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Table 3 NBO charges for the b-atoms of 3a–3m at B3LYP/
6-31?G* level
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Compound
Natural charge
at b-atoms
Yield/%
C-10 and C-100
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3a
3b
3c
3d
3e
3f
-0.1483
-0.1526
-0.1461
-0.1404
-0.1455
-0.1629
-0.1564
-0.1473
-0.1433
-0.1435
-0.1531
-0.1496
-0.1788
98
89
92
98
98
80
90
93
96
98
95
95
Trace
3g
3h
3i
3j
3k
3l
3m
15. Rostamizadeh S, Amani AM, Mahdavinia GH, Sepehrian H,
Ebrahimia S (2009) Synthesis 1356
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55.7, 113.0, 115.3, 115.5, 120.3, 120.4, 127.4, 129.4, 129.5,
130.9, 131.0, 132.3, 132.4, 139.1, 139.6, 139.7, 159.5, 159.6,
159.7, 162.8 ppm; MS (EI): m/z (%) = 42 (16), 65 (63), 91
(100), 131 (40), 174 (44), 198 (19), 222 (23), 250 (63), 382
(86), 410 (54), 473 (30), 501 (75), 567 (16).
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Computational methods
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B, Pomelly C, Adamo C, Clifford S, Ochterski J, Petersson GA,
Ayala PY, Cui Q, Morokuma K, Malick DK, Rabuck AD, Ragh-
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StefanovBB, LiuG,LiashenkoA, PiskorzP, KomaromiI, Gomperts
R, Martin RL, Fox DJ, Keith T, Al-Laham MA, Peng CY, Nana-
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Full geometry optimizations of 3a–3m were accomplished
without any symmetry constraints by means of hybrid
functional B3LYP [19–21]. The applied basis set is com-
prised of Pople’s well-known 6-31?G* basis set, using
Gaussian 98 code [22–24] and an extra plus because of the
importance of diffuse functions [25, 26]. The reliability of
the optimized structures was confirmed through the
development of the basis set B3LYP/6-31?G* [27, 28]. To
obtain natural charge data of atoms NBO calculations were
performed at the B3LYP/6-31?G* level [29].
Acknowledgments The authors gratefully acknowledge the Research
Council of K. N. Toosi University of Technology for financial support of
this work.
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27. Moller C, Plesset MS (1934) Phys Rev 46:618
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96:6796
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