Abstract:
A water solution in which an observation sample is, for example, dissolved is sandwiched on a first insulative thin film side provided under a conductive thin film. When an electron beam incident part is charged minus, electric dipoles of water molecules are arrayed along a potential gradient. Electric charges are also generated on the surface of a second insulative thin film. The electric charges are detected by a terminal section and changes to a measurement signal. In a state in which an electron beam is blocked, the minus potential disappears. Consequently, the electric charges on the surface of the first insulative thin film also disappear, and the measurement signal output from the terminal section changes to 0.
Abstract:
In an upper main body of a sample holder, a laminate of an insulative thin film and a secondary electron emission protective thin film is provided. An electron beam emitted from an electron gun enters the secondary electron emission protective thin film side. The undersurface of the insulative thin film is a sample adhesion surface, where a sample to be an observation target is held by adsorption or the like. The secondary electron emission protective thin film is made of a material having a low secondary electron emission coefficient δ and, preferably, is non-insulative. That is, the secondary electron emission protective thin film is conductive even though the electric resistance is high. Accordingly, the charge level of a site irradiated with the electron beam has a low charge level.
Abstract:
A risk of breakage of a sample holder can be reduced and a biochemical sample or a liquid sample can be observed easily and with a high observation throughput. A sample holder 101 holding a sample includes: a sample chamber including a first insulating thin film 110 and a second insulating thin film 111 that sandwich and hold the sample 200 in a liquid or gel form and face each other, a vacuum partition wall inside which the sample chamber holding the sample is fixed in a state in which the thin film is exposed to a surrounding atmosphere, and whose internal space is kept at a degree of vacuum at least lower than that of the sample room at the time of observation of the sample, a detection electrode 820 disposed to face the second insulating thin film in a state in which the sample chamber is fixed to the vacuum partition wall, and a signal detection unit 50 connected to the detection electrode. Before the surrounding atmosphere of the sample holder is evacuated from an atmospheric pressure to a vacuum, the charged particle beam device receives a detection signal from the signal detection unit via a connector and detects an abnormality of the sample chamber based on the detection signal.
Abstract:
In an upper main body of a sample holder, a laminate of an insulative thin film and a secondary electron emission protective thin film is provided. An electron beam emitted from an electron gun enters the secondary electron emission protective thin film side. The undersurface of the insulative thin film is a sample adhesion surface, where a sample to be an observation target is held by adsorption or the like. The secondary electron emission protective thin film is made of a material having a low secondary electron emission coefficient δ and, preferably, is non-insulative. That is, the secondary electron emission protective thin film is conductive even though the electric resistance is high. Accordingly, the charge level of a site irradiated with the electron beam has a low charge level.
Abstract:
When injection of electrons into a sample supporting member causes a potential gradient between an insulative thin film and a conductive thin film at a site of electron beam injection, the potential barrier of the surface of the insulative thin film becomes thin, and an electron emission phenomenon is caused by tunnel effects. Secondary electrons caused in the insulative thin film tunnel to the conductive thin film along the potential gradient. The secondary electrons, having tunneled, reach a sample while diffusing in the conductive thin film. In the case where the sample is a sample with a high electron transmittance, such as a biological sample, the secondary electrons also tunnel through the interior of the sample. The secondary electrons are detected to acquire an SEM image in which the inner structure of the sample is reflected.
Abstract:
An image forming method includes: arranging a sample between a first main surface of an insulating thin film and a counter electrode, measuring an impedance value by inputting an AC potential signal to the counter electrode, scanning a physical beam while focusing and irradiating a conductive thin film given to cover a second main surface of the insulating thin film with the physical beam to lower an insulation property of the insulating thin film directly below an irradiation position, guiding the AC potential signal to the irradiation position, and forming an image from the impedance value corresponding to the irradiation position.
Abstract:
When injection of electrons into a sample supporting member causes a potential gradient between an insulative thin film and a conductive thin film at a site of electron beam injection, the potential barrier of the surface of the insulative thin film becomes thin, and an electron emission phenomenon is caused by tunnel effects. Secondary electrons caused in the insulative thin film tunnel to the conductive thin film along the potential gradient. The secondary electrons, having tunneled, reach a sample while diffusing in the conductive thin film. In the case where the sample is a sample with a high electron transmittance, such as a biological sample, the secondary electrons also tunnel through the interior of the sample. The secondary electrons are detected to acquire an SEM image in which the inner structure of the sample is reflected.