Abstract:
PROBLEM TO BE SOLVED: To provide a method and a device for crystal structure analysis by electron diffraction.SOLUTION: A method and a device for electron diffraction tomography of a crystal sample comprises the steps of: acquiring a series of electron diffraction patterns, in combination with a beam scanning protocol so that a beam converges at every discrete location 42 and 43 of a sample 38, by using scanning of the electron beam over a plurality of discrete locations of the sample; and acquiring a common intensity scaling factor, by using template matching to determine crystal orientations and thickness maps.
Abstract:
PROBLEM TO BE SOLVED: To create improved compositional mapping of samples.SOLUTION: Disclosed is a method, system and program for improving characteristic peak signals in EELS measurement and EDS measurement of crystalline materials. A beam scanning protocol is applied which varies the inclination angle and/or the azimuth angle of the incident beam while spectroscopic data is acquired. The method and system may be applied to compositional mapping.
Abstract:
Devices and methods are described for performing high angle tilting tomography on samples in a liquid medium using transmission electron beam instruments.
Abstract:
A method and system are disclosed for improving characteristic peak signals in electron energy loss spectroscopy (EELS) and energy dispersive x-ray spectroscopy (EDS) measurements of crystalline materials. A beam scanning protocol is applied which varies the inclination, azimuthal angle, or a combination thereof of the incident beam while spectroscopic data is acquired. The method and system may be applied to compositional mapping.
Abstract:
Devices and methods are described for performing high angle tilting tomography on samples in a liquid medium using transmission electron beam instruments.
Abstract:
A method and device for electron diffraction tomography of a crystal sample, which employs scanning of the electron beam over a plurality of discrete locations of the sample, in combination with a beam scanning protocol as the beam converges at every discrete location (42, 43) of the sample (38) to obtain a series of electron diffraction patterns, use of template matching to determine crystal orientations and thickness maps to obtain a common intensity scaling factor.
Abstract:
Devices and methods are described for performing high angle tilting tomography on samples in a liquid medium using transmission electron beam instruments.
Abstract:
A method and system are disclosed for improving characteristic peak signals in electron energy loss spectroscopy (EELS) and energy dispersive x-ray spectroscopy (EDS) measurements of crystalline materials. A beam scanning protocol is applied which varies the inclination, azimuthal angle, or a combination thereof of the incident beam while spectroscopic data is acquired. The method and system may be applied to compositional mapping.
Abstract:
A device and method which enable a transmission electron microscope to measure electron diffraction patterns of a sample very precisely are disclosed. The patterns are suitable for structure determination. The electron beam is precessed by means of deflector coils (6) in the transmission electron microscope before the sample (4), in combination with a similar precession of the electron diffraction pattern by means of deflector coils (9) situated after the sample. The electron diffraction pattern is scanned by means of deflector coils (9) situated after the sample.
Abstract:
A device and method which enable a transmission electron microscope to measure electron diffraction patterns of a sample very precisely are disclosed. The patterns are suitable for structure determination. The electron beam is precessed by means of deflector coils (6) in the transmission electron microscope before the sample (4), in combination with a similar precession of the electron diffraction pattern by means of deflector coils (9) situated after the sample. The electron diffraction pattern is scanned by means of deflector coils (9) situated after the sample.