Abstract: Pattern critical dimension measurement equipment includes an electron source configured to generate a primary electron beam, a deflector configured to deflect the primary electron beam emitted from the electron source, a focusing lens configured to focus the primary electron beam deflected by the deflector, a decelerator configured to decelerate the primary electron beam that irradiates the sample, a first detector located between the electron source and the focusing lens, the first detector being configured to detect electrons at part of azimuths of electrons generated from the sample upon irradiation of the sample with the primary electron beam, and a second detector located between the electron source and the first detector, the second detector being configured to detect electrons at substantially all azimuths of the electrons generated from the sample.

Abstract: To improve the efficiency of generation of chromatic aberrations of an energy filter for reducing energy distribution. Mounted are an energy filter for primary electrons, the energy filter having a beam slit and a pair of a magnetic deflector and an electrostatic deflector that are superimposed with each other. An electron lens is arranged between the beam slit and the pair of the magnetic deflector and the electrostatic deflector.

Abstract: A scanning electron beam device having: a deflector (5) for deflecting an electron beam (17) emitted from an electron source (1); an objective lens (7) for causing the electron beam to converge; a retarding electrode; a stage (9) for placing a wafer (16); and a controller (15); wherein the stage can be raised and lowered. In the low acceleration voltage region, the controller performs rough adjustment and fine adjustment of the focus in relation to the variation in the height of the wafer using electromagnetic focusing performed through excitation current adjustment of the objective lens. In the high acceleration voltage region, the controller performs rough adjustment of the focus in relation to the variation in the height of the wafer by mechanical focusing performed through raising and lowering of the stage, and performs fine adjustment by electrostatic focusing performed through adjustment of the retarding voltage.

Abstract: To provide a scanning electron microscope that can detect reflected electrons of any emission angle, the scanning electron microscope, which obtains an image by detecting electrons from a sample (19) has: a control electrode (18) that discriminates between secondary electrons from the sample (19) and reflected electrons; a secondary electron conversion electrode (13) that generates secondary electrons by the impact of reflected electrons; a withdrawing electrode (12) that withdraws those secondary electrons; an energy filter (11) that discriminates between the secondary electrons withdrawn and electrons reflected from the sample (19); and a control calculation means (36) that selects a combination of voltages applied to the secondary electron conversion electrode (13), the withdrawing electrode (12), and energy filter (11).

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: 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: A scanning electron microscope suppresses a beam drift by reducing charging on a sample surface while suppressing resolution degradation upon observation of an insulator sample. An electron microscope includes an electron source and an objective lens that focuses an electron beam emitted from the electron source, which provides an image using a secondary signal generated from the sample irradiated with the electron beam. A magnetic body with a continuous structure and an inside diameter larger than an inside diameter of an upper pole piece that forms the objective lens is provided between the objective lens and the sample.

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: 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: Provided is a high-resolution scanning electron microscope with minimal aberration, and equipped with an electro-optical configuration that can form a tilted beam having wide-angle polarization and a desired angle, without interfering with an electromagnetic lens. In the scanning electron microscope, an electromagnetic deflector (201) is disposed above a magnetic lens (207), and a control electrode (202) that accelerates or decelerates electrons is provided so at to overlap (in such a manner that the height positions overlap with respect to the vertical direction) with the electromagnetic deflector (201). In wide field polarization, electrodes are accelerated, and in tilted beam formation, electrons are decelerated.

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: In order that a displacement between patterns of different heights, formed on a sample in a plurality of different pattern-forming steps, can be measured at fixed throughput and with high accuracy, correspondence between parameters of lenses and beam deflector of an electron optical system and an angle of incidence of a beam upon the sample is recorded as data, then a correction value for the amount of displacement or edge positions is calculated, and a true amount of displacement is calculated from the correction value and an image under observation.

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: 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: Disclosed is a charged particle beam microscope which can obtain information about pattern materials and stereostructure without lowering throughput of pattern dimension measurement. To achieve this, the charged particle beam microscope acquires a plurality of frame images by scanning the field of view of the sample (S304, 305), adds the images together (S307), computes the dimensions of the pattern formed on the sample (308) and at the same time acquires pattern information (314) using components of a frame image, such as a single frame image or subframe image, as a separated image (309, 310).

Abstract: A charged particle instrument including a controlling and operating unit for controlling a charged particle source, deflecting means, and focus changing means and making a data for an image by an electric signal detected by a detector, and a recording unit for preserving a correction coefficient registered at each image-acquisition, in which the controlling and operating unit acquires plural images while changing a focus, and controls an optical condition such that a landing angle of a charged particle beam becomes perpendicular when an image for measurement is acquired on the basis of a position shift amount of a mark in the image and a correction coefficient registered to the recording unit.

Abstract: Provided is a high-resolution scanning electron microscope with minimal aberration, and equipped with an electro-optical configuration that can form a tilted beam having wide-angle polarization and a desired angle, without interfering with an electromagnetic lens. In the scanning electron microscope, an electromagnetic deflector (201) is disposed above a magnetic lens (207), and a control electrode (202) that accelerates or decelerates electrons is provided so at to overlap (in such a manner that the height positions overlap with respect to the vertical direction) with the electromagnetic deflector (201). In wide field polarization, electrodes are accelerated, and in tilted beam formation, electrons are decelerated.

Abstract: In a mold in which a pattern is formed of a fine concavo-convex shape, two or more of alignment marks for determining a relative positional relation between a substrate and a mold are formed concentrically. Moreover, a damaged mark is identified from the positional information and shape of the respective marks, and an alignment between the mold and the substrate to which a resin film is applied is carried out excluding the damaged mark.