2002
DOI: 10.1021/ic025992j
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Hydrothermal Preparation, Structures, and NLO Properties of the Rare Earth Molybdenyl Iodates, RE(MoO2)(IO3)4(OH) [RE = Nd, Sm, Eu]

Abstract: The reactions of RE(IO3)3 [RE = Nd, Sm, Eu] with I2O5 and MoO3 in a 1:2:2 molar ratio at 200 degrees C in aqueous media provide access to RE(MoO2)(IO3)4(OH) [RE = Nd (1), Sm (2), Eu (3)] as pure phases as determined from powder X-ray diffraction data. Single crystal X-ray diffraction experiments demonstrate that these compounds are isostructural and crystallize in the chiral and polar space group P2(1). The structures are composed of three-dimensional networks formed from eight-coordinate, square antiprismatic… Show more

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Cited by 111 publications
(81 citation statements)
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“…[27] Cs 2 I 4 O 11 has an SHG efficiency of approximately 300 SiO 2 . This efficiency is comparable to other NCS iodates, including HIO 3 (300 SiO 2 ), [26] LiIO 3 (300 SiO 2 ), [26] NdMoO 2 (IO 3 ) 4 (OH) (350 SiO 2 ), [28] and AMoO 3 (IO 3 ) (A = Rb or Cs, 400 SiO 2 ). [29] By sieving the polycrystalline powder into various particle sizes (20-150 mm) and measuring the SHG as a function of particle size, we were able to determine that Cs 2 I 4 O 11 is non-phasematchable (Type 1).…”
Section: +supporting
confidence: 62%
“…[27] Cs 2 I 4 O 11 has an SHG efficiency of approximately 300 SiO 2 . This efficiency is comparable to other NCS iodates, including HIO 3 (300 SiO 2 ), [26] LiIO 3 (300 SiO 2 ), [26] NdMoO 2 (IO 3 ) 4 (OH) (350 SiO 2 ), [28] and AMoO 3 (IO 3 ) (A = Rb or Cs, 400 SiO 2 ). [29] By sieving the polycrystalline powder into various particle sizes (20-150 mm) and measuring the SHG as a function of particle size, we were able to determine that Cs 2 I 4 O 11 is non-phasematchable (Type 1).…”
Section: +supporting
confidence: 62%
“…For the monoclinic compound 2,t he calculated rotationa ngle between the crystallographic axes and the dielectric principle axes is 25.928.C onsidering the restriction of Kleinman's symmetry,c ompounds 1 (Cmc2 1 )a nd 2 (C2) have three (d 15 To investigate the origin of such strong SHG effects, we have performed the spectral decomposition of d 15 for compound 1 and of d 23 for compound 2,w hich are plottedi nt he bottommost panels of Figure 7. For compound 1,t he most contributing regions are just the upper part of VB (À1.76 0eV) and the bottommost CB (< 3.44 eV) corresponding to the O-2p non-bondings tates mixingw ith small amount of Aud xy states and the unoccupied antibonding states formed by Au-d x 2 Ày 2 and bridged O-2p, respectively.C ompared to compound 1,c ompound 2 has ar elativelyb roaderc ontributed region in the CB, which extends to 5.35 eV.I ts uggests that except the AuÀOa ntibonding states, the I-5p and other O-2p states also give some contributions to the SHG coefficient d 23 in the CB of compound 2.…”
Section: Theoretical Studiesmentioning
confidence: 99%
“…Another effective route for designing new NLO metal iodates is the incorporation of as econd cation into the ternary metal iodates, which affords abundant new structures. [15][16][17][18][19][20][21] Mostly,t ransition-metal ions with d 0 electronic configurations (i.e.,T i 4 + ,N b 5 + ,V 5 + ,M o 6 + ,e tc.) are introducedi nto iodates becauset hey usually form distorted MO 6 (M represent the d 0 transitionm etal)o ctahedra, which are also polar and SHG active.…”
Section: Introductionmentioning
confidence: 99%
“…The lone-pair cation coordination environment may be considered as pre-distorted, [38] as these cations are almost always found in local NCS environments. Halasyamani et al, [38][39][40][41][42][43][44][45][46][47][48][49][50] Norquist et al, [51][52][53] and others [54][55][56][57][58][59][60][61][62][63] have used SOJT-distorted cations in the design and synthesis of new NCS materials.…”
Section: Electronic Distortionsmentioning
confidence: 99%