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    Near-Edge X‑ray Absorption Fine Structure Investigation of the Quasi-One-Dimensional Organic Conductor (TMTSF)<sub>2</sub>PF<sub>6</sub>

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    We present high-resolution near-edge X-ray absorption fine structure (NEXAFS) measurements at the P L<sub>2/3</sub> edges, F K edge, C K edge, and Se M<sub>2/3</sub> edges of the quasi-one-dimensional (1D) conductor and superconductor (TMTSF)<sub>2</sub>PF<sub>6</sub>. NEXAFS allows probing the donor and acceptor moieties separately; spectra were recorded between room temperature (RT) and 30 K at normal incidence. Spectra taken around RT were also studied as a function of the angle (θ) between the electric field of the X-ray beam and the 1D conducting direction. In contrast with a previous study of the S L<sub>2/3</sub>-edges spectra in (TMTTF)<sub>2</sub>AsF<sub>6</sub>, the Se M<sub>2/3</sub> edges of (TMTSF)<sub>2</sub>PF<sub>6</sub> do not exhibit a well-resolved spectrum. Surprisingly, the C K-edge spectra contain three well-defined peaks exhibiting strong and nontrivial θ and temperature dependence. The nature of these peaks as well as those of the F K-edge spectra could be rationalized on the basis of first-principles DFT calculations. Despite the structural similarity, the NEXAFS spectra of (TMTSF)<sub>2</sub>PF<sub>6</sub> and (TMTTF)<sub>2</sub>AsF<sub>6</sub> exhibit important differences. In contrast with the case of (TMTTF)<sub>2</sub>AsF<sub>6</sub>, the F K-edge spectra of (TMTSF)<sub>2</sub>PF<sub>6</sub> do not change with temperature despite stronger donor–anion interactions. All these features reveal subtle differences in the electronic structure of the TMTSF and TMTTF families of salts
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