Synchrotron XPS evidence for Fe2+-S and Fe3+-S surface species on pyrite fracture-surfaces, and their 3D electronic states

Citation
Hw. Nesbitt et al., Synchrotron XPS evidence for Fe2+-S and Fe3+-S surface species on pyrite fracture-surfaces, and their 3D electronic states, AM MINERAL, 85(5-6), 2000, pp. 850-857
Citations number
36
Categorie Soggetti
Earth Sciences
Journal title
AMERICAN MINERALOGIST
ISSN journal
0003004X → ACNP
Volume
85
Issue
5-6
Year of publication
2000
Pages
850 - 857
Database
ISI
SICI code
0003-004X(200005/06)85:5-6<850:SXEFFA>2.0.ZU;2-C
Abstract
A X-ray photoelectron Fe 2p(3/2) spectrum of a pristine pyrite fracture sur face was collected using synchrotron radiation with the source tuned to 800 eV. Comparison of this highly surface sensitive Fe 2p spectrum with Fe 2p spectra collected by conventional means(1487 eV A1k alpha source) reveals t hat the high binding energy tail of the pyrite Fe 2p(3/2) line results prim arily from Fe surfBcr state contributions. The three major contributions to the spectrum are interpreted to be: (1) Fe2+ resident on bulk sires: (2) F e2+ resident on surfaces, edges and corners: (3) Fe3+ surface states produc ed during fracture by an auto-redox reaction involving Fe and S. The intens e main peak is ascribed to the bulk state, whereas the high binding energy tail of the spectrum is composed primarily of Fe2+ and Fe3+ surface state c ontributions. Fe2+ on bulk sites is octahedrally coordinated (O-h symmetry) . All valence electrons of Fe2+ on bulk sires are paired (diamagnetic) and a singlet photopeak at 707 eV is consequently produced. Fracture produces Fe2+ surface states with low er coordination than bulk sites. Fe2+ located at surfaces, edges and corner s experiences modified Ligand Field Stabilization Energies (LFSE) which res ults: in stabilization of the d(7)2 orbital and destabilization of the d(xy ) orbital. Promotion of a d(xy) electron to the d(4)2 orbital makes surface Fe2+ surface states paramagnetic resulting in multiplet splitting of their associated photopeaks. The Fe3+ surface state is necessarily paramagnetic and its photoemissions are consequently multiply split. Analysis of photopeak structures and binding energy splittings of Fe2+ and Fe3+ surface states demonstrates that they are located at the appropriate b inding energies, and span the appropriate energy range, to satisfactorily e xplain the high binding energy tail on of the Fe 2p(M2) spectrum.