Abstract: A disclosed scanning electron microscope (SEM) is intended to prevent deterioration of resolution due to increase in off-axis aberration resulting from a deviation of a primary electron bean from the optical axis of the microscope. An example of the SEM has an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed, and dimensions can be measured in a high accuracy. The SEM is able to achieve precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.

Abstract: A scanning electron microscope with an energy filter which can positively utilize secondary electrons and/or reflected electrons which collide against a mesh electrode and are lost. The scanning electron microscope which has a porous electrode for producing an electric field for energy-filtering electrons produced by applying a primary electron beam to a sample and a 1st electron detector which detects electrons passing through the porous electrode is characterized by further having a porous structure provided near the sample, a deflector which deflects electrons from the axis of the primary electron beam, and a 2nd electron detector which detects the electrons deflected by the deflector.

Abstract: A scanning electron microscope with an energy filter which can positively utilize secondary electrons and/or reflected electrons which collide against a mesh electrode and are lost. The scanning electron microscope which has a porous electrode for producing an electric field for energy-filtering electrons produced by applying a primary electron beam to a sample and a 1st electron detector which detects electrons passing through the porous electrode is characterized by further having a porous structure provided near the sample, a deflector which deflects electrons from the axis of the primary electron beam, and a 2nd electron detector which detects the electrons deflected by the deflector.

Abstract: To make it possible to observe the bottom of a contact hole and internal wires, in observation of the contact hole 102, by scanning it at a predetermined acceleration voltage, the positive charge 106 is formed on the surface of the insulator 101, and the secondary electrons 104 are attracted in the hole by this electric field, and the hole is continuously scanned at an acceleration voltage different from the acceleration voltage, and the sample is observed. When the wires embedded in the insulator are to be observed, by observing the insulator at a predetermined acceleration voltage, an electron beam is allowed to enter the sample, and the sample is continuously scanned at an acceleration voltage different from the acceleration voltage, and hence the existence of wires is reflected as a change in the charge of the surface, and it is observed.

Abstract: An invention providing a scanning electron microscope composed of a monochromator capable of high resolution, monochromatizing the energy and reducing chromatic aberrations without significantly lowering the electrical current strength of the primary electron beam. A scanning electron microscope is installed with a pair of sectorial magnetic and electrical fields having opposite deflection directions to focus the electron beam and then limit the energy width by means of slits, and another pair of sectorial magnetic and electrical fields of the same shape is installed at a position forming a symmetrical mirror versus the surface containing the slits. This structure acts to cancel out energy dispersion at the object point and symmetrical mirror positions, and by spatially contracting the point-converged spot beam with a converging lens system, improves the image resolution of the scanning electron microscope.

Abstract: A charged-particle beam emitting device which includes the following configuration devices so that a lowering in the image resolution will be suppressed even if a primary beam is tilted relative to a sample: A device for causing orbit of the primary beam to pass through off-axes of a plurality of lenses, and controlling off-axis orbit of the primary beam. This device allows the aberration which occurs in the objective lens at the time of beam tilt to be cancelled out by the aberration which occurs in the other lens. Also, there is provided a device for simultaneously modulating excitations of the plurality of lenses including the objective lens.

Abstract: A charged particle beam apparatus produces little reduction in resolution when the beam is inclined with respect to a sample. The trajectory of a primary beam 4 is deflected by a deflector or changed by a movable aperture such that the beam is incident on a plurality of lenses 6 and 7 off the axes thereof. A means is provided to control the off-axis trajectory of the beam such that an aberration produced by the objective lens 7 when the beam is inclined can be canceled by an aberration produced by the other lens 6.

Abstract: A charged particle beam apparatus produces little reduction in resolution when the beam is inclined with respect to a sample. The trajectory of a primary beam 4 is deflected by a deflector or changed by a movable aperture such that the beam is incident on a plurality of lenses 6 and 7 off the axes thereof. A means is provided to control the off-axis trajectory of the beam such that an aberration produced by the objective lens 7 when the beam is inclined can be canceled by an aberration produced by the other lens 6.

Abstract: The present invention has the object of providing a charged particle beam irradiation method ideal for reducing the focus offset, magnification fluctuation and measurement length error in charged particle beam devices. To achieve these objects, a method is disclosed in the invention for measuring the electrical potential distribution on the sample with a static electrometer while loaded by a loader mechanism. Another method is disclosed for measuring the local electrical charge at specified points on the sample, and isolating and measuring the wide area electrostatic charge quantity from those local electrostatic charges.

Abstract: It is an object of the present invention to obtain an image which is focused on all portions of a sample and to provide a charged particle beam apparatus capable of obtaining a two-dimensional image which has no blurred part over an entire sample. In order to achieve the above object, the present invention comprises means for changing a focus condition of a charged particle beam emitted from a charged particle source, a charged particle detector for detecting charged particles irradiated from a surface portion of said sample in response to the emitted charged particle beam, and means for composing a two-dimensional image of the surface portion of the sample based on signals on which said charged particle beam is focused, said signals being among signals output from the charged particle detector.

