Abstract: Provided is a scanning electron microscope provided with an energy selection and detection function for a SE1 generated on a sample while suppressing the detection amount of a SE3 excited due to a BSE in the scanning electron microscope that does not apply a deceleration method.

Abstract: A charged particle beam device includes: a charged particle source that emits a charged particle beam; a boosting electrode disposed between the charged particle source and a sample to form a path of the charged particle beam and to accelerate and decelerate the charged particle beam; a first pole piece that covers the boosting electrode; a second pole piece that covers the first pole piece; a first lens coil disposed outside the first pole piece and inside the second pole piece to form a first lens; a second lens coil disposed outside the second pole piece to form a second lens; and a control electrode formed between a distal end portion of the first pole piece and a distal end portion of the second pole piece to control an electric field formed between the sample and the distal end portion of the second pole piece.

Abstract: To provide a scanning electron microscope having an electron spectroscopy system to attain high spatial resolution and a high secondary electron detection rate under the condition that energy of primary electrons is low, the scanning electron microscope includes: an objective lens 105; primary electron acceleration means 104 that accelerates primary electrons 102; primary electron deceleration means 109 that decelerates the primary electrons and irradiates them to a sample 106; a secondary electron deflector 103 that deflects secondary electrons 110 from the sample to the outside of an optical axis of the primary electrons; a spectroscope 111 that disperses secondary electrons; and a controller that controls application voltage to the objective lens, the primary electron acceleration means and the primary electron deceleration means so as to converge the secondary electrons to an entrance of the spectroscope.

Abstract: The purpose of the present invention is to eliminate the effort in placement and extraction of samples in observations using transmitted charged particles. A charged particle beam device (601) is characterized by having: a charged particle optical lens tube that irradiates a sample (6) with a primary charged particle beam; a sample stage on which a light emitting member (500) that emits light because of charged particles that have come by transmission internally in the sample (6) or scattering therefrom or a sample platform (600) having the light emitting member (500) is attachably and detachably disposed; and a detector (503) that detects the light emitted by the light emitting member.

Abstract: This composite charged particle beam device comprises a first charged particle beam column (6), a second charged particle beam column (1) which is equipped with a deceleration system, and is equipped with a detector (3) inside the column, a test piece stage (10) on which a test piece (9) is placed, and an electric field correction electrode (13) which is provided around the tip of the first charged particle beam column, wherein the electric field correction electrode is an electrode that corrects the electric field distribution formed in the vicinity of the test piece, and the electric field correction electrode is positioned between the test piece and the first charged particle beam column, and on the opposite side from the second charged particle beam column with respect to the optical axis of the first charged particle beam column.

Abstract: This composite charged particle beam device comprises a first charged particle beam column (6), a second charged particle beam column (1) which is equipped with a deceleration system, and is equipped with a detector (3) inside the column, a test piece stage (10) on which a test piece (9) is placed, and an electric field correction electrode (13) which is provided around the tip of the first charged particle beam column, wherein the electric field correction electrode is an electrode that corrects the electric field distribution formed in the vicinity of the test piece, and the electric field correction electrode is positioned between the test piece and the first charged particle beam column, and on the opposite side from the second charged particle beam column with respect to the optical axis of the first charged particle beam column.

Abstract: The objective of the present invention is to simply perform image observation through transmitted charged particles. A sample irradiated by a charged particle beam is disposed directly or via a predetermined member on a light-emitting element (23) whereinto charged particles that have traversed or scattered inside the sample enter, causing a light to be emitted therefrom, which is collected and detected efficiently using a light transmission means (203) to generate a transmission charged particle image of the sample.

Abstract: To provide a scanning electron microscope having an electron spectroscopy system to attain high spatial resolution and a high secondary electron detection rate under the condition that energy of primary electrons is low, the scanning electron microscope includes: an objective lens 105; primary electron acceleration means 104 that accelerates primary electrons 102; primary electron deceleration means 109 that decelerates the primary electrons and irradiates them to a sample 106; a secondary electron deflector 103 that deflects secondary electrons 110 from the sample to the outside of an optical axis of the primary electrons; a spectroscope 111 that disperses secondary electrons; and a controller that controls application voltage to the objective lens, the primary electron acceleration means and the primary electron deceleration means so as to converge the secondary electrons to an entrance of the spectroscope.

Abstract: The objective of the present invention is to simply perform image observation through transmitted charged particles. A sample irradiated by a charged particle beam is disposed directly or via a predetermined member on a light-emitting element (23) whereinto charged particles that have traversed or scattered inside the sample enter, causing a light to be emitted therefrom, which is collected and detected efficiently using a light transmission means (203) to generate a transmission charged particle image of the sample.

Abstract: The purpose of the present invention is to provide a charged particle gun using merely an electrostatic lens, said charged particle gun being relatively small and having less aberration, and to provide a field emission-type charged particle gun having high luminance even with a high current. This charged particle gun has: a charged particle source; an acceleration electrode that accelerates charged particles emitted from the charged particle source; a control electrode, which is disposed further toward the charged particle source side than the acceleration electrode, and which has a larger aperture diameter than the aperture diameter of the acceleration electrode; and a control unit that controls, on the basis of a potential applied to the acceleration electrode, a potential to be applied to the control electrode.

Abstract: This scanning electron microscope is provided with: a deceleration means that decelerates an electron beam (5) when the electron beam is passing through an objective lens; and a first detector (8) and a second detector (7) that are disposed between the electron beam and the objective lens and have a sensitive surface having an axially symmetric shape with respect to the optical axis of the electron beam. The first detector is provided at the sample side with respect to the second detector, and exclusively detects the signal electrons having a high energy that have passed through a retarding field energy filter (9A). When the distance between the tip (13) at the sample side of the objective lens and the sensitive surface of the first detector is L1 and the distance between the tip at the sample side of the objective lens and the sensitive surface of the second detector is L2, then L1/L2?5/9.

