Splitting the plasmon peak in high-energy reflection electron energy loss experiments

被引:7
作者
Vos, M. [1 ]
Went, M. R. [1 ]
机构
[1] Australian Natl Univ, Res Sch Phys Sci & Engn, Atom & Mol Phys Labs, Canberra, ACT 0200, Australia
基金
澳大利亚研究理事会;
关键词
thin films; elastic electron scattering; plasmon excitation;
D O I
10.1016/j.elspec.2007.05.003
中图分类号
O433 [光谱学];
学科分类号
0703 ; 070302 ;
摘要
Elastic scattering of energetic electrons over large angles (in this study 40 keV and 120 degrees) implies momentum and hence energy transfer from an electron to a nucleus. Due to the large mass of the nucleus (relative to the mass of an electron) this energy transfer is small, but it has recently been shown that it can be resolved in a modern spectrometer. Hence the elastic peak of an overlayer/substrate system splits into different components corresponding to atoms with different mass. Here we extend this type of experiment to the plasmon part of a reflection energy loss spectroscopy (REELS) spectrum. It is shown that, for suitable systems, the plasmon peak of an overlayer/substrate system is split by the same amount as the elastic peak. This is a consequence of the fact that detection of an electron in REELS always requires a large-angle elastic scattering event. Moreover, we show that the relative intensity of the plasmon components contains information on the depth distribution of the scatterers. (c) 2007 Elsevier B.V. All rights reserved.
引用
收藏
页码:1 / 7
页数:7
相关论文
共 18 条
[1]  
[Anonymous], SPRINGER TRACTS MODE
[2]   EXPERIMENTAL ENERGY-LOSS FUNCTION, IM[-1/EPSILON(Q,OMEGA)], FOR ALUMINUM [J].
BATSON, PE ;
SILCOX, J .
PHYSICAL REVIEW B, 1983, 27 (09) :5224-5239
[3]  
Egerton R. F., 1996, ELECT ENERGY LOSS SP
[4]   ELSEPA - Dirac partial-wave calculation of elastic scattering of electrons and positrons by atoms, positive ions and molecules [J].
Salvat, F ;
Jablonski, A ;
Powell, CJ .
COMPUTER PHYSICS COMMUNICATIONS, 2005, 165 (02) :157-190
[5]   Calculations of electron inelastic mean free paths. VIII. Data for 15 elemental solids over the 50-2000 eV range [J].
Tanuma, S ;
Powell, CJ ;
Penn, DR .
SURFACE AND INTERFACE ANALYSIS, 2005, 37 (01) :1-14
[6]   CALCULATIONS OF ELECTRON INELASTIC MEAN FREE PATHS (IMFPS) .4. EVALUATION OF CALCULATED IMFPS AND OF THE PREDICTIVE IMFP FORMULA TPP-2 FOR ELECTRON ENERGIES BETWEEN 50 AND 2000 EV [J].
TANUMA, S ;
POWELL, CJ ;
PENN, DR .
SURFACE AND INTERFACE ANALYSIS, 1993, 20 (01) :77-89
[7]  
VOMFELDE A, 1984, PHYS REV LETT, V53, P922, DOI DOI 10.1103/PHYSREVLETT.53.922
[8]   High-energy (e, 2e) spectrometer for the study of the spectral momentum density of materials [J].
Vos, M ;
Cornish, GP ;
Weigold, E .
REVIEW OF SCIENTIFIC INSTRUMENTS, 2000, 71 (10) :3831-3840
[9]   Effects of bonding on the energy distribution of electrons scattered elastically at high momentum transfer [J].
Vos, M. ;
Went, M. R. .
PHYSICAL REVIEW B, 2006, 74 (20)
[10]   Experimental confirmation of the EPES sampling depth paradox for overlayer/substrate systems [J].
Vos, M. ;
Went, M. R. .
SURFACE SCIENCE, 2007, 601 (06) :1536-1543