Abstract: It is an object of the present invention to obtain an image which is focused on all portions of a sample and to provide a charged particle beam apparatus capable of obtaining a two-dimensional image which has no blurred part over an entire sample. In order to achieve the above object, the present invention comprises means for changing a focus condition of a charged particle beam emitted from a charged particle source, a charged particle detector for detecting charged particles [obtained at] irradiated from a surface portion of said sample [irradiated with] in response to the emitted charged particle beam, and means for composing a two-dimensional image of the surface portion of the sample [as viewed from a direction of said charged particle beam source,] based on signals on which said charged particle beam is focused, said signals being among signals output from the charged particle detector.

Abstract: The present invention has the object of providing a charged particle beam irradiation method ideal for reducing the focus offset, magnification fluctuation and measurement length error in charged particle beam devices. To achieve these objects, a method is disclosed in the invention for measuring the electrical potential distribution on the sample with a static electrometer while loaded by a loader mechanism. Another method is disclosed for measuring the local electrical charge at specified points on the sample, and isolating and measuring the wide area electrostatic charge quantity from those local electrostatic charges.

Abstract: The present invention is intended to prevent the deterioration of resolution due to increase in off-axis aberration resulting from the deviation of a primary electron bean from the optical axis of a scanning electron microscope. A scanning electron microscope is provided with an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector disposed at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed and dimensions can be measured in a high accuracy. The SEM is able to achieving precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.

Abstract: A scanning electron microscope with an energy filter which can positively utilize secondary electrons and/or reflected electrons which collide against a mesh electrode and are lost. The scanning electron microscope which has a porous electrode for producing an electric field for energy-filtering electrons produced by applying a primary electron beam to a sample and a 1st electron detector which detects electrons passing through the porous electrode is characterized by further having a porous structure provided near the sample, a deflector which deflects electrons from the axis of the primary electron beam, and a 2nd electron detector which detects the electrons deflected by the deflector.

Abstract: The present invention is intended to prevent the deterioration of resolution due to increase in off-axis aberration resulting from the deviation of a primary electron bean from the optical axis of a scanning electron microscope. A scanning electron microscope is provided with an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector disposed at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed and dimensions can be measured in a high accuracy. The SEM is able to achieving precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.

Abstract: The present invention relates to a scanning electron microscope employing a deceleration field forming technology (retarding), more particularly a scanning electron microscope which separates and detects secondary electrons at high efficiency. The object of the present invention is accomplished by providing an electron source, a lens for condensing the primary electron beam which is emitted from said electron source, a detector for detecting electrons which are generated by radiation of the primary electron beam onto a specimen, a first deceleration means for decelerating the primary electron beam which is radiated onto said specimen, a second deceleration means for decelerating electrons which are generated on the specimen, and a deflector for deflecting said electrons which are decelerated by said second decelerating means.

Abstract: An object of the present invention is to provide a charged particle beam apparatus and an alignment method of the charged particle beam apparatus, which make it possible to align an optical axis of a charged particle beam easily even when a state of the charged particle beam changes. The present invention comprises calculation means for calculating a deflection amount of an alignment deflector which performs an axis alignment for an objective lens, a plurality of calculation methods for calculating the deflection amount is memorized in the calculation means, and a selection means for selecting at least one of the calculation methods is provided.

Abstract: A scanning electron microscope with an energy filter which can positively utilize secondary electrons and/or reflected electrons which collide against a mesh electrode and are lost. The scanning electron microscope which has a porous electrode for producing an electric field for energy-filtering electrons produced by applying a primary electron beam to a sample and a 1st electron detector which detects electrons passing through the porous electrode is characterized by further having a porous structure provided near the sample, a deflector which deflects electrons from the axis of the primary electron beam, and a 2nd electron detector which detects the electrons deflected by the deflector.

Abstract: The present invention has the object of providing a charged particle beam irradiation method ideal for reducing the focus offset, magnification fluctuation and measurement length error in charged particle beam devices.

Abstract: The present invention is intended to prevent the deterioration of resolution due to increase in off-axis aberration resulting from the deviation of a primary electron bean from the optical axis of a scanning electron microscope. A scanning electron microscope is provided with an image shifting deflector system including two deflectors disposed respectively at upper and lower stages. The deflector disposed at the lower stage is a multipole electrostatic deflecting electrode and is disposed in an objective. Even if the distance of image shifting is great, an image of a high resolution can be formed and dimensions can be measured in a high accuracy. The SEM is able to achieving precision inspection at a high throughput when applied to inspection in semiconductor device fabricating processes that process a wafer having a large area and provided with very minute circuit elements.