattern position displacement between observation images acquired by irradiating from two different directions is changed depending on beam deflection for moving an image acquisition position. In a pattern evaluation method that measures astigmatic difference or focus position displacement having a small amount of dose at a high speed using parallax caused by the tilted beam, a correction value obtained in advance by measurement is reflected in an amount of pattern position displacement between observation images obtained by irradiating from at least two different directions and generated in accordance with the amount of beam deflection for moving an image acquisition position. A processing unit calculates an amount of correction of an amount of pattern position displacement depending on beam deflection of a beam deflecting unit for moving an image acquisition position on the sample at a high speed.

Abstract: A sample fabricating method of irradiating a sample with a focused ion beam at an incident angle less than 90 degrees with respect to the surface of the sample, eliminating the peripheral area of a micro sample as a target, turning a specimen stage around a line segment perpendicular to the sample surface as a turn axis, irradiating the sample with the focused ion beam while the incident angle on the sample surface is fixed, and separating the micro sample or preparing the micro sample to be separated. A sample fabricating apparatus for forming a sample section in a sample held on a specimen stage by scanning and deflecting an ion beam, wherein an angle between an optical axis of the ion beam and the surface of the specimen stage is fixed and formation of a sample section is controlled by turning the specimen stage.

Abstract: A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.

Abstract: A charged-particle-beam device is characterized in having a control value for an aligner coil (29) being determined by: a coil current and an electrode applied-voltage at a control value for objectives (30, 31), which is an electromagnetic-field superposition lens; a control value for image-shift coils (27, 28); and the acceleration voltage of the charged-particle-beam. By doing this, it has become possible to avoid image disturbances that occur on images to be displayed at boundaries between charged areas and non-charged areas, and provide a charged-particle-beam device that obtains clear images without any unevenness in brightness.

Abstract: The astigmatism control processing time is decreased to 1 second or less by improving the astigmatic difference measurement accuracy. A charged particle beam device includes: a stage on which a sample is loaded; a transport mechanism which carries the sample onto the stage; a charged particle beam optical system which irradiates the sample on the stage with a charged particle beam and detects secondary charged particles generated from the sample; and a controller which determines setup parameters for the charged particle beam optical system and controls the charged particle beam optical system. The controller registers and holds electro-optical system setup parameters for irradiation with a beam tilted from a normal line on the sample as the charged particle beam, compares observation images obtained by the tilted beam, measures the amount and direction of movement and calculates the amount of astigmatism correction from the amount of movement and the direction.

Abstract: The electron beam device includes a source of electrons and an objective deflector. The electron beam device obtains an image on the basis of signals of secondary electrons, etc. which are emitted from a material by an electron beam being projected. The electron beam device further includes a bias chromatic aberration correction element, further including an electromagnetic deflector which is positioned closer to the source of the electrons than the objective deflector, and an electrostatic deflector which has a narrower interior diameter than the electromagnetic deflector, is positioned within the electromagnetic deflector such that the height-wise position from the material overlaps with the electromagnetic deflector, and is capable of applying an offset voltage. It is thus possible to provide an electron beam device with which it is possible to alleviate geometric aberration (parasitic aberration) caused by deflection and implement deflection over a wide field of view with high resolution.

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: Provided is a scanning electron microscope equipped with a high-speed and high-precision astigmatism measuring means to be used when both astigmatism generated by an electron-beam column and astigmatism generated from the surroundings of a measuring sample exist. This scanning electron microscope is characterized in controlling an astigmatism corrector (201) with high-speed and high-precision, to correct the astigmatism, by using both a method of obtaining the astigmatism from the qualities of two-dimensional images to be acquired upon changing the intensity of the astigmatism corrector (201), and a method of measuring the astigmatism from the change in the position displacement of an electron beam that occurs when the electron beam is tilted using a tilt deflector (202).

Abstract: An object of the invention is to realize a method and an apparatus for processing and observing a minute sample which can observe a section of a wafer in horizontal to vertical directions with high resolution, high accuracy and high throughput without splitting any wafer which is a sample. In an apparatus of the invention, there are included a focused ion beam optical system and an electron optical system in one vacuum container, and a minute sample containing a desired area of the sample is separated by forming processing with a charged particle beam, and there are included a manipulator for extracting the separated minute sample, and a manipulator controller for driving the manipulator independently of a wafer sample stage.

Abstract: The present invention provides an electron beam measurement technique for measuring the shapes or sizes of portions of patterns on a sample, or detecting a defect or the like. An electron beam measurement apparatus has a unit for irradiating the patterns delineated on a substrate by a multi-exposure method, and classifying the patterns in an acquired image into multiple groups according to an exposure history record. The exposure history record is obtained based on brightness of the patterns and a difference between white bands of the patterns.

