Abstract: For a novice user to easily recognize a difference between imaging results caused by a difference between observation conditions, a computer has an operation screen display observation target setting buttons for changing an observation condition for a specimen including a combination of parameter setting values of a charged particle beam apparatus. The processing unit has the operation screen display a radar chart including a characteristic, indicated by three or more incompatible items, of an observation condition for each of the observation target setting buttons. The radar chart indicates at least items of high resolution, emphasis on surface structure and emphasis on material difference.

Abstract: The sample 3 is tilted/oscillated with respect to the optical axis (Z-axis) of the ion beam 2 to repeat tilt and tilt/restoration of a processing target surface 3a of the sample 3 between a surface state in which the processing target surface 3a of the sample 3 faces a tilt axis direction (Y-axis direction) and a tilted surface state in which a portion of the processing target surface 3a on the sample stage side protrudes in the tilt axis direction (Y-axis direction) than does a portion of the processing target surface 3 on the mask side, so that the processing target surface 3a is irradiated with the ion beam 2 at a low angle, and projections/recesses 63 derived from a void 61 or a dissimilar material 62 are suppressed. Accordingly, it is possible to suppress generation of projections/recesses derived from a void or dissimilar material in fabrication of a cross section sample, and thus fabricate a sample cross section suitable for observation/analysis.

Abstract: The electrical charging by a primary electronic is inhibited to produce a clear edge contrast from an observation specimen (i.e., a specimen to be observed), whereby the shape of the surface of a sample can be measured with high accuracy. An observation specimen in which a liquid medium comprising an ionic liquid is formed in a thin-film-like or a webbing-film-like form on a sample is used. An electron microscopy using the observation specimen comprises: a step of measuring the thickness of a liquid medium comprising an ionic liquid on a sample; a step of controlling the conditions for irradiation with a primary electron on the basis of the thickness of the liquid medium comprising the ionic liquid; and a step of irradiating the sample with the primary electron under the above-mentioned primary electron irradiation conditions to form an image of the shape of the sample.

Abstract: A charged particle beam apparatus is provided with a parameter adjustment practice function for allowing any user to easily learn manual focus adjustment and stigma adjustment. Control conditions of the focus arrangement of an objective lens, an X-stigmator and a Y-stigmator are set according to the user's operation. According to a group of the focus adjustment, an X-stigma adjustment and a Y-stigma adjustment which are set, a practice-purpose image corresponding to the control conditions is read out from a storage device and is displayed on a screen.

Abstract: For a novice user to easily recognize a difference between imaging results caused by a difference between observation conditions, a computer has an operation screen display observation target setting buttons for changing an observation condition for a specimen including a combination of parameter setting values of a charged particle beam apparatus. The processing unit has the operation screen display a radar chart including a characteristic, indicated by three or more incompatible items, of an observation condition for each of the observation target setting buttons. The radar chart indicates at least items of high resolution, emphasis on surface structure and emphasis on material difference.

Abstract: The electrical charging by a primary electronic is inhibited to produce a clear edge contrast from an observation specimen (i.e., a specimen to be observed), whereby the shape of the surface of a sample can be measured with high accuracy. An observation specimen in which a liquid medium comprising an ionic liquid is formed in a thin-film-like or a webbing-film-like form on a sample is used. An electron microscopy using the observation specimen comprises: a step of measuring the thickness of a liquid medium comprising an ionic liquid on a sample; a step of controlling the conditions for irradiation with a primary electron on the basis of the thickness of the liquid medium comprising the ionic liquid; and a step of irradiating the sample with the primary electron under the above-mentioned primary electron irradiation conditions to form an image of the shape of the sample.

Abstract: In recent years, a range of users for a charged particle beam apparatus such as a scanning electron microscope has been broadened. All users want to learn a manual adjustment technology, but it is very difficult to adjust all parameters for observation to have an appropriate value. Therefore, a beginner is unlikely to sufficiently show a performance of an apparatus. This disclosure aims to provide the charged particle beam apparatus including a parameter adjustment practice function for allowing any user to easily learn the manual adjustment technology. In order to solve the above-described problem, there is provided means for practicing a focus adjustment and a stigma adjustment. Control conditions of the focus arrangement of an objective lens, an X-stigmator and a Y-stigmator are set according to the user's operation.

Abstract: The sample 3 is tilted/oscillated with respect to the optical axis (Z-axis) of the ion beam 2 to repeat tilt and tilt/restoration of a processing target surface 3a of the sample 3 between a surface state in which the processing target surface 3a of the sample 3 faces a tilt axis direction (Y-axis direction) and a tilted surface state in which a portion of the processing target surface 3a on the sample stage side protrudes in the tilt axis direction (Y-axis direction) than does a portion of the processing target surface 3 on the mask side, so that the processing target surface 3a is irradiated with the ion beam 2 at a low angle, and projections/recesses 63 derived from a void 61 or a dissimilar material 62 are suppressed. Accordingly, it is possible to suppress generation of projections/recesses derived from a void or dissimilar material in fabrication of a cross section sample, and thus fabricate a sample cross section suitable for observation/analysis.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.

Abstract: There is disclosed a charged particle beam device which judges whether or not an image based on a dark-field signal has an appropriate atomic number contrast. Input reference information, a bright-field image or a back-scattered electron image is compared with a dark-field image, and it is judged whether or not a correlation value between them or the dark-field image has a predetermined contrast. According to such a constitution, it is possible to obtain information by which it is judged whether or not the dark-field image has an appropriate atomic number contrast.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.

Abstract: There is disclosed a charged particle beam device which judges whether or not an image based on a dark-field signal has an appropriate atomic number contrast. Input reference information, a bright-field image or a back-scattered electron image is compared with a dark-field image, and it is judged whether or not a correlation value between them or the dark-field image has a predetermined contrast. According to such a constitution, it is possible to obtain information by which it is judged whether or not the dark-field image has an appropriate atomic number contrast.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.

Abstract: The charged particle beam device of this invention separately detects secondary signal particles emitted from the surface of a sample, dark field signal particles scattered within and transmitted through the sample, bright field signal particles transmitted through the sample without being scattered within the sample, and thereby allows the operator to observe the image with an optimum contrast according to applications. In order to detect only the dark field transmitted signal particles scattered within the sample, among the transmitted signal particles obtained by the primary charged particle beams having transmitted through the thin film sample, the device includes a transmitted signal conversion member having an opening through which the bright field transmitted signal particles not being scattered within the sample can pass, and a detection means for detecting signals colliding against the conversion member.