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The performance evaluation of direct detection electron energy-loss spectroscopy at 200 kV and 80 kV accelerating voltages
•The performance of direct electron detector (K2 IS) has been compared with the charge coupled device (CCD) detector at both 200 kV and 80 kV.•The advantages of using K2 detectors become more obvious when operating at higher accelerating voltage.•The spectroscopic application of direct electron dete...
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Published in: | Ultramicroscopy 2020-05, Vol.212 (C), p.112942-112942, Article 112942 |
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Main Authors: | , , , , , |
Format: | Article |
Language: | English |
Subjects: | |
Citations: | Items that this one cites Items that cite this one |
Online Access: | Get full text |
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Summary: | •The performance of direct electron detector (K2 IS) has been compared with the charge coupled device (CCD) detector at both 200 kV and 80 kV.•The advantages of using K2 detectors become more obvious when operating at higher accelerating voltage.•The spectroscopic application of direct electron detector will help the microscopy field extract bonding and electronic structures of difficult materials (beam sensitive/ charging/ easy contaminated/ fast drifting samples) at higher resolution.
Direct electron detectors (DeDs) have been widely used for imaging studies because of their higher beam sensitivity, lower noise, improved pixel resolution, etc. However, there have been limited studies related to the performance in spectroscopic applications for the direct electron detection. Hereby, taking the advantage of the DeD installed on a high-performance electron energy-loss spectrometer, we systematically studied the performance of a DeD (Gatan's K2 IS) fitted on an aberration-corrected transmission electron microscope (TEM) equipped with an electron monochromator. Using SrTiO3 as the model system, the point spread function in the zero-loss region of the spectrum and the performance for core loss spectroscopy have been investigated under both 200 kV and 80 kV operating conditions. We demonstrate that the K2 detector can achieve an overall better performance at 200 kV than a charge coupled device (CCD) detector. At 80 kV, the K2 DeD is still better than a CCD, except for the relative broad tails of the zero-loss peak. The signal-to-noise ratio is very close for DeD and CCD under 80 kV. Based on our data obtained at different operating voltages, it is clear that DeD will benefit the microscopy community and boost the development of cutting-edge materials science studies by pushing the frontiers in electron energy-loss spectroscopy. |
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ISSN: | 0304-3991 1879-2723 |
DOI: | 10.1016/j.ultramic.2020.112942 |