Abstract:From stoichiometric amounts of CaO, Fe, and Se, pure powders and single crystals of quaternary [Formula: see text] can be obtained by solid-state reaction and self-flux growth, respectively. The as-synthesized compound exhibits a polymorphic crystal structure, where the two modifications have different stacking sequences of [Formula: see text] layers. The two polymorphs have similar unit cells but different crystal symmetries (Cmc2 and Pnma), of which the former is non-centrosymmetric. Fe is divalent (d) and h… Show more
“…XAS at the 3d transition metal (TM) L 2,3 edges is a very sensitive technique to establish their valence states, spin states, and local symmetries in the solid state matter. − Figure shows that the Fe-L 2,3 XAS spectrum of (a) Sr 2 Fe 3 S 2 O 3 has its main weight at the same energy position as that of an Fe 2+ reference (b) CaFeSeO and (c) Mg 0.94 Fe 0.04 O, but is shifted by 1.6 eV to lower energies with respect to Fe 3+ reference (d) α-Fe 2 O 3 . This confirms an Fe 2+ valence state of Sr 2 Fe 3 S 2 O 3 , agreeing with the expectations from the chemical compositions.…”
Small single crystals of SrFeChO (Ch = S, Se) have been synthesized by flux methods, and bulk materials have been obtained by solid state reactions. Both compounds are isostructural to the compound SrCoSO (space group Pbam), which contains a novel hybrid spin ladder: a combination of a 2-leg rectangular ladder and a necklace ladder. The 2-leg ladder acts as a well-defined magnetic entity, while intimate magnetic coupling to the necklace ladder induces three successive phase transitions in the range of 40-120 K in each composition (Ch = S or Se), as revealed by Mössbauer spectroscopy, thermodynamics, and magnetometry. The complex magnetic behaviors can be explained by the unique spin-lattice topology.
“…XAS at the 3d transition metal (TM) L 2,3 edges is a very sensitive technique to establish their valence states, spin states, and local symmetries in the solid state matter. − Figure shows that the Fe-L 2,3 XAS spectrum of (a) Sr 2 Fe 3 S 2 O 3 has its main weight at the same energy position as that of an Fe 2+ reference (b) CaFeSeO and (c) Mg 0.94 Fe 0.04 O, but is shifted by 1.6 eV to lower energies with respect to Fe 3+ reference (d) α-Fe 2 O 3 . This confirms an Fe 2+ valence state of Sr 2 Fe 3 S 2 O 3 , agreeing with the expectations from the chemical compositions.…”
Small single crystals of SrFeChO (Ch = S, Se) have been synthesized by flux methods, and bulk materials have been obtained by solid state reactions. Both compounds are isostructural to the compound SrCoSO (space group Pbam), which contains a novel hybrid spin ladder: a combination of a 2-leg rectangular ladder and a necklace ladder. The 2-leg ladder acts as a well-defined magnetic entity, while intimate magnetic coupling to the necklace ladder induces three successive phase transitions in the range of 40-120 K in each composition (Ch = S or Se), as revealed by Mössbauer spectroscopy, thermodynamics, and magnetometry. The complex magnetic behaviors can be explained by the unique spin-lattice topology.
