10 research outputs found

    Two Novel Acentric Borate Fluorides: M<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> (M = Sr, Ba)

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    Two novel, noncentrosymmetric borate fluorides, Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>, have been synthesized hydrothermally and their structures determined. The compounds are isostructural, crystallizing in space group <i>P</i>2<sub>1</sub>, having lattice parameters of <i>a</i> = 6.4093 (13) Å, <i>b</i> = 8.2898 (17) Å, <i>c</i> = 9.3656 (19) Å, and β = 101.51 (3)° for Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and <i>a</i> = 6.5572 (13) Å, <i>b</i> = 8.5107 (17) Å, <i>c</i> = 9.6726 (19) Å, and β = 101.21 (3)° for Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>. The structure consists of a complex triple-ring borate framework having aligned triangular [BO<sub>3</sub>] groups that impart polarity. Fluorine atoms are bound only to the alkaline-earth metals and are not part of the borate framework, resulting in a vastly different structure from those of the hydrated borates Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> with similar formulas. The title compounds are transparent to nearly 200 nm, making them potentially useful for deep-ultraviolet nonlinear-optical applications

    Two Novel Acentric Borate Fluorides: M<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> (M = Sr, Ba)

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    Two novel, noncentrosymmetric borate fluorides, Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>, have been synthesized hydrothermally and their structures determined. The compounds are isostructural, crystallizing in space group <i>P</i>2<sub>1</sub>, having lattice parameters of <i>a</i> = 6.4093 (13) Å, <i>b</i> = 8.2898 (17) Å, <i>c</i> = 9.3656 (19) Å, and β = 101.51 (3)° for Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and <i>a</i> = 6.5572 (13) Å, <i>b</i> = 8.5107 (17) Å, <i>c</i> = 9.6726 (19) Å, and β = 101.21 (3)° for Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>. The structure consists of a complex triple-ring borate framework having aligned triangular [BO<sub>3</sub>] groups that impart polarity. Fluorine atoms are bound only to the alkaline-earth metals and are not part of the borate framework, resulting in a vastly different structure from those of the hydrated borates Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> with similar formulas. The title compounds are transparent to nearly 200 nm, making them potentially useful for deep-ultraviolet nonlinear-optical applications

    Two Novel Acentric Borate Fluorides: M<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> (M = Sr, Ba)

    No full text
    Two novel, noncentrosymmetric borate fluorides, Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>, have been synthesized hydrothermally and their structures determined. The compounds are isostructural, crystallizing in space group <i>P</i>2<sub>1</sub>, having lattice parameters of <i>a</i> = 6.4093 (13) Å, <i>b</i> = 8.2898 (17) Å, <i>c</i> = 9.3656 (19) Å, and β = 101.51 (3)° for Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and <i>a</i> = 6.5572 (13) Å, <i>b</i> = 8.5107 (17) Å, <i>c</i> = 9.6726 (19) Å, and β = 101.21 (3)° for Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>. The structure consists of a complex triple-ring borate framework having aligned triangular [BO<sub>3</sub>] groups that impart polarity. Fluorine atoms are bound only to the alkaline-earth metals and are not part of the borate framework, resulting in a vastly different structure from those of the hydrated borates Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> with similar formulas. The title compounds are transparent to nearly 200 nm, making them potentially useful for deep-ultraviolet nonlinear-optical applications

    Two Novel Acentric Borate Fluorides: M<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> (M = Sr, Ba)

    No full text
    Two novel, noncentrosymmetric borate fluorides, Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>, have been synthesized hydrothermally and their structures determined. The compounds are isostructural, crystallizing in space group <i>P</i>2<sub>1</sub>, having lattice parameters of <i>a</i> = 6.4093 (13) Å, <i>b</i> = 8.2898 (17) Å, <i>c</i> = 9.3656 (19) Å, and β = 101.51 (3)° for Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and <i>a</i> = 6.5572 (13) Å, <i>b</i> = 8.5107 (17) Å, <i>c</i> = 9.6726 (19) Å, and β = 101.21 (3)° for Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>. The structure consists of a complex triple-ring borate framework having aligned triangular [BO<sub>3</sub>] groups that impart polarity. Fluorine atoms are bound only to the alkaline-earth metals and are not part of the borate framework, resulting in a vastly different structure from those of the hydrated borates Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> with similar formulas. The title compounds are transparent to nearly 200 nm, making them potentially useful for deep-ultraviolet nonlinear-optical applications

    Two Novel Acentric Borate Fluorides: M<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> (M = Sr, Ba)

    No full text
    Two novel, noncentrosymmetric borate fluorides, Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>, have been synthesized hydrothermally and their structures determined. The compounds are isostructural, crystallizing in space group <i>P</i>2<sub>1</sub>, having lattice parameters of <i>a</i> = 6.4093 (13) Å, <i>b</i> = 8.2898 (17) Å, <i>c</i> = 9.3656 (19) Å, and β = 101.51 (3)° for Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub> and <i>a</i> = 6.5572 (13) Å, <i>b</i> = 8.5107 (17) Å, <i>c</i> = 9.6726 (19) Å, and β = 101.21 (3)° for Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>F<sub>2</sub>. The structure consists of a complex triple-ring borate framework having aligned triangular [BO<sub>3</sub>] groups that impart polarity. Fluorine atoms are bound only to the alkaline-earth metals and are not part of the borate framework, resulting in a vastly different structure from those of the hydrated borates Sr<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> and Ba<sub>3</sub>B<sub>6</sub>O<sub>11</sub>(OH)<sub>2</sub> with similar formulas. The title compounds are transparent to nearly 200 nm, making them potentially useful for deep-ultraviolet nonlinear-optical applications

