10.1002/ejoc.201800787
European Journal of Organic Chemistry
FULL PAPER
ESI-MS and CID experiments. Instead, we consistently identify
the elimination of intact 2-phenylpyridine as the energetically
favoured reaction pathway. Therefore, we concluded that the C-
H activation most likely proceeds in neutral complexes, and we
have continued our studies using the charge-tagging method.
For this purpose, we have synthesised imidazolium-based
charge-tagged 2-phenylpyridine for further analysis of
ruthenium(II)-β-diketonate-assisted C-H activation. We have
observed C-H activation in the [Ru(β-diketonate)(CTPhPy)Cl]+
complex as HCl elimination. Further, we have excluded the role
of carbonate in the C-H activation step by control experiments.
DFT analysis of the C-H activation reaction in neutral
[Ru(β-diketonate)(PhPy)Cl] suggested that the β-diketonate
ligand remains bidentally coordinated to ruthenium throughout
the reaction pathway. The most stable structure of [Ru(β-
diketonate)(PhPy)Cl] contains pre-activated 2-phenylpyridine
with a partly developed Ru-H bond. The C-H activation can
proceed directly via ruthenium-assisted H-transfer to the β-
diketonate or via the ruthenium(IV) intermediate. The
experimentally observed hydrogen transfer to the chlorine anion
results from the gas-phase-favoured fragmentation pathway.
thank to the Management Committee of the COST Action
CA15106 (C-H Activation in Organic Synthesis – CHAOS) for a
Short Term Scientific Mission grant. The authors also thank to
Dr. Carlos V. Melo for proofreading the manuscript. We further
thank Fernando Bonin Okasaki for preliminary experiments.
Keywords: Ruthenium • Mass spectrometry • C-H activation •
Collision-induced dissociation • Charge-tagging method
[1]
[2]
Q. Zhao, T. Poisson, X. Pannecoucke, T. Besset, Synthesis 2017, 49,
4808-4826.
L. Ping, D. S. Chung, J. Bouffard, S.-G. Lee, Chem. Soc. Rev. 2017, 46,
4299-4328.
[3]
[4]
P. Nareddy, F. Jordan, M. Szostak, ACS Catal. 2017, 7, 5721-5745.
S. Murai, F. Kakiuchi, S. Sekine, Y. Tanaka, A. Kamatani, M. Sonoda,
N. Chatani, Nature 1993, 366, 529-531.
[5]
[6]
[7]
P. B. Arockiam, C. Bruneau, P. H. Dixneuf, Chem. Rev. 2012, 112,
5879-5918.
S. Oi, S. Fukita, N. Hirata, N. Watanuki, S. Miyano, Y. Inoue, Org. Lett.
2001, 3, 2579-2581.
a) L. Ackermann, R. Vicente, A. Althammer, Org. Lett. 2008, 10, 2299-
2302; b) L. Ackermann, R. Vicente, H. K. Potukuchi, V. Pirovano, Org.
Lett. 2010, 12, 5032-5035.
[8]
[9]
I. Özdemir, S. Demir, B. Çetinkaya, C. Gourlaouen, F. Maseras, C.
Bruneau, P. H. Dixneuf, J. Am. Chem. Soc. 2008, 130, 1156-1157.
Also see: C. Shan, X. Luo, X. Qi, S. Liu, Y. Li, Y. Lan, Organometallics
2016, 35, 1440−1445.
Experimental Section
The synthesis of the ruthenium(II) catalyst has been previously
reported.13 ESI-MS spectra were acquired with
[10] A. Gray, A. Tsybizova, J. Roithová, Chem. Sci. 2015, 6, 5544-5553.
[11] D. Zell, S. Warratz, D. Gelman, S. J. Garden, L. Ackermann, Chem. Eur.
J. 2016, 22, 1248-1252.
a linear ion trap
instrument LTQ equipped with an electrospray ionisation source. The
ions of interest were generated from the acetonitrile solution of the
ruthenium(II) catalyst, 2-phenylpyridine or imidazolium-based charge-
tagged phenylpyridine, both with and without potassium carbonate. The
details for the preparation of the reaction mixtures are included in
Supporting information. The electrospray voltage was 4.5 kV, and the
capillary was heated to 300°C. The sheath gas, flow rate and voltages of
capillary and lenses were optimised to maximise the signal of the
required ions. Energy-resolved CID experiments were performed using a
Finnigan LCQ Deca mass spectrometer equipped with an electrospray
ionisation source. For mass-selected ions, the excitation period was 30
ms and the trapping parameter was qz= 0.25. The Schröder’s calibration
method was used to calibrate the collision energy and to determine the
appearance energies.17 The calibration was performed by correlating the
[12] L. V. Graux, M. Giorgi, G. Buono, H. Clavier, Dalton Trans. 2016, 45,
6491-6502.
