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w = 1:1) to give white crystals (yield 47%).
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w = 1:1) to give white crystals (yield 47%).
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Crystal data: X-ray single-crystal diffraction data for the compound were collected on a Bruker Smart 1000 CCD area-detector diffractometer at 294(2) K with Mo Ko. radiation (λ, 0.71073 A) in the ω-Φ scan mode in the range of 1.07 < θ < 26.33°. The SAINT program (Bruker AXS, SAINT Software Reference Manual; Bruker: Madison, WI, 2000) was used for integration of the diffraction profiles. All the structures were solved by direct methods using the SHELXS program of the SHELXTL package and refined by full-matrix least-squares methods with SHELXL semiempirical absorption corrections were applied using the SADABS program, Sheldrick, G. M. SHELXTL NT Program for Solution and Refinement of Crystal Structures, version 5.1: University of Göttingen: Göttingen, Germany, 1997, The maximum and minimum transmission factors were 0.990 and 0.962, respectively. In all cases, non-hydrogen atoms are refined anisotropically. Whenever possible, th
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Crystal data: X-ray single-crystal diffraction data for the compound were collected on a Bruker Smart 1000 CCD area-detector diffractometer at 294(2) K with Mo Ko. radiation (λ = 0.71073 A) in the ω-Φ scan mode in the range of 1.07 < θ < 26.33°. The SAINT program (Bruker AXS, SAINT Software Reference Manual; Bruker: Madison, WI, 2000) was used for integration of the diffraction profiles. All the structures were solved by direct methods using the SHELXS program of the SHELXTL package and refined by full-matrix least-squares methods with SHELXL (semiempirical absorption corrections were applied using the SADABS program) (Sheldrick, G. M. SHELXTL NT Program for Solution and Refinement of Crystal Structures, version 5.1: University of Göttingen: Göttingen, Germany, 1997). The maximum and minimum transmission factors were 0.990 and 0.962, respectively. In all cases, non-hydrogen atoms are refined anisotropically. Whenever possible, the hydrogen atoms were located on a difference Fourier map.
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