metal-organic compounds
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The positions of all H atoms were obtained from the difference
Fourier map. Full-matrix least-squares re®nement on F2 was
employed with isotropic displacement parameters for H atoms. The
exception was the H atom bonded to C1 whose isotropic displace-
ment parameter was set to be equal to 1.2Ueq(C1). A Regina
weighting scheme (Wang & Robertson, 1985) using a normal equa-
tion of second order was applied for individual re¯ections so that w =
A(0,0) + A(1,0)V(F) + A(0,1)V(S) + A(2,0)V(F)2 + A(0,2)V(S)2 +
A(1,1)V(F)V(S), where V(F) = F2obs/F2obs(max), F2obs(max) = 12638,
V(S) = (sinꢄ/ꢈ)/[(sinꢄ/ꢈ)(max)] and (sinꢄ/ꢈ)(max) = 0.6497; the
parameters are A(0,0) = 3200.667, A(1,0) = 22.59881, A(0,1) =
2802.914, A(2,0) = 0.0017726, A(1,1) = 14.87134 and A(0,2) =
7847.764. The highest peak in the ®nal difference Fourier map is
Ï
Ï
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Ê
located between atoms Na and O32 [1.723 (3) A from Na and
Ê
1.255 (7) A from O32], and the deepest hole is between atoms Cu1
Ê
Ê
and O32 [1.2329 (8) A from Cu1 and 1.030 (8) A from O22].
Data collection: COLLECT (Nonius, 2000); cell re®nement:
DENZO±SMN (Otwinowski & Minor, 1997); data reduction:
DENZO±SMN; program(s) used to solve structure: SIR97 (Altomare
et al., 1999); program(s) used to re®ne structure: Xtal3.6 (Hall et al.,
1999); molecular graphics: ORTEP-3 (Farrugia, 1997); software used
to prepare material for publication: Xtal3.6 and PLATON (Spek,
2003).
È
È
Hokelek, T., Mert, Y. & Unaleroglu, C. (1998). Acta Cryst. C54, 310±313.
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The authors thank the Ministry of Higher Education,
Science and Technology of the Republic of Slovenia for
®nancial support through grants X-2000 and P1-0175-103.
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Supplementary data for this paper are available from the IUCr electronic
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described at the back of the journal.
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m104 Golobic et al. Na2[Cu3(CHO2)8]
Acta Cryst. (2006). C62, m102±m104