[13] S. Seršen, J. Kljun, F. Poꢀgan, B. ꢁtefane, I. Turel, Organometallics
2013, 32, 609-616.
[14] S. Seršen, J. Kljun, K. Kryeziu, R. Panchuk, B. Alte, W. Körner, P.
Heffeter, W. Berger, I. Turel, J. Med. Chem. 2015, 58, 3984 – 3996.
[15] Ch. Gaiddon, M. Pfeffer, Eur. J. Inorg. Chem. 2017, 1639–1654.
[16] a) A. L. Noffke, A. Habtemariam, A. M. Pizarro, P. J. Sadler, Chem.
Commun. 2012, 48, 5219–5246. b) J. J. Soldevila-Barreda, I. Romero-
Canelo, A. Habtemariam, P. J. Sadler, Nat. Commun. 2015, 6, 6582; c)
M. Tomas-Gamasa, M. Martinez-Calvo, J. R. Couceiro, J. L.
Mascarenas, Nat. Commun. 2016, 7, 12538.
[17] E. L. Zins, C. Pepe, D. Schröder, J. Mass Spectrom. 2010, 45, 1253-
1260.
[18] J. E. Carpenter, C. P. McNary, A. Furin, A. F. Sweeney, P. B.
Armentrout, J. Am. Soc. Mass Spectrom. 2017, 28, 1876-1888.
[19] a) G. Yassaghi, L. Jašíková, J. Roithová, Int. J. Mass Spectrom. 2016,
407, 92-100; b) J. Schulz, E. Shcherbachenko, J. Roithová,
Organometallics 2015, 34, 3979-3987; c) A. ꢁkríba, J. Schulz, J.
Roithová, Organometallics, 2014, 33, 6868-6878; d) J. Schulz, L.
Jašíková, A. ꢁkríba, J. Roithová, J. Am. Chem. Soc., 2014, 136, 11513-
11523; e) J. Hꢂvl, J. Roithová, Org. Lett. 2014, 16, 200-203.
[20] A. D. Dwivedi, C. Binnani, D. Tyagi, K. S. Rawat, P.-Z. Li, Y. Zhao, S. M.
Mobin, B. Pathak, S. K. Singh, Inorg. Chem. 2016, 55, 6739-6749.
[21] a) F. Coelho, M. N. Eberlin, Angew. Chem. Int. Ed. 2011, 50, 5261-
5263; b) C. Iacobucci, S. Reale, J.-F. Gal, F. De Angelis, Angew. Chem.
Int. Ed. 2015, 54, 3065-3068.
experimental appearance energies of
a
set of substituted
benzylpyridiunium ions [RBnPy]+ with the values determined by
Carpenter et al (Figure S5 in the Supporting Information).18 The values of
the appearance energies are given with the experimental uncertainties of
different measurements.
The DFT calculations were performed using the M06L functional[24],the
SDD basis set for ruthenium and the 6-31+G* basis set for the remaining
atoms, as implemented in the Gaussian program package.[25] All complexes
were fully optimized, and the minima were assessed by frequency calculations
(none of the second derivatives were imaginary). The geometries of the
optimized complexes can be found in Supporting Information.
[22] A. D. Dwivedi, C. Binnani, D. Tyagi, K. S. Rawat, P.-Z. Li, Y. Zhao, S. M.
Mobin, B. Pathak, S. K. Singh, Inorg. Chem. 2016, 55, 6739-6749.
[23] For a recent theoretical study on this type of ruthenium complexes see:
Z. Sochorová Vokáčová, I. Turel, J. V. Burda, J. Mol. Model. 2018, 24,
98.
Acknowledgements
[24] Y. Zhao, D. G. Truhlar, J. Chem. Phys. 2006, 125, 194101: 1-18.
[25] Gaussian 09, Revision D.01, M. J. Frisch, G. W. Trucks, H. B. Schlegel,
G. E. Scuseria, M. A. Robb, J. R. Cheeseman, G. Scalmani, V. Barone,
G. A. Petersson, H. Nakatsuji, X. Li, M. Caricato, A. Marenich, J. Bloino,
This work was supported by the European Research Council
(ERC CoG IsoMS No. 682275) and by Charles University
Research Centre program No. UNCE/SCI/014. The authors
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