“…These close packed layers are stacked parallel with A 2+ layers perpendicular to the hexagonal c -axis, unlike SrZn 2 S 2 O, where the layers are parallel to the hexagonal c -axis. Another example is CaFeSeO, crystallizing in the space group Cmc 2 1 , , which can be considered to be a member of a homologous series (AO)(MQ) n (M = Fe, Zn; n = 1, 2) to which CaFeSeO and SrZn 2 S 2 O belong. CaFeSeO contains puckered sheets consisting of FeSe 2 O 2 tetrahedra located in the ac plane that are also vertically separated by Ca 2+ layers oriented parallel to the hexagonal c axis.…”
Section: Results
and Discussionmentioning
confidence: 99%
“…One of the most useful elements for optical applications is Zn 2+ with a d 10 electron configuration, where for oxychalcogenides, large band gap, optically transparent, polar materials have been reported, including BaZnSO, SrZnSO, and CaZnSO . These compositions are related to several iron and cobalt oxychalcogenide phases, CaFeSO, CaCoSO, and CaFeSeO. ,, The symmetries and tilts of these compositions are quite varied and result in different space groups, for example, BaZnSO ( Cmcm ), SrZnSO ( P 6 3 mc ), CaFeSO ( P 6 3 mc ), CaZnSO ( P 6 3 mc ), CaFeSeO ( Cmc 2 1 ), and CaFeSeO ( Pmcn ); furthermore, multiple polymorphs can crystallize together.…”
Single
crystals of a new zinc oxysulfide SrZn2S2O were
grown in a eutectic KF–KCl flux, and the structure
was determined by single-crystal X-ray diffraction. SrZn2S2O crystallizes in the noncentrosymmetric polar space
group Pmn21 with lattice parameters of a = 3.87440(10) Å, b = 9.9847(3) Å,
and c = 6.0916(2) Å. In the crystal structure,
close-packed corrugated double layers of ZnS3O tetrahedra,
which are derived from the wurtzite structure, are vertically separated
by Sr2+ ions. In addition, the O/S anion ordered arrangement
in each close-packed layer yields two distinct orientations of the
Zn-centered tetrahedra. The crystals of SrZn2S2O are colorless and transparent, and the oxysulfide has a band gap
of 3.86 eV, based on UV–vis–NIR diffuse reflectance
measurements. Thermogravimetric measurements showed that SrZn2S2O is stable up to 650 °C in O2 gas atmosphere. First-principle calculations indicate that the valence
band maximum is mainly composed of O-2p and S-3p states, whereas the
conduction band minimum is derived from Zn-4s, Zn-4p, and Sr-4d states.
The calculated band dispersion reveals a direct band gap corresponding
to a transition between S-3p and Zn-4s energy levels. Second harmonic
generation (SHG) measurements determined that SrZn2S2O is phase matchable with twice the SHG intensity of potassium
dihydrogen phosphate (KDP) in contrast to CaZnSO with similar ZnS3O building units, which exhibits non-phase matching behavior.
“…To date, researchers are interested in the oxychalcogenides based on late transition metals (Fe, Co, Cu, Ag, Zn, Cd) for their abundant physical properties and potential applications. Taking Fe as an example, the reported Fe-based oxychalcogenides include the superconducting [Li 0.8 Fe 0.2 OH][Fe Q ] ( Q = S, Se), − the semiconductive CaFe Q O ( Q = S, Se), − the antiferromagnetic Ln 2 Fe 2 Q 2 O 3 ( Ln = La, Ce; Q = S, Se), and Sr 2 Fe 3 Se 2 O 3 with much complex magnetic ordering. , Even though the oxychalcogenides in the Ln / M /Q/O ( Ln = rare earth metal, M = early transition metals) family have also been explored, researches on their physical properties remain far to be desired. − Hence, more work should focus on the early transition metal oxychalcogenides as well as their physical properties.…”
The layered oxyselenides with the
formula LnCrSe2O (Ln =
Ce–Nd) were synthesized via molten salt methods. The isostructural
compounds crystallize in the monoclinic space group of C2/m. The crystal structures
feature ∞
2[CrSe2O]3– motifs stacked along the a axis, which are separated by Ln
3+ ions. The ∞
2[CrSe2O]3– layers are composed
of [Cr1Se6]9– and [Cr2Se4O2]9– octahedra via corner and edge sharing.
Powder X-ray diffraction results confirm the phase purities of the
as-synthesized compounds. LnCrSe2O (Ln = Ce–Nd) show typical antiferromagnetic ordering
with T
N = 125, 120, and 118 K, respectively.
Heat capacity measurement for NdCrSe2O indicates that the
Debye temperature is 278.4 K. Similar metal-to-semiconductor phase
transitions were observed for LnCrSe2O
(Ln = Ce–Nd) plates with transition temperatures
of 115, 109, and 95 K, respectively. NdCrSe2O also possesses
a magnetoresistance effect at low temperature (<25 K) with a significant
positive magnetoresistance ∼ 16% at 2 K and 1 T.
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