Abstract: The electron beam device includes a source of electrons and an objective deflector. The electron beam device obtains an image on the basis of signals of secondary electrons, etc. which are emitted from a material by an electron beam being projected. The electron beam device further includes a bias chromatic aberration correction element, further including an electromagnetic deflector which is positioned closer to the source of the electrons than the objective deflector, and an electrostatic deflector which has a narrower interior diameter than the electromagnetic deflector, is positioned within the electromagnetic deflector such that the height-wise position from the material overlaps with the electromagnetic deflector, and is capable of applying an offset voltage. It is thus possible to provide an electron beam device with which it is possible to alleviate geometric aberration (parasitic aberration) caused by deflection and implement deflection over a wide field of view with high resolution.

Abstract: A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.

Abstract: Provided is a scanning electron microscope equipped with a high-speed and high-precision astigmatism measuring means to be used when both astigmatism generated by an electron-beam column and astigmatism generated from the surroundings of a measuring sample exist. This scanning electron microscope is characterized in controlling an astigmatism corrector (201) with high-speed and high-precision, to correct the astigmatism, by using both a method of obtaining the astigmatism from the qualities of two-dimensional images to be acquired upon changing the intensity of the astigmatism corrector (201), and a method of measuring the astigmatism from the change in the position displacement of an electron beam that occurs when the electron beam is tilted using a tilt deflector (202).

Abstract: In order to provide a charged beam device capable of obtaining a precise image of a sample surface pattern while improving the accuracy of automatic focus/astigmatism correction, there are provided an electron gun (1), a deflection control portion (8) which allows an electron beam to scan, a focus control portion (10) and an astigmatism correction portion (3) for the electron beam, an image processing portion (11), and a switching portion (9) which switches scan conditions when obtaining pattern information of the sample (1001) surface and scan conditions when performing the automatic focus/astigmatism correction, and a scan speed and scan procedures are switched between when obtaining the pattern information and when performing the automatic focus/astigmatism correction.

Abstract: A system is provided that realizes both reduction in coordinate error and improvement in throughput and allows observation of a micro-defect. The system includes: a function of measuring an amount of displacement between preliminarily calculated coordinates and an actual specimen position; a function of optimizing a coordinate correction formula so as to minimize the amount of displacement from the measured amount of displacement; and a function of calculating variation of displacement between the preliminarily calculated coordinates and the actual specimen position by statistical processing. When a value of coordinate variation is sufficiently small with respect to the field of view of an image for observation, which is to be a defect observation image, the system acquires only the image for observation without performing acquisition of an image for search, which is to be a defect search image.

Abstract: This charged particle beam microscope is characterized by being provided with selection means (153, 155) for a measurement processing method for detected particles (118) and by this means selecting a different measurement processing method for a scanning region with a large number of secondary electrons (115) emitted from a sample (114) and for a region with a small number of secondary electrons. Thus, in sample scanning using a charged particle beam microscope, an image in which the contrast of bottom holes and channel bottoms with few emitted secondary electrons is emphasized and images that emphasize shadow contrast can be acquired in a short period of time.

Abstract: A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.

Abstract: An electron beam apparatus which includes a sample stage on which a sample is placed, and an electron optical system. The electron optical system includes an electron gun that generates a primary electron beam, an immersion objective lens that converges the primary electron beam on the sample, an E×B deflector that separates a secondary particle, which is generated from irradiation of the primary beam to the sample, from an optical axis of the primary beam, a reflecting member to which the secondary particle collides, an assist electrode which is located under the reflecting member, a plurality of incidental particle detectors that selectively detect a velocity component and an azimuth component of a ternary particle which is generated by the secondary particle colliding to the reflecting member, and a center detector that is located above the reflecting member.

Abstract: Disclosed herewith is a charged particle beam apparatus capable of controlling each of the probe current and the objective divergence angle to obtain a desired probe current and a desired objective divergence angle in accordance with the diameter of the subject objective aperture. The apparatus is configured to include an objective aperture between first and second condenser lenses to calculate and set a control value of a first condenser lens in accordance with the diameter of the hole of the objective aperture so as to obtain a desired probe current and calculate a control value of a second condenser lens setting device in accordance with the diameter of the hole of the objective divergence angle and the control value of the second condenser lens setting device, thereby setting the calculated control value for the second condenser lens setting device to control the objective divergence angle.

Abstract: A lower pole piece of an electromagnetic superposition type objective lens is divided into an upper magnetic path and a lower magnetic path. A voltage nearly equal to a retarding voltage is applied to the lower magnetic path. An objective lens capable of acquiring an image with a higher resolution and a higher contrast than a conventional image is provided. An electromagnetic superposition type objective lens includes a magnetic path that encloses a coil, a cylindrical or conical booster magnetic path that surrounds an electron beam, a control magnetic path that is interposed between the coil and sample, an accelerating electric field control unit that accelerates the electron beam using a booster power supply, a decelerating electric field control unit that decelerates the electron beam using a stage power supply, and a suppression unit that suppresses electric discharge of the sample using a control magnetic path power supply.