https://doi.org/10.1140/epjb/e2014-50499-y
Regular Article
Hard X-ray photoemission study of the Fabre salts (TMTTF)2X (X = SbF6 and PF6)
1 Institut für Physik, Johannes
Gutenberg-Universität, 55099
Mainz,
Germany
2 Instituto de Geociências e Ciências
Exatas – IGCE, Unesp – Univ Estadual Paulista, Departamento de Física, Caixa Postal
178, 13506-900
Rio Claro ( SP), Brazil
3 Deutsches Elektronen-Synchrotron
DESY, Notkestr. 85,
22607
Hamburg,
Germany
4 Physikalisches Institut,
Goethe-Universität, 60438
Frankfurt,
Germany
5 Laboratoire de Physique des Solides,
Université Paris-Sud, CNRS UMR-8502, 91405
Orsay,
France
a e-mail: medyanyk@uni-mainz.de
Received:
24
July
2014
Received in final form:
15
September
2014
Published online:
3
November
2014
Core-level photoemission spectra of the Fabre salts with X = SbF6 and PF6 were taken using hard X-rays from PETRA III, Hamburg. In these salts TMTTF layers show a significant stack dimerization with a charge transfer of 1e per dimer to the anion SbF6 or PF6. At room temperature and slightly below the core-level spectra exhibit single lines, characteristic for a well-screened metallic state. At reduced temperatures progressive charge localization sets in, followed by a 2nd order phase transition into a charge-ordered ground state. In both salts groups of new core-level signals occur, shifted towards lower kinetic energies. This is indicative of a reduced transverse-conductivity across the anion layers, visible as layer-dependent charge depletion for both samples. The surface potential was traced via shifts of core-level signals of an adsorbate. A well-defined potential could be established by a conducting cap layer of 5 nm aluminum which appears “transparent” due to the large probing depth of HAXPES (8–10 nm). At the transition into the charge-ordered phase the fluorine 1s line of (TMTTF)2SbF6 shifts by 2.8 eV to higher binding energy. This is a spectroscopic fingerprint of the loss of inversion symmetry accompanied by a cooperative shift of the SbF6 anions towards the more positively charged TMTTF donors. This shift does not occur for the X = PF6 compound, most likely due to smaller charge disproportion or due to the presence of charge disorder.
Key words: Solid State and Materials
© EDP Sciences, Società Italiana di Fisica, Springer-Verlag, 2014