Patent Number: 
Section: claims

1. A transmission electron microscope (TEM) comprising:a high-voltage source configured to supply a high voltage to two high-voltage outputs and and to supply a control signal to a controller output, wherein the control signal is indicative of at least one of a deviation of the supplied high voltage from a reference voltage and temporal fluctuations of the supplied high voltage;an acceleration electrode configured and arranged to accelerate electrons of an electron beam to a kinetic energies corresponding to the high voltage, wherein the acceleration electrode is electrically connected to one of the two high-voltage outputs;a focusing lens configured and arranged to focus the electron beam onto a location in an object plane, wherein the focusing lens is arranged in a beam path of the electron beam system downstream of the acceleration electrode;an energy-dispersive component configured and arranged to deflect electrons of different kinetic energies differently, wherein the energy-dispersive component is arranged in the beam path downstream of the object plane;a detector arranged in the beam path downstream of the energy-dispersive component; anda controller connected to the controller output of the high-voltage source, wherein at least one of the following holds:(a) the controller is configured to control a beam deflector, which is arranged in the beam path downstream of the energy-dispersive component and upstream of the detector, such that a deflective effect of the beam deflector on the electron beam changes in dependence on the control signal supplied by the high-voltage source;(b) the controller is configured to control a monochromator, which is arranged in the beam path upstream of the focusing lens, such that only electrons of the electron beam having a kinetic energies from within an adjustable energy interval are allowed to traverse the monochtomator and such that a central energy of the energy interval changes in dependence on the control signal supplied by the high-voltage source;(c) the controller is configured to control the energy-dispersive component such that a dispersion by the energy-dispersive component changes in dependence on the control signal supplied by the high-voltage source;(d) the controller is configured to collect a plural intensity distributions detected by the detector and to accumulate the plural intensity distributions, wherein the intensity distributions are offset relative to one another by an amount which is determined in dependence on the control signal supplied by the high-voltage source; and(e) the controller is configured to control an actuator configured to displace the detector in a direction transverse to the beam path in dependence on the control signal supplied by the high-voltage source. 2. A method of operating a transmission electron microscope, the method comprising:generating a high voltage;accelerating electrons of an electron beam to a kinetic energies which correspond to the high voltage;directing the electron beam onto an object;measuring intensities of the electrons of the electron beam having interacted with the object in dependence on the kinetic energy of the electrons;detecting deviations of the generated high voltage from a reference voltage; andperforming at least one of:(a) deflecting the electron beam between the object and a detector in dependence on the detected deviations of the generated high voltage;(b) monochromatizing the electron beam such that the kinetic energies of the electrons of the electron beam are in a selected energy interval, and changing the selected energy interval in dependence on the detected deviations;(c) changing a dispersion of an energy-dispersive component traversed by the electron beam in dependence on the detected deviations;(d) repeatedly measuring intensities of the electrons of the electron beam having interacted with the object in dependence on the kinetic energies of the particles, wherein the measured intensities of plural measurements are corrected with respect to the kinetic energies of the electrons in dependence on the detected deviations and wherein the corrected intensities are accumulated to form an accumulated spectrum; and(e) displacing a detector used for measuring the intensities of the electrons relative to the object in dependence on the detected deviations.