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Relative electron inelastic mean free paths for diamond and graphite at 8 keV and intrinsic contributions to the energy-loss
Authors:C Kunz  BCC Cowie  W Drube  T-L Lee  S Thiess  C Wild  J Zegenhagen
Institution:1. Inst. f. Exp. Physik University Hamburg, Luruper Ch. 149, D-22761 Hamburg, Germany;2. Australian Synchrotron, 800 Blackburn Rd, Clayton, VIC 3168, Australia;3. Deutsches Elektronen Synchrotron, DESY, D-22607 Hamburg, Germany;4. Diamond Light Source Ltd., Didcot, Oxfordshire OX11 0DE, United Kingdom;5. Fraunhofer-Inst. f. Angew. Festkörperphysik, IAF, Tullastraße 72, D-79108 Freiburg, Germany;6. ESRF, F-38043 Grenoble Cedex, France
Abstract:We used hard X-ray photoelectron spectroscopy (HAXPES) with 8 keV X-rays to investigate the 1s emission of carbon. We recorded spectra extending from the peak of the C 1s electrons (“elastic” line) to electrons with up to 110 eV energy-loss. Using two samples side by side, we could compare the inelastic mean free paths (IMFPs) of the electrons of almost 8 keV in diamond and graphite and find them to be practically identical despite about 50% difference in densities. Published extrapolations of their IMFP calculations at lower energies are in good agreement with this result. We show that information from the almost structureless region of overlapping multiple extrinsic energy-losses can be used to quantify the fraction of photoelectrons experiencing intrinsic energy-losses (those due to the sudden creation of the hole). We find that this fraction is 58% of the primary excited C 1s electrons for diamond and is practically the same for graphite. This is at first sight an unexpected result since hole-screening should differ in a semimetal from that in an insulator. The observation can be accounted for by dynamic screening in contrast to static screening.
Keywords:Hard X-ray photoemission  Synchrotron radiation  Electron attenuation lengths  Diamond  Graphite
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