R. Tacke et al.
ARTICLE
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dried in vacuo (0.01 mbar, 20 °C, 3 h) to give 9 in 73% yield (50.8 g,
249 mmol) as a yellow crystalline solid. 1H NMR (500.1 MHz,
4
CD2Cl2): δ = 1.78 [d, J(1H,1H) = 0.5 Hz, 3 H, CCH3], 2.04–2.06 (m,
3
3 H, CCH3), 2.82 [d, J(1H,1H) = 5.0 Hz, 3 H, NCH3], 4.05 [br. s, 1
H, N(CH3)H], 5.22–5.24 (m, 1 H, CCHC), 6.62–6.70, 6.93–6.99, and
7.12–7.21 (m, 4 H, C6H4), 11.8 ppm (br. s, 1 H, HNCCH3). 13C NMR
(125.8 MHz, CD2Cl2): δ = 19.3 (CCH3), 29.2 (CCH3), 30.5 (NCH3),
97.2 (CCHC), 110.6, 116.5, 124.4, 128.0, 128.6, and 145.9 (C6H4),
163.2 (NCCH3), 196.4 ppm (CO). 15N VACP/MAS NMR (data for
two crystallographically independent molecules): δ = –257.7/–252.1
(NCCH3), –323.9 ppm (2 N, NCH3). C12H16N2O: calcd. C 70.56; H,
7.89; N, 13.71%; found: C 70.5; H, 7.8; N, 13.7%.
Crystal Structure Analyses: Suitable single crystals of 5a,
5b·CH3CN, 5c·CH3CN, and 6a–c were mounted in inert oil (perfluo-
ropolyalkyl ether, ABCR) on a glass fiber and then transferred to the
cold nitrogen gas stream of the diffractometer [Stoe IPDS (5a,
5c·CH3CN, and 6a–c; graphite-monochromated Mo-Kα radiation, λ =
0.71073 Å) or Bruker Nonius KAPPA APEX II (5b·CH3CN; Montel
mirror, Mo-Kα radiation, λ = 0.71073 Å)]. All structures were solved
by direct methods (SHELXS-97[16]) and refined by full-matrix least-
squares methods on F2 for all unique reflections (SHELXL-97[16]).
SHELXLE was used as refinement GUI.[17] For the CH hydrogen
atoms, a riding model was employed.
Crystallographic data (excluding structure factors) for the structures in
this paper have been deposited with the Cambridge Crystallographic
Data Centre, CCDC, 12 Union Road, Cambridge CB21EZ, UK.
Copies of the data can be obtained free of charge on quoting the de-
pository numbers CCDC-966387 (5a), CCDC-966388 (5b·CH3CN),
CCDC-966389 (5c·CH3CN), CCDC-966390 (6a), CCDC-966391 (6b),
and CCDC-966392 (6c) (Fax: +44-1223-336-033; E-Mail:
deposit@ccdc.cam.ac.uk, http://www.ccdc.cam.ac.uk).
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Z. Anorg. Allg. Chem. 2014, 300–309