10.1002/asia.201900677
Chemistry - An Asian Journal
FULL PAPER
(S = 1) and m = 7 (S = 2) were considered. Again optimization of
complex 5b structure at m = 3 resulted in the almost square-
planar environment of the metal center, whereas in 3b it
remained in a tetrahedral form. Relative energies of various
forms are predicted to be also similar to the monomeric case: for
3b the state with m = 3 is more stable than the form with m = 7
by 12 kcal mole-1, whereas for 5b the high-spin state is more
energetically advantageous by 12 kcal mole-1. Thus, according
to computations for both monomeric and dimeric complexes,
fluoride ligand stabilizes forms with higher multiplicity and with
spin density being localized not only at the Ni ion but also at the
bian ligand. For all the other co-ligands, the forms with lower
multiplicity and spin density localized mostly on the Ni ions are
more energetically stable.
unpaired electron at bian1- and high-spin Ni2+ (SNi = 1) is realized.
The discovered features about structural and electronic diversity
of reduced nickel complexes may be useful tool for analysis and
planning the catalytic systems based on them.
Acknowledgements
The authors gratefully acknowledge the RFBR (grant № 19-03-
00084) for financial support and the CSF-SAC FRC KSC RAS
for providing necessary facilities to carry out this work.
For the most energetically stable high-spin form of dimeric
complex 5b with spin density localized both on Ni and bian
fragments the following broken-symmetry (BS) states were also
considered: (a) antiparallel spins at bians and parallel spins at Ni
ions, m = 5; (b) antiparallel spins at Ni ions and parallel spins at
bians, m=3; and (c) antiparallel spins both at Ni ions and bians,
m=1. All these cases are energetically very slightly less stable
compared to m=7 state, indicating very weak ferromagnetic
interactions of less than 2 cm-1.
Keywords: nickel • dpp-bian • reduction • electrochemistry •
cyclic voltammetry
1
2
3
4
W. Kaim, Inorg. Chem., 2011, 50, 9752-9765.
P. J. Chirik, Inorg. Chem., 2011, 50, 9737-9740.
H. Grützmacher, Angew. Chem. Int. Ed., 2008, 47, 1814-1818.
C. J. Rolle, K. I. Hardcastle, J. D. Soper, J. D., Inorg. Chem., 2008,
47, 1892-1894.
5
6
7
8
K. J. Blackmore, N. Lal, J. W. Ziller, A. F. Heyduk, J. Am. Chem.
Soc., 2008, 130, 2728-2729.
S. C. Bart, K. Schlopek, E. Bill, M. W. Boukamp, E. Lobkovsky, K.
Wieghardt, P. J. Chirik, J. Am. Chem. Soc., 2006, 128, 13901-13912.
On the example of complexes 3a and 3b the energies of
dimerization (ΔE = Edimer – Emonomer + 2EMeCN) in the gas phase
and in MeCN and THF solutions were estimated for the more
stable spin states with m = 2 for 3a and m = 3 for 3b.
Computations predicted the monomeric form to be more
advantageous both for THF and MeCN solutions: ΔE = 7.5
kcal mole-1 for MeCN and 6 kcal mole-1 for THF. For the gas
phase, the dimeric form was predicted to be slightly more stable:
ΔE = –0.6 kcal mole-1. Similar computations for the high-spin
forms of complexes 5a and 5b with m=4 and 7 in gas-phase
have shown that dimeric species are more stable by 9 kcal mole-
Q. Knijnenburg, S. Gambarotta, P. H. M. Budzelaar, Dalton Trans.,
2006, 46, 5442-5448.
G. D. Jones, J. L. Martin, C. McFarland, O. R. Allen, R. E. Hall, A. D.
Haley, R. J. Brandon, T. Konovalova, P. J. Desrochers, P. Peter, D.
A. Vicic, J. Am. Chem. Soc., 2006, 128, 13175-13183.
9
A. Klein, Yu. H. Budnikova, O. G. Sinyashin, J. Organomet. Chem.,
2007, 692, 3156-3166.
10 M. J. Sgro, D. W. Stephan, Dalton Trans., 2010, 39, 5786-5794.
11 H. Yang, Y. Zhao, B. Liu, J.-H. Su, I. L. Fedushkin, B. Wu, X.-J.
Yang, Dalton Trans., 2017, 46, 7857-7865.
1
12 W. Gao, L. Xin, Z. Hao, G. Li, J.-H. Su, L. Zhou, Y. Mu, Chem.
Comm., 2015, 51, 7004-7007.
.
13 L. K. Johnson, C. M. Killian, M. Brookhart, J. Am. Chem. Soc., 1995,
117, 6414-6415.
CONCLUSIONS
14 W. C. Anderson, J. L. Rhinehart, A. G. Tennyson, B. K. Long, J. Am.
Chem. Soc., 2016, 138, 774-777.
15 C. M. Killian, L. K. Johnson, M. Brookhart, Organometallics, 1997,
16, 2005-2007.
In summary, we have successfully prepared a series of the new
one-electron reduced nickel complexes 1-5 with dpp-bian and
BF4– or various halide ligands by two different pathways, namely
by chemical and electrochemical procedures. It was found that
varying the conditions makes possible to control the reversible
solvent-induced transitions between the monomeric and dimeric
complexes. Both EPR experiments and magnetic data showed
that electron localization at the nickel center occurs in the case
16 S. A. Svejda, M. Brookhart, Organometallics, 1999, 18, 65-74.
17 C. S. B. Gomes, P. T. Gomes, M. T. Duarte, J. Organomerallic
Chemistry, 2014, 760, 101-107.
18 M. D. Leatherman, M. Brookhart, Macromolecules, 2001, 34, 2748-2750.
19 R. J. Maldanis, J. S. Wood, A. Chandrasekaran, M. D. Rausch, J. C. W.
Chien, J. Organomet. Chem., 2002, 645, 158-167.
20 M. D. Leatherman, S. A. Svejda, L. K. Johnson, M. Brookhart, J. Am.
Chem. Soc., 2003, 125, 3068-3081.
–
of the complexes 1-4 with a BF4 anion and the iodide, chloride
and bromide co-ligands and leads to the NiI complexes with
neutral bian. In the case of the fluoride co-ligand, anion-radical
complex 5 with an unpaired electron on the ligand was found.
The observed trends were reproduced by computations: for
complexes 2a-4a and 2b-4b computations predicted spin
density mostly localized on the metal center, however, slightly
shifted to bian. In the case of 5a and 5b, the form with one
21 Z. Chen, M. Brookhart, Acc. Chem. Res., 2018, 51, 1831-1839.
22 S. D. Ittel, L. K. Johnson, M. Brookhart, Chem. Rev., 2000, 100
,
1169-1204.
23 I. E. Sochnikov, N. V. Semikolenova, K. P. Bryliakov, A. A. Antonov,
V. A. Zakharov, E. P. Talsi, Dalton Trans., 2018, 47, 4968-4974.
24 I. E. Sochnikov, N. V. Semikolenova, K. P. Bryliakov, A. A. Antonov,
W.-H. Sun, E. P. Talsi, J. Organomet. Chem., 2019, 880, 267-271.
For internal use, please do not delete. Submitted_Manuscript
This article is protected by copyright. All rights reserved.