[Ni(BuOpdt)2tptz] (5·tptz). Tptz (15.6 mg; 0.050 mmol) and
5 (26.8 mg; 0.050 mmol) were heated in 30 mL of BuOH in
an Ace pressure tube until complete dissolution. The product
was obtained as deep green crystals by slow evaporation of the
solution at room temperature. Mp 86 ◦C. Elemental analysis found
(calc. for C40H44O4P2S4N6Ni): C, 52.36 (52.13); H, 5.01 (4.81); N,
8.94 (9.12); S, 13.64 (13.91). Yield: 26.0 mg, 0.0282 mmol, 56%.
FT-IR (1700–350 cm-1): 1594 vs, 1575 vs, 1558 vs, 1536 vs, 1497 s,
1465 ms, 1450 ms, 1403 m, 1392 ms, 1375 vs, 1300 m, 1290 ms,
1255 ms, 1177 ms, 1110 s, 1059 ms, 1021 s, 1012 s, 999 ms, 970 s,
830 m, 800 ms, 770 vs, 683 m, 670 s, 649 ms, 637 s, 623 s, 565 m,
552 ms cm-1. FT-Raman (1700–50 cm-1; relative intensities in
parentheses related to the highest peak taken equal to 10.0): 1583
(8.9), 1484 (10.0), 1438 (4.0), 1402 (7.0), 1373 (3.4), 1255 (1.5),
1182 (1.5), 1110 (2.6), 1046 (5.1), 1029 (9.4), 1010 (4.0), 993 (2.8),
802 (1.3), 635 (1.3), 83 (8.5) cm-1.
X-Ray diffraction
X-Ray structure determinations and crystallographic data were
collected at 293(2) K for compound 2·tptz, and at 120(2) K for
compounds 4·tptz, 3·tptz, 5·tptz, 6·tptz, 7, and 8, by means of
combined phi and omega scans on a Bruker-Nonius KappaCCD
area detector, situated at the window of a rotating anode (graphite
Mo-Ka radiation for 4·tptz, 3·tptz, 6·tptz, and 10 cm confocal
˚
mirrors for 5·tptz, 7, and 8, respectively, l = 0.71073 A). The
structures were solved by direct methods, SHELXS-97 and refined
on F2 using SHELXL-97.22 Anisotropic displacement parameters
were assigned to all non-hydrogen atoms. Hydrogen atoms were
included in the refinement, but thermal parameters and geometry
were constrained to ride on the atom to which they are bonded.
The data were corrected for absorption effects using SORTAV23
for 2·tptz, 4·tptz, and using SADABS V2.1024 for 3·tptz, 5·tptz,
6·tptz, 7, and 8. The disorder in compounds 2·tptz, 5·tptz, and 8
was modeled by splitting the respective residues of the molecules
into two parts allowing the populations of the two sites to refine
freely. In structure 5·tptz the geometries of the disordered parts
of the molecule had to be restrained to be the same for the two
positions and rigid-body constraints were also applied.
[Ni((EtO)2PS2)2tptz] (6·tptz). Tptz (0.15 g; 0.48 mmol) and
6 (0.21 g; 0.49 mmol) were heated in 30 mL of EtOH in
an Ace pressure tube until complete dissolution in 50 mL of
EtOH. The product was obtained as deep green crystals by slow
evaporation of the solution at room temperature. Yield 0.236 g,
0.32 mmol, 67%. Mp 198 ◦C. Elemental analysis found (calc.
for C26H32N6NiO4P2S4): C, 42.00 (42.12); H, 4.39 (4.35); N, 11.21
(11.33) S, 16.87 (17.30). FT-IR (1700–50 cm-1): 1608 m, 1577 s,
1559 s, 1537 vs, 1486 m, 1473 m, 1443 m, 1395 ms, 1377 vs,
1258 mw, 1156 mw, 1098 m, 1042 s, 1011 vs, 947 s, 930 s, 774 vs,
684 ms, 658 vs, 635 ms, 551 m, 472 mw, 419 mw, 376 m cm-1. FT-
Raman (1700–50 cm-1; relative intensities in parentheses related to
the highest peak taken equal to 10.0): 1608 (4.6), 1586 (6.9), 1575
(8.4), 1484 (10.0), 1442 (3.5), 1402 (5.7), 1377 (3.0), 1260 (1.2),
1185 (1.3), 1046 (4.5), 1030 (8.4), 1010 (5.9), 994 (2.1), 815 (1.0),
780 (1.4), 706 (0.9), 664 (1.1), 634 (2.4), 553 (2.1), 492 (1.0), 374
(0.7), 334 (0.8) cm-1.
Theoretical calculations
Quantum-chemical DFT calculations were carried out on com-
pounds 2·tptz and 6·tptz with the mPW1PW25 hybrid functional
and Schafer, Horn, and Ahlrichs double-zeta plus polarization all-
electron BSs26 using the commercially available suite of programs
Gaussian03.27 NBO populations28 and Wiberg bond indexes29
were calculated at the geometries obtained from structural data.30
The programs Gabedit 2.0.731 and Molden 4.632 were used to
investigate the charge distributions and molecular orbital shapes.
Acknowledgements
CINECA (Consorzio Interuniversitario per il Calcolo Automatico
dell’Italia Nord Orientale) is gratefully acknowledged.
[Ni(EtOpdt)(tptz)(H2O)]NO3 (7).
A CH3CN solution of
AgNO3 (5.0 mL; 7.0 mg; 0.04 mmol) was layered on a CH2Cl2
solution of 2·tptz (5.0 mL; 34.6 mg; 0.04 mmol) in a dark tube, and
stored in the darkness. After five weeks few deep ruby crystals have
been isolated from a light brown solution. Due to the paucity of
the product, only X-ray crystal structure and FT-IR analyses have
been performed. FT-IR (4000–400 cm-1): 3447 ms(br), 2982 m,
1653 w, 1589 ms, 1559 m, 1541 mw, 1497 ms, 1458 m, 1437 mw,
1386 mw, 1291 ms, 1254 s, 1181 ms, 1107 vs, 1016 s, 947 ms, 833 m,
800 mw, 773 mw, 658 ms, 633 ms, 621 s, 547 s, 517 m, 421 mw cm-1.
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[Ni(tptz)(l-SO4)(H2O)]2·6H2O (8). A MeOH solution of
CuSO4·5H2O (5.0 mL; 5.0 mg; 0.02 mmol) was added to a CH2Cl2
solution of 2·tptz (5.0 mL; 18.0 mg; 0.02 mmol) in a dark tube.
The resulting yellow opaque solution was filtered and diethyl ether
diffused on it. After three months few small green cubic crystals
have been isolated. Due to the paucity of the product, only X-ray
crystal structure and FT-IR analyses have been performed. FT-IR
(4000–400 cm-1): 3404 s(br), 1637 w, 1611 w, 1576 s, 1560 vs,
1542 vs, 1490 ms, 1477 ms, 1395 s, 1381 s, 1261 m, 1112 vs, 1048 s,
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374 ms cm-1.
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This journal is
The Royal Society of Chemistry 2009
Dalton Trans., 2009, 2510–2520 | 2519
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