2013
DOI: 10.1103/physrevb.87.115114
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Coupled valence and spin state transition in (Pr0.7Sm0.3)0.7

Abstract: The coupled valence and spin state transition (VSST) taking place in (Pr0.7Sm0.3)0.7Ca0.3CoO3 was investigated by soft x-ray absorption spectroscopy (XAS) experiments carried out at the Pr-M4,5, Co-L2,3, and O-1s edges. This VSST is found to be composed of a sharp Pr/Co valence and Co spin state transition centered at T*=89.3 K, followed by a smoother Co spin-state evolution at higher temperatures. At T < T*, we found that the praseodymium displays a mixed valence Pr3+/Pr4+ with about 0.13 Pr4+/f.u., while all… Show more

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Cited by 43 publications
(42 citation statements)
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“…For the prototypical compound Pr 0.5 Ca 0.5 CoO 3 this valence shift was confirmed and determined quantitatively with the identification of the Pr 4þ -related Schottky peak in heat capacity measurements 12 and by X-ray absorption spectroscopy at the Pr L 3 edge. 13 Similar evidence was presented also for the Pr 0.7 Ca 0.3 CoO 3 systems doped by Y, [14][15][16] Sm, 17 and Tb. 18 Many studies have been done especially on the (Pr 1Ày Y y ) 0.7 Ca 0.3 CoO 3 system, which displays a MI-SS transition and partial Pr 3þ !…”
Section: Introductionsupporting
confidence: 76%
“…For the prototypical compound Pr 0.5 Ca 0.5 CoO 3 this valence shift was confirmed and determined quantitatively with the identification of the Pr 4þ -related Schottky peak in heat capacity measurements 12 and by X-ray absorption spectroscopy at the Pr L 3 edge. 13 Similar evidence was presented also for the Pr 0.7 Ca 0.3 CoO 3 systems doped by Y, [14][15][16] Sm, 17 and Tb. 18 Many studies have been done especially on the (Pr 1Ày Y y ) 0.7 Ca 0.3 CoO 3 system, which displays a MI-SS transition and partial Pr 3þ !…”
Section: Introductionsupporting
confidence: 76%
“…In order to further investigate the difference of electronic structures, X‐ray absorption spectroscopy of Co L‐edge was performed. In the spectra as shown in Figure a,b and Figure S6 (Supporting Information, the L 3 edge peak includes contributions from Co 2+ (Td) , Co 3+ (Oh, LS) , and Co 3+ (Oh, HS) (HS and LS stand for high spin and low spin, respectively) . We noticed a more intensive shoulder at around 777780 eV in PE‐ z ‐Co 3 O 4 as compared to that in Co 3 O 4 , which could be assigned to the increase of either the Co 2+ /Co 3+ ratio and/or high‐spin Co 3+ content.…”
Section: Resultsmentioning
confidence: 85%
“…Hence, increased Co 2+ /Co 3+ ratio would unlikely be the main cause for the more intensive shoulder observed in the Co L 3 edge spectrum of PE‐ z ‐Co 3 O 4 . The cobalt L 3 edge peak can be further deconvoluted to Co 2+ (Td) , Co 3+ (Oh, LS) , and Co 3+ (Oh, HS) (Figure a,b), which exhibits a much higher content of Co 3+ (Oh, HS) in PE‐ z ‐Co 3 O 4 as compared to that in Co 3 O 4 (conventional spinel). The higher content of Co 3+ (Oh, HS) in PE‐ z ‐Co 3 O 4 can be attributed to the structural distortion induced by surface ZIF‐67 transformation as ZIF‐67 has larger lattice constants than that of the substrate.…”
Section: Resultsmentioning
confidence: 99%
“…The bulk electronic structure of pristine and cycled LiNi 0.5 Mn 1.5 O 4 is revealed by soft X‐ray absorption spectroscopy (XAS) at the O‐K edge using a bulk sensitive fluorescence yield (FY) mode (Figure b). The O‐K XAS spectra of 3d transition metal (TM) oxides is also sensitive to the electronic structure of 3d TM ions . O‐K XAS spectra of SrMnO 3 and NiO is used as a Mn 4+ reference and a Ni 2+ reference, respectively.…”
Section: Resultsmentioning
confidence: 99%