Abstract:
A method of operating a Post Column Filter (PCF) in a Scanning/Transmission Electron Microscope, and a Post Column Filter configured to operate according to the method. In an embodiment, the method includes receiving, at an entrance plane, an incoming beam of electrons; dispersing, by an energy dispersive element, the incoming beam of electrons into an energy dispersed beam of electrons; disposing a first plurality of quadrupoles between the entrance plane and a slit plane; operating the PCF in an EELS mode; and operating the PCF in an EFTEM mode. Operating the PCF in an EELS mode includes exciting one or more quadrupoles of the first plurality of quadrupoles at a first excitation level, wherein the first excitation level does not enlarge the energy dispersion of the energy dispersed beam of electrons; and forming an image of the energy dispersed beam of electrons on the image plane, the image being an EELS spectrum. Operating the PCF in the EFTEM mode includes including a slit at the slit plane in an optical path; exciting one or more quadrupoles of the first plurality of quadrupoles at a second excitation level, the second excitation level different from the first excitation level; forming an energy dispersed focus of the energy dispersed beam of electrons on the slit at the slit plane; and enlarging the energy dispersion of the energy dispersed beam of electrons caused by the energy dispersive element based on the one or more first plurality quadrupoles excited at the second excitation level.
Abstract:
A Charged Particle Microscope includes A specimen holder, for holding a specimen; A source, for producing a beam of charged particles; An illuminator, for directing said beam so as to irradiate the specimen; and A detector, for detecting a flux of radiation emanating from the specimen in response to said irradiation. The illuminator includes: An aperture plate comprising an aperture region in a path of said beam, for defining a geometry of the beam prior to its impingement upon said specimen. The aperture region includes a distribution of multiple holes, each of which is smaller than a diameter of the beam incident on the aperture plate.
Abstract:
A method of performing spectroscopy in a Transmission Charged-Particle Microscope comprising: a specimen holder; a source, for producing a beam of charged particles; an illuminator, for directing said beam so as to irradiate the specimen; an imaging system, for directing a flux of charged particles transmitted through the specimen onto a spectroscopic apparatus comprising a dispersing device for dispersing said flux into an energy-resolved array of spectral sub-beams, the method comprising: using an adjustable aperture device to admit a first portion of said array to a detector, while blocking a second portion of said array; providing; using a radiation sensor in said flux upstream of said aperture device to perform localized radiation sensing in a selected region of said second portion of the array, simultaneous with detection of said first portion by said detector; using a sensing result from said sensor to adjust a detection result from said detector.
Abstract:
A Charged Particle Microscope, comprising: includes A specimen holder, for holding a specimen; A source, for producing a beam of charged particles; An illuminator, for directing said beam so as to irradiate the specimen; and A detector, for detecting a flux of radiation emanating from the specimen in response to said irradiation. The illuminator includes: An aperture plate comprising an aperture region in a path of said beam, for defining a geometry of the beam prior to its impingement upon said specimen. The aperture region includes a distribution of multiple holes, each of which is smaller than a diameter of the beam incident on the aperture plate.
Abstract:
The invention relates to a transmission charged particle microscope comprising a charged particle beam source for emitting a charged particle beam, a sample holder for holding a sample, an illuminator for directing the charged particle beam emitted from the charged particle beam source onto the sample, and a control unit for controlling operations of the transmission charged particle microscope. As defined herein, the transmission charged particle microscope is arranged for operating in at least two modes that substantially yield a first magnification whilst keeping said diffraction pattern substantially in focus. Said at least two modes comprise a first mode having first settings of a final projector lens of a projecting system; and a second mode having second settings of said final projector lens.
Abstract:
Molecular structure of a crystal may be solved based on at least two diffraction tilt series acquired from a sample. The two diffraction tilt series include multiple diffraction patterns of at least one crystal of the sample acquired at different electron doses. In some examples, the two diffraction tilt series are acquired at different magnifications.
Abstract:
The invention relates to a system for sensor protection in electron imaging applications comprising a beam control device configured to provide a beam signal based on an incoming beam signal, wherein the beam signal comprises an altered beam intensity, wherein the beam control device is further configured to receive a control signal and to activate based on the control signal. The system further comprises a sensor configured to capture the beam signal and to provide a capture signal based on the beam signal, and a control module configured to provide the control signal to the beam control device, to generate an exposure value based on the capture signal and to modify the control signal based on the exposure value.
Abstract:
The invention relates to a transmission charged particle microscope comprising a charged particle beam source for emitting a charged particle beam, a sample holder for holding a sample, an illuminator for directing the charged particle beam emitted from the charged particle beam source onto the sample, and a control unit for controlling operations of the transmission charged particle microscope. As defined herein, the transmission charged particle microscope is arranged for operating in at least two modes that substantially yield a first magnification whilst keeping said diffraction pattern substantially in focus. Said at least two modes comprise a first mode having first settings of a final projector lens of a projecting system; and a second mode having second settings of said final projector lens.
Abstract:
Various methods and systems are provided for generating an energy resolved chroma image of a sample. Upon irradiated by a charged particle beam, scattered charged particles from the sample are directed to form a first image before entering a spectrometer. The scattered charged particles are then dispersed based on their energy when passing through the spectrometer. The dispersed particles form a second image on a detector. The scattered particles at each location of the first image is spread along a corresponding energy spread vector in the second image.
Abstract:
A method of operating a charged particle microscope comprising the following steps: Providing a specimen on a specimen holder; Using a source to produce a beam of charged particles that is subject to beam current fluctuations; Employing a beam current sensor, located between said source and specimen holder, to intercept a part of the beam and produce an intercept signal proportional to a current of the intercepted part of the beam, the beam current sensor comprising a hole arranged to pass a beam probe with an associated probe current; Scanning said probe over the specimen, thereby irradiating the specimen with a specimen current, with a dwell time associated with each scanned location on the specimen; Using a detector to detect radiation emanating from the specimen in response to irradiation by said probe, and producing an associated detector signal; Using said intercept signal as input to a compensator to suppress an effect of said current fluctuations in said detector signal, wherein: The beam current sensor is configured as a semiconductor device with a sensing layer that is oriented toward the source, in which: Each charged particle of said intercepted part of the beam generates electron/hole pairs in said sensing layer; Generated electrons are drawn to an anode of the semiconductor device; Generated holes are drawn to a cathode of the semiconductor device, thereby producing said intercept signal.