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1
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84918188303
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B. Giese, W. Damm, M. Roth, M. Zehnder, Synlett 1992, 441. See also: Y. Yamamoto, S. Nishii, T. Ibuka, J. Am. Chem. Soc. 1988, 110, 617.
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(1992)
Synlett
, pp. 441
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Giese, B.1
Damm, W.2
Roth, M.3
Zehnder, M.4
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2
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0001611849
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B. Giese, W. Damm, M. Roth, M. Zehnder, Synlett 1992, 441. See also: Y. Yamamoto, S. Nishii, T. Ibuka, J. Am. Chem. Soc. 1988, 110, 617.
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(1988)
J. Am. Chem. Soc.
, vol.110
, pp. 617
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Yamamoto, Y.1
Nishii, S.2
Ibuka, T.3
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4
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85031234521
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note
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The alkenes were synthesized by Knoevenagel condensation of malonodinitrile with suitably substituted aldehydes.
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-
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5
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0008766842
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The formation of radicals by the sonication method is described in: C. Petrier, C. Dupuy, J. L. Luche, Tetrahedron Lett. 1986, 27, 3149; P. Erdmann, J. Schäfer, R. Springer, H.-G. Zeitz, B. Giese, Helv. Chim. Acta 1992, 75, 638.
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(1986)
Tetrahedron Lett.
, vol.27
, pp. 3149
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Petrier, C.1
Dupuy, C.2
Luche, J.L.3
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6
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84987590661
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The formation of radicals by the sonication method is described in: C. Petrier, C. Dupuy, J. L. Luche, Tetrahedron Lett. 1986, 27, 3149; P. Erdmann, J. Schäfer, R. Springer, H.-G. Zeitz, B. Giese, Helv. Chim. Acta 1992, 75, 638.
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(1992)
Helv. Chim. Acta
, vol.75
, pp. 638
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Erdmann, P.1
Schäfer, J.2
Springer, R.3
Zeitz, H.-G.4
Giese, B.5
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7
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84947886797
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The X-ray structures will be published
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The X-ray structures will be published in Acta Cryst.C.
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Acta Cryst.C
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8
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85031223028
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note
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1) exhibit significant trends in the NMR spectra: Hα (δ: 3.75-4.00), Cα (δ:11.3-14.0), and Cβ (δ:40.9-55.3) appear at lower field in the anti isomer 7 (Cα is the C-atom which is substituted by the two nitrile groups). In addition, the coupling JHβHγ (0.5-1.6 Hz) is slightly smaller in compound 6 than in compound 7.
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9
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0342490073
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The AM1 calculations of 4A and 4B were carried out using the MOPAC6 program QCPE 455. AM1 calculations: M. J. S. Dewar, E. G. Zoebisch, E. F. Healy, J. J. Stewart, J. Am. Chem. Soc. 1985, 121, 2063.
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(1985)
J. Am. Chem. Soc.
, vol.121
, pp. 2063
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Dewar, M.J.S.1
Zoebisch, E.G.2
Healy, E.F.3
Stewart, J.J.4
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10
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85031210920
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The calculations were carried out with Gaussian 92/DFT, Revision F.2, Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Gill, P. M. W.; Johnson, B. G.; Wong, M. W.; Foresman, J. B.; Robb, M. A.; Head-Gordon, M.; Replogle, E. S.; Gomperts, R.; Andres, J. L.; Raghavachari, K.; Binkley, J. S.; Gonzalez, C.; Martin, R. L.; Fox, D. J.; Defrees, D. J.; Baker, J.; Stewart, J. J. P.; Pople, J. A. Gaussian, Inc., Pittsburgh PA, 1993. The transition state structures 8 and 9 were calculated at the MP2/6-31G*//UHF/3-21G level of theory
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The calculations were carried out with Gaussian 92/DFT, Revision F.2, Frisch, M. J.; Trucks, G. W.; Schlegel, H. B.; Gill, P. M. W.; Johnson, B. G.; Wong, M. W.; Foresman, J. B.; Robb, M. A.; Head-Gordon, M.; Replogle, E. S.; Gomperts, R.; Andres, J. L.; Raghavachari, K.; Binkley, J. S.; Gonzalez, C.; Martin, R. L.; Fox, D. J.; Defrees, D. J.; Baker, J.; Stewart, J. J. P.; Pople, J. A. Gaussian, Inc., Pittsburgh PA, 1993. The transition state structures 8 and 9 were calculated at the MP2/6-31G*//UHF/3-21G level of theory.
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