K-edge

Figure Bl.22.10. Carbon K-edge near-edge x-ray absorption (NEXAFS) speetra as a fiinotion of photon ineidenee angle from a submonolayer of vinyl moieties adsorbed on Ni(lOO) (prepared by dosing 0.2 1 of ethylene on that surfaee at 180 K). Several eleetronie transitions are identified in these speetra, to both the pi (284 and 286 eV) and the sigma (>292 eV) imoeeupied levels of the moleeule. The relative variations in the intensities of those peaks with ineidenee angle ean be easily eonverted into adsorption geometry data the vinyl plane was found in this ease to be at a tilt angle of about 65° from the surfaee [71], Similar geometrieal detenninations using NEXAFS have been earried out for a number of simple adsorbate systems over the past few deeades.

Figure C2.10.5. Magnitude of the Fourier transfonn of tire /c-weighted absorjDtion fine stmcture k (/c) measured at tire Cu K edge for tire underiDotential deposition of Cu/Au(l 11) from 0.1 M KCIO +IO M HCIO +S x 10 M Cu (010 )2+10 M potassium salt of sulfate, chloride, bromide and a mixture of sulfate and chloride, for polarization of tire x-rays parallel to tire sample surface ( ) or parallel to tire surface nonnal (E (from [81]).

Figure 2 Molybdenum K-edge X-ray absorption spectrum, ln(i /i ) versus X-ray energy (eV), for molybdenum metal foil (25- jjn thick), obtained by transmission at 77 K with synchrotron radiation. The energy-dependent constructive and destructive interference of outgoing and backscattered photoelectrons at molybdenum produces the EXAFS peaks and valleys, respectively. The preedge and edge structures marked here are known together as X-ray absorption near edge structure, XANES and EXAFS are provided in a new compilation of literature entitled X-rsy Absorption Fine Structure (S.S. Hasain, ed.) Ellis Norwood, New York, 1991.

Figures Background-subtracted, normalized, and ili -weighted Mo K-edge EXAFS, versus k (A ), for molybdenum metal foil obtained from the primary experimental data of Figure 2 with Eq = 20,025 eV.

Figures Fourier transform (soiid curve), Osir ) versus r (A, without phase-shift correction), of the Mo K-edge EXAFS of Figure 5 for moiybdenum metal foii. The Fourier filtering window (dashed curve) is applied over the region -1.5-4.0 A to isolate the two nearest Mo-Mo peaks.

It is known that thin (-20 A) passive films form on iron, nickel, chromium, and other metals. In s ressive environments, these films provide excellent corrosion protection to the underlying metal. The structure and composition of passive films on iron have been investigated through iron K-edge EXAFS obtained under a variety of conditions, yet there is still some controversy about the exact nature of... 

Rgure 5 NEXAFS spectra above the C K-edge for a saturation coverage of pyridine C5H5N on Pt(111), measured at two different polarisation angles with the X-ray beam at normal incidence and at 20° to the sample surface. 

Figure 6 NEXAFS spectra above the C K-edge for the polymers PMPO poly (dimethyl...

Fig. 2.39. Fi ne structures of inner-shell edges (A) Al-K edge of AI4C3 exhibiting ELNES and EXELFS, (B) O-K ELNES of different titanates and Ti-containing silicates.

The accuracy achievable by the ratio method amounts to approximately 5-10 atom% when ionization edges of the same type are used, i. e. only K edges or only L edges, whereas the error in quantification increases to +15-20 atom% for the use of dissimilar edges. Improvement of the quantification accuracy up to approximately 1 atom% is possible if standards are used. 

Fig, 6. EEL spectra of bundle of four SWCNTs, MWCNT and graphite in the energy ranges (a) from 0 to 45 eV (plasmon region) and (b) from 280 to 300 eV (carbon K-edge) (modified from ref. 14). 

Dent et al. [47] also investigated the V K-edge EXAFS for the dissolution of [EMIM][VOCl4] and [NEt4][V02Cl2] in basic [EMIM]C1/A1C13 and compared the data with those of solid samples. In both cases the dissolved and the solid samples showed similar EXAFS and no coordination of the chloroaluminate species to, for example, the vanadyl oxygen was found. 

Brouder, C., Alouani, M and Bennemann, K. H., 1996, Multiple-scattering theory of x-ray magnetic circular dlchroism Implementation and results for iron K-edge , Phys. Rev. B 54 7334. 

The experiments were performed at the energy dispersive absorption beam line of the DCI ring at LURE. In figure 1 we have plotted the XAFS and XMCD signals at the nickel K-edge. 

Figure 1. Thin line experimental XAFS at Ni K-edge in CsNi[Cr(CN)J,2H20 Thick line experimental XMCD spectra at Ni K-edge in CsNi[Cr(CN)gl,2H20...

Figure 3. Experimental (thin line) and theoretical (thick line) XMCD spectra at Cr K-edge in CsNi[Cr(CN)6],2H20.

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