Sample holder for scanning electron microscope, scanning electron microscope image observation system, and scanning electron microscope image observation method
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.
1. An observation system for imaging an organic material sample in a water solution, wherein:
the organic material sample is interposed between opposing surfaces of a pair of opposing first and second insulative thin films together with the water solution; an electron beam is scan-irradiated to a conductive thin film provided on the outwardly facing surface of the first insulative thin film while the intensity of the electron beam is changed in an on-off pulsed manner; and a potential change on the outwardly facing surface of the second insulative thin film, the potential change corresponding to a difference between the dielectric constant of the organic material sample and the dielectric constant of the water solution, is detected.
2. The observation system according to claim 1 , wherein the electron beam is supplied to the conductive thin film having ground potential from an electron beam gun provided in a scanning electron microscope.
3. The observation system according to claim 1 , wherein signal components of intensity change frequencies are extracted from potential signals, and an image of the potential changes is formed on the basis of the signal components.
4. The observation system according to claim 3 , wherein the electron beam is supplied to the conductive thin film having ground potential from an electron beam gun provided in a scanning electron microscope.
5. The observation system according to claim 3 , wherein a plurality of terminal sections for detecting the potential changes are provided at different positions along the second insulative thin film; an image is formed for each set of the signal components of the intensity change frequencies extracted from each of the terminal sections; an inclination angle of the image is obtained from a positional relation between an incident position of the electron beam and the terminal section; and three-dimensional structure information is obtained by correcting the image on the basis of the inclination angle.
6. The observation system according to claim 5 , wherein the electron beam is supplied to the conductive thin film having ground potential from an electron beam gun provided in a scanning electron microscope.
7. The observation system according to claim 5 , wherein the extraction of the signal components of the intensity change frequencies is carried out by using one of the methods of a band pass filter method, a lock-in amplifier method, an autocorrelation analysis method, and a Fourier transform analysis method.
8. The observation system according to claim 7 , wherein the electron beam is supplied to the conductive thin film having ground potential from an electron beam gun provided in a scanning electron microscope.
9. The observation system according to claim 1 , wherein the water solution is perfused between the opposing surfaces of the first and second insulative thin films.
10. The observation system according to claim 9 , wherein the electron beam is supplied to the conductive thin film having ground potential from an electron beam gun provided in a scanning electron microscope.