Apparatuses and methods for improved reconstructions of electron-based holograms are disclosed herein. An example method at least includes forming a hologram of a sample and a known object, forming a reconstruction of the known object using a reconstruction algorithm, comparing the reconstruction of the known object to a reference reconstruction of the known object, and adjusting the reconstruction algorithm based on the comparison of the reconstruction of the known object to the reference reconstruction of the known object. The example method may further include forming a reconstruction of the sample using the adjusted reconstruction algorithm.

Apparatuses and methods for comparative holographic imaging to improve structural and molecular information of reconstructions is disclosed herein. An example method at least includes acquiring a plurality of holograms of a sample, wherein each hologram of the plurality of holograms is acquired at a different electron beam energy, and determining atomic and structural information of the sample based at least on a comparison of at least two of the holograms of the plurality of holograms.

A lensless Fourier transform holography high accuracy reconstruction method using a charged particle beam apparatus which holds a sample on a diffraction surface of a diffraction grating provided on the downstream side of a traveling direction of the charged particle beam and which is formed of a material having permeability. The charged particle beam passed through the diffraction surface is image-formed, and the formed image is detected. An opening region of the diffraction grating is smaller than an irradiation region of the charged particle beam on the diffraction grating. Image data is obtained in a state where the irradiation region of the charged particle beam diffracted with the diffraction grating is within the irradiation region of the charged particle beam transmitted through the diffraction grating. Plural holograms obtained based on the image data are Fourier transformed and an intensity distribution image is displayed and stored.

An X-ray imaging apparatus with an interferometer (IF) and an X-ray detector (D). A footprint of the X-ray detector (D) is larger than a footprint of the interferometer (IF). The interferometer is moved in scan motion across the detector (D) whilst the detector (D) remains stationary. Preferably the detector is a 2D full field detector.

The present disclosure concerns an electron microscopy method, including the emission of a precessing electron beam and the acquisition, at least partly simultaneous, of an electron diffraction pattern and of intensity values of X rays.

Method for acquisition of at least one hologram of a sample by off-axis holography using a transmission electron microscope, the microscope comprising an electron beam source, at least one objective lens, a sample holder, at electron biprism and means of displacing the electron beam in precession mode upstream from the sample holder and a compensator of the precession downstream from the sample holder, said method comprising the activation of means of displacing the electron beam in precession mode and the compensator and acquisition of a hologram of said sample in precession mode.

Method for acquisition of at least one hologram of a sample by off-axis holography using a transmission electron microscope, the microscope comprising an electron beam source, at least one objective lens, a sample holder, at electron biprism and means of displacing the electron beam in precession mode upstream from the sample holder and a compensator of the precession downstream from the sample holder, said method comprising the activation of means of displacing the electron beam in precession mode and the compensator and acquisition of a hologram of said sample in precession mode.

Continuous and automatic acquisition of electron beam holograms is made possible by using a sample holding mechanism that includes a sample end region that has a linear shape that is suited for electron beam holography, separates a thin-film rectangular window with an extreme-thin support film that supports a sample being disposed and a rectangular hole that has a linear-shaped edge and through which a reference wave is transmitted from each other, and configures a part of a layer that is thicker than the support film.

Continuous and automatic acquisition of electron beam holograms is made possible by using a sample holding mechanism that includes a sample end region that has a linear shape that is suited for electron beam holography, separates a thin-film rectangular window with an extreme-thin support film that supports a sample being disposed and a rectangular hole that has a linear-shaped edge and through which a reference wave is transmitted from each other, and configures a part of a layer that is thicker than the support film.

A holographic antenna for recording a comprehensive interference pattern beyond the mere minimum and maximum values and reconstructing waveform of a target antenna includes a feed antenna and a holographic structure. The holographic structure includes a substrate and a plurality of spaced metal strips disposed on the substrate. Heights of the metal strips are negatively correlated with intensities of the interference pattern. A method for fabricating such a holographic antenna is also provided.