3 research outputs found

    Luminescent P‑Chirogenic Copper Clusters

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    P-chirogenic clusters of the cubanes [Cu<sub>4</sub>I<sub>4</sub>L<sub>4</sub>] (L = chiral phosphine) were prepared from (+)- and (−)-ephedrine with L = (<i>S</i>)- or (<i>R</i>)-(R)­(Ph)­(<i>i</i>-Pr)P (with R = CH<sub>3</sub> (seven steps) or C<sub>17</sub>H<sub>35</sub> (10 steps)) with e.e. up to 96%. The X-ray structure of [Cu<sub>4</sub>I<sub>4</sub>((<i>R</i>)-(CH<sub>3</sub>)­(Ph)­(<i>i</i>-Pr)­P)<sub>4</sub>] confirmed the cubane structure with average Cu···Cu and Cu···I distances of 2.954 and 2.696 Å, respectively. The cubane structure of the corresponding [Cu<sub>4</sub>I<sub>4</sub>((<i>S</i>)-(CH<sub>3</sub>)­(Ph)­(<i>i</i>-Pr)­P)<sub>4</sub>] was established by the comparison of the X-ray powder diffraction patterns, and the opposite optical activity of the (<i>S</i>)- and (<i>R</i>)-ligand-containing clusters was confirmed by circular dichroism spectroscopy. Small-angle X-ray scattering patterns of one cluster bearing a C<sub>17</sub>H<sub>35</sub> chain exhibit a weak signal at 2θ ∼ 2.8° (<i>d</i> ∼ 31.6 Å), indicating some molecular ordering in the liquid state. The emission spectra exhibit two emission bands, both associated with triplet excited states. These two bands are assigned as follows: the high energy emission is due to a halide-to-ligand charge transfer, XLCT, state mixed with LXCT (ligand-to-halide-charge-transfer). The low energy band is assigned to a cluster-centered excited state. Both emissions are found to be thermochromic with the relative intensity changing between 77 and 298 K for the clusters in methylcyclohexane solution. Several differences are observed in the photophysical parameters, emission quantum yields and lifetimes for R = CH<sub>3</sub> and C<sub>17</sub>H<sub>35</sub>. The measurements of the polarization along the emission indicate that the emission is depolarized, consistent with an approximate tetrahedral geometry of the chromophores

    Luminescent P‑Chirogenic Copper Clusters

    No full text
    P-chirogenic clusters of the cubanes [Cu<sub>4</sub>I<sub>4</sub>L<sub>4</sub>] (L = chiral phosphine) were prepared from (+)- and (−)-ephedrine with L = (<i>S</i>)- or (<i>R</i>)-(R)­(Ph)­(<i>i</i>-Pr)P (with R = CH<sub>3</sub> (seven steps) or C<sub>17</sub>H<sub>35</sub> (10 steps)) with e.e. up to 96%. The X-ray structure of [Cu<sub>4</sub>I<sub>4</sub>((<i>R</i>)-(CH<sub>3</sub>)­(Ph)­(<i>i</i>-Pr)­P)<sub>4</sub>] confirmed the cubane structure with average Cu···Cu and Cu···I distances of 2.954 and 2.696 Å, respectively. The cubane structure of the corresponding [Cu<sub>4</sub>I<sub>4</sub>((<i>S</i>)-(CH<sub>3</sub>)­(Ph)­(<i>i</i>-Pr)­P)<sub>4</sub>] was established by the comparison of the X-ray powder diffraction patterns, and the opposite optical activity of the (<i>S</i>)- and (<i>R</i>)-ligand-containing clusters was confirmed by circular dichroism spectroscopy. Small-angle X-ray scattering patterns of one cluster bearing a C<sub>17</sub>H<sub>35</sub> chain exhibit a weak signal at 2θ ∼ 2.8° (<i>d</i> ∼ 31.6 Å), indicating some molecular ordering in the liquid state. The emission spectra exhibit two emission bands, both associated with triplet excited states. These two bands are assigned as follows: the high energy emission is due to a halide-to-ligand charge transfer, XLCT, state mixed with LXCT (ligand-to-halide-charge-transfer). The low energy band is assigned to a cluster-centered excited state. Both emissions are found to be thermochromic with the relative intensity changing between 77 and 298 K for the clusters in methylcyclohexane solution. Several differences are observed in the photophysical parameters, emission quantum yields and lifetimes for R = CH<sub>3</sub> and C<sub>17</sub>H<sub>35</sub>. The measurements of the polarization along the emission indicate that the emission is depolarized, consistent with an approximate tetrahedral geometry of the chromophores

    Stereoselective Synthesis of <i>o</i>-Bromo (or Iodo)aryl P-Chirogenic Phosphines Based on Aryne Chemistry

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    The efficient synthesis of chiral or achiral tertiary phosphines bearing an <i>o</i>-bromo (or iodo)­aryl substituent is described. The key step of this synthesis is based on the reaction of a secondary phosphine borane with the 1,2-dibromo (or diiodo)­arene, owing to the formation in situ of an aryne species in the presence of <i>n</i>-butyllithium. When P-chirogenic secondary phosphine boranes were used, the corresponding <i>o</i>-halogeno-arylphosphine boranes were obtained without racemization in moderate to good yields and with ee up to 99%. The stereochemistry of the reaction, with complete retention of the configuration at the P atom, has been established by X-ray structures of P-chirogenic <i>o</i>-halogenophenyl phosphine borane complexes. The decomplexation of the borane was easily achieved without racemization using DABCO to obtain the free <i>o</i>-halogeno-arylphosphines in high yields
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