Abstract: This scanning electron microscope is provided with: a deceleration means that decelerates an electron beam (5) when the electron beam is passing through an objective lens; and a first detector (8) and a second detector (7) that are disposed between the electron beam and the objective lens and have a sensitive surface having an axially symmetric shape with respect to the optical axis of the electron beam. The first detector is provided at the sample side with respect to the second detector, and exclusively detects the signal electrons having a high energy that have passed through a retarding field energy filter (9A). When the distance between the tip (13) at the sample side of the objective lens and the sensitive surface of the first detector is L1 and the distance between the tip at the sample side of the objective lens and the sensitive surface of the second detector is L2, then L1/L2?5/9.

Abstract: The purpose of the present invention is to provide a charged particle gun using merely an electrostatic lens, said charged particle gun being relatively small and having less aberration, and to provide a field emission-type charged particle gun having high luminance even with a high current. This charged particle gun has: a charged particle source; an acceleration electrode that accelerates charged particles emitted from the charged particle source; a control electrode, which is disposed further toward the charged particle source side than the acceleration electrode, and which has a larger aperture diameter than the aperture diameter of the acceleration electrode; and a control unit that controls, on the basis of a potential applied to the acceleration electrode, a potential to be applied to the control electrode.

Abstract: The purpose of the present invention is to eliminate the effort in placement and extraction of samples in observations using transmitted charged particles. A charged particle beam device (601) is characterized by having: a charged particle optical lens tube that irradiates a sample (6) with a primary charged particle beam; a sample stage on which a light emitting member (500) that emits light because of charged particles that have come by transmission internally in the sample (6) or scattering therefrom or a sample platform (600) having the light emitting member (500) is attachably and detachably disposed; and a detector (503) that detects the light emitted by the light emitting member.

Abstract: The present invention provides an electron beam apparatus comprising a means for visualizing an axial displacement of a retarding electric field, and a means for adjusting axial displacement. The axial displacement visualizing means includes a reflective plate (6), and an optical system (2, 3) for converging a secondary electron beam (9) on the reflective plate (6), and the axial displacement adjusting means includes an incline rotation mechanism (8) for a sample stage (5). With this configuration, in electron beam apparatuses such as SEM and the like, such problems as visual field displacement caused by displacement of the axial symmetry of the electric field between an objective lens (3) and a sample (4) and inability to measure secondary electrons and reflected electrons that provide desired information can be eliminated.

Abstract: To provide a low acceleration scanning electron microscope that can discriminate and detect reflected electrons and secondary electrons even with a low probe current, this scanning electron microscope is provided with an electron gun (29), an aperture (26), a sample table (3), an electron optical system (4-1) for making an electron beam (31) converge on a sample (2), a deflection means (10), a secondary electron detector (8), a reflected electron detector (9), and a cylindrical electron transport means (5) in a position between the electron gun (29) and sample (2). The reflected electron detector (9) is provided within the electron transport means (5) and on a side further away from the electron gun (29) than the secondary electron detector (8) and the deflection means (10). The reception surface (9-1) of the reflected electron detector (9) is electrically wired so as to have the same potential as the electron transport means (5).

Abstract: To provide a low acceleration scanning electron microscope that can discriminate and detect reflected electrons and secondary electrons even with a low probe current, this scanning electron microscope is provided with an electron gun (29), an aperture (26), a sample table (3), an electron optical system (4-1) for making an electron beam (31) converge on a sample (2), a deflection means (10), a secondary electron detector (8), a reflected electron detector (9), and a cylindrical electron transport means (5) in a position between the electron gun (29) and sample (2). The reflected electron detector (9) is provided within the electron transport means (5) and on a side further away from the electron gun (29) than the secondary electron detector (8) and the deflection means (10). The reception surface (9-1) of the reflected electron detector (9) is electrically wired so as to have the same potential as the electron transport means (5).

Abstract: In order to provide a charged particle beam apparatus that can detect charged particle beam signals in discrimination into a plurality of energy bands, and obtain high-resolution images for each of the energy bands using the signals, the charged particle beam apparatus has a charged particle source (12-1); an aperture (16) that limits the diameter of the charged particle beam (4); optics (14, 17, 19) for the charged particle beam; a specimen holder (21); a charged particle detector (40) that detects secondary charged particles and reflected charged particles from a specimen; and signal calculation unit that processes the output signal from the charged particle detector.

Abstract: The present invention provides an electron beam apparatus comprising a means for visualizing an axial displacement of a retarding electric field, and a means for adjusting axial displacement. The axial displacement visualizing means includes a reflective plate (6), and an optical system (2,3) for converging a secondary electron beam (9) on the reflective plate (6), and the axial displacement adjusting means includes an incline rotation mechanism (8) for a sample stage (5). With this configuration, in electron beam apparatuses such as SEM and the like, such problems as visual field displacement caused by displacement of the axial symmetry of the electric field between an objective lens (3) and a sample (4) and inability to measure secondary electrons and reflected electrons that provide desired information can be eliminated.

Abstract: In order to provide a charged particle beam apparatus that can detect charged particle beam signals in discrimination into a plurality of energy bands, and obtain high-resolution images for each of the energy bands using the signals, the charged particle beam apparatus has a charged particle source (12-1); an aperture (16) that limits the diameter of the charged particle beam (4); optics (14, 17, 19) for the charged particle beam; a specimen holder (21); a charged particle detector (40) that detects secondary charged particles and reflected charged particles from a specimen; and signal calculation unit that processes the output signal from the charged particle detector.