Abstract:
In a direct electron detector, backscattering of electrons into the detector volume from below the sensor is prevented. In some embodiments, an empty space is maintained below the sensor. In other embodiments, a structure below the sensor includes geometry, such as multiple high aspects ratio channels, either extending to or from the sensor to trap electrons, or a structure of angled surfaces to deflect the electrons that pass through the sensor.
Abstract:
The invention relates to a Method of protecting a direct electron detector (151) in a TEM. The invention involves predicting the current density on the detector before setting new beam parameters, such as changes to the excitation of condenser lenses (104), projector lenses (106) and/or beam energy. The prediction is made using an optical model or a Look-Up-Table. When the predicted exposure of the detector is less than a predetermined value, the desired changes are made, otherwise a warning message is generated and changes to the settings are postponed.
Abstract:
The invention relates to a Method of protecting a direct electron detector (151) in a TEM. The invention involves predicting the current density on the detector before setting new beam parameters, such as changes to the excitation of condenser lenses (104), projector lenses (106) and/or beam energy. The prediction is made using an optical model or a Look-Up-Table. When the predicted exposure of the detector is less than a predetermined value, the desired changes are made, otherwise a warning message is generated and changes to the settings are postponed.
Abstract:
In a direct electron detector, backscattering of electrons into the detector volume from below the sensor is prevented. In some embodiments, an empty space is maintained below the sensor. In other embodiments, a structure below the sensor includes geometry, such as multiple high aspects ratio channels, either extending to or from the sensor to trap electrons, or a structure of angled surfaces to deflect the electrons that pass through the sensor.
Abstract:
A method of using a direct electron detector in a TEM, in which an image with a high intensity peak, such as a diffractogram or an EELS spectrum, is imaged on said detector. As known the high intensity peak may damage the detector. To avoid this damage, the center of the image is moved, as a result of which not one position of the detector is exposed to the high intensity, but the high intensity is smeared over the detector, displacing the high intensity peak before damage results.
Abstract:
A method of using a direct electron detector in a TEM, in which an image with a high intensity peak, such as a diffractogram or an EELS spectrum, is imaged on said detector. As known the high intensity peak may damage the detector. To avoid this damage, the centre of the image is moved, as a result of which not one position of the detector is exposed to the high intensity, but the high intensity is smeared over the detector, displacing the high intensity peak before damage results.