    Synthesis and Spectroscopy of New Plutonium(III) and -(IV) Molybdates: Comparisons of Electronic Characteristics

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    Synthesis of a plutonium­(III) molybdate bromide, PuMoO<sub>4</sub>Br­(H<sub>2</sub>O), has been accomplished using hydrothermal techniques in an inert-atmosphere glovebox. The compound is green in color, which is in stark contrast to the typical blue color of plutonium­(III) complexes. The unusual color arises from the broad charge transfer (CT) spanning from approximately 300 to 500 nm in the UV–vis–near-IR spectra. Repeating the synthesis with an increase in the reaction temperature results in the formation of a plutonium­(IV) molybdate, Pu<sub>3</sub>Mo<sub>6</sub>O<sub>24</sub>(H<sub>2</sub>O)<sub>2</sub>, which also has a broad CT band and red-shifted f–f transitions. Performing an analogous reaction with neodymium produced a completely different product, [Nd­(H<sub>2</sub>O)<sub>3</sub>]­[NdMo<sub>12</sub>O<sub>42</sub>]·2H<sub>2</sub>O, which is built of Silverton-type polyoxometallate clusters

    Synthesis and Spectroscopy of New Plutonium(III) and -(IV) Molybdates: Comparisons of Electronic Characteristics

    No full text
    Synthesis of a plutonium­(III) molybdate bromide, PuMoO<sub>4</sub>Br­(H<sub>2</sub>O), has been accomplished using hydrothermal techniques in an inert-atmosphere glovebox. The compound is green in color, which is in stark contrast to the typical blue color of plutonium­(III) complexes. The unusual color arises from the broad charge transfer (CT) spanning from approximately 300 to 500 nm in the UV–vis–near-IR spectra. Repeating the synthesis with an increase in the reaction temperature results in the formation of a plutonium­(IV) molybdate, Pu<sub>3</sub>Mo<sub>6</sub>O<sub>24</sub>(H<sub>2</sub>O)<sub>2</sub>, which also has a broad CT band and red-shifted f–f transitions. Performing an analogous reaction with neodymium produced a completely different product, [Nd­(H<sub>2</sub>O)<sub>3</sub>]­[NdMo<sub>12</sub>O<sub>42</sub>]·2H<sub>2</sub>O, which is built of Silverton-type polyoxometallate clusters

    Covalency-Driven Dimerization of Plutonium(IV) in a Hydroxamate Complex

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    The reaction of formohydroxamic acid [NH­(OH)­CHO, FHA] with Pu<sup>III</sup> should result in stabilization of the trivalent oxidation state. However, slow oxidation to Pu<sup>IV</sup> occurs, which leads to formation of the dimeric plutonium­(IV) formohydroxamate complex Pu<sub>2</sub>(FHA)<sub>8</sub>. In addition to being reductants, hydroxamates are also strong π-donor ligands. Here we show that formation of the Pu<sub>2</sub>(FHA)<sub>8</sub> dimer occurs via covalency between the 5f orbitals on plutonium and the π* orbitals of FHA<sup>–</sup> anions, which gives rise to a broad and intense ligand-to-metal charge-transfer feature. Time-dependent density functional theory calculations corroborate this assignment

    Covalency-Driven Dimerization of Plutonium(IV) in a Hydroxamate Complex

    No full text
    The reaction of formohydroxamic acid [NH­(OH)­CHO, FHA] with Pu<sup>III</sup> should result in stabilization of the trivalent oxidation state. However, slow oxidation to Pu<sup>IV</sup> occurs, which leads to formation of the dimeric plutonium­(IV) formohydroxamate complex Pu<sub>2</sub>(FHA)<sub>8</sub>. In addition to being reductants, hydroxamates are also strong π-donor ligands. Here we show that formation of the Pu<sub>2</sub>(FHA)<sub>8</sub> dimer occurs via covalency between the 5f orbitals on plutonium and the π* orbitals of FHA<sup>–</sup> anions, which gives rise to a broad and intense ligand-to-metal charge-transfer feature. Time-dependent density functional theory calculations corroborate this assignment

    Spontaneous Partitioning of Californium from Curium: Curious Cases from the Crystallization of Curium Coordination Complexes

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    The reaction of <sup>248</sup>CmCl<sub>3</sub> with excess 2,6-pyridinedicarboxylic acid (DPA) under mild solvothermal conditions results in crystallization of the tris-chelate complex Cm­(HDPA)<sub>3</sub>·H<sub>2</sub>O. Approximately half of the curium remains in solution at the end of this process, and evaporation of the mother liquor results in crystallization of the bis-chelate complex [Cm­(HDPA)­(H<sub>2</sub>DPA)­(H<sub>2</sub>O)<sub>2</sub>Cl]­Cl·2H<sub>2</sub>O. <sup>248</sup>Cm is the daughter of the α decay of <sup>252</sup>Cf and is extracted in high purity from this parent. However, trace amounts of <sup>249,250,251</sup>Cf are still present in all samples of <sup>248</sup>Cm. During the crystallization of Cm­(HDPA)<sub>3</sub>·H<sub>2</sub>O and [Cm­(HDPA)­(H<sub>2</sub>DPA)­(H<sub>2</sub>O)<sub>2</sub>Cl]­Cl·2H<sub>2</sub>O, californium­(III) spontaneously separates itself from the curium complexes and is found doped within crystals of DPA in the form of Cf­(HDPA)<sub>3</sub>. These results add to the growing body of evidence that the chemistry of californium is fundamentally different from that of earlier actinides
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