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Dalton Transactions
Page 4 of 6
COMMUNICATION
Journal Name
M. Gretton, B. Kamino, M. Brook and T. Bender,
S. Tian, J. Li, Z. Cai, B. Shi, W. Chen andDYO. IC: h10e.n10g3,9E/uDr0.DPTo0l1y5m55.E
J., 2018, 108, 373-379.
L. Ai, Y. Chen, L. He, Y. Luo, S. Li and C. Xu, Chem. Comm.,
2019, 55, 14019-14022.
J. Chojnowski, S. Rubinsztajn, W. Fortuniak and J. Kurjata,
Macromolecules, 2008, 41, 7352-7358.
6
7
8
9
functional group exchange process until complete consumption
of PhMe2SiH.
Macromolecules, 2012, 45, 723-728.
The disproportionation of Ge(II) precursors to Ge0 and Ge(IV)
is well known in the literature but usually requires a
temperature much higher than 100 °C. GeI2 disproportionation
at a temperature above 210 °C was previously used for the
deposition of crystalline Ge and for the synthesis of Ge NPs.27,
10 J. Kurjata, W. Fortuniak, S. Rubinsztajn and J. Chojnowski,
Eur. Polym. J., 2009, 45, 3372-3379.
11 D. Thompson and M. Brook, J. Am. Chem. Soc., 2008, 130,
32-33.
12 J. Li, Z. Zhang, T. Zhu, Z. Li, J. Wang and Y. Cheng, Eur. Polym.
J., 2020, 109562.
13 K. Matsumoto, S. Shimada and K. Sato, Chem. Eur. J., 2019,
25, 920-928.
39-41
Recently, the disproportionation of diphenylgermylene,
Ph2Ge, at 300 °C was proposed as the last step in the synthesis
of Ge NPs from Ph3GeX, where X = Cl, Br.28 The synthesis of
germanium nanowires by thermal decomposition of
germanium 2,6-dibutylphenoxide at 300 °C has also been
demonstrated.42
It should be mentioned that the standard Gibbs free energy
for the disproportionation of Ge(OBu)2 calculated for the gas
phase conditions is thermodynamically unfavourable. The
Ge(II)(OBu)2 disproportionation becomes thermodynamically
allowed when the standard Gibbs free energy of Ge0 transition
from the gas phase (Ge0(g)) to the solid phase (Ge0(s)), estimated
at -79.1 kcal/mol, 43 is taken into account (Equation 12, Table 2).
14 J. Grande, A. Fawcett, A. McLaughlin, F. Gonzaga, T. Bender
and M. Brook, Polymer, 2012, 53, 3135-3142.
15 J. Escorihuela, S. Pujari and H. Zuilhof, Langmuir, 2017, 33,
2185-2193.
16 R. Chadwick, J. Grande, M. Brook and A. Adronov,
Macromolecules, 2014, 47, 6527-6530.
17 J. Zhang, S. Liang, L. Yu, A. Skov, H. Etmimi, P. Mallon, A.
Adronov and M. Brook, J. Polym. Sci. Pol. Chem., 2016, 54,
2379-2385.
18 S. Rubinsztajn, J. Inorg. Organomet. Polym. Mater., 2014, 24,
1092-1095.
19 F. Drozdov, S. Milenin, V. Gorodov, N. Demchenko, M. Buzin
and A. Muzafarov, J. Organomet. Chem., 2019, 891, 72-77.
20 S. Rubinsztajn, M. Cypryk, J. Chojnowski, W. Fortuniak, U.
Mizerska and P. Pospiech, Organometallics, 2018, 37, 1585-
1590.
21 D. J. Parks, W. E. Piers and G. P. A. Yap, Organometallics,
1998, 17, 5492-5503.
22 S. Rubinsztajn, J. Chojnowski, M. Cypryk, U. Mizerska, W.
Fortuniak and I. I. Bak-Sypien, J. Catal., 2019, 379, 90-99.
23 D. A. Ruddy, J. C. Johnson, E. R. Smith and N. R. Neale, ACS
Nano, 2010, 4, 7459-7466.
24 N. H. Chou, K. D. Oyler, N. E. Motl and R. E. Schaak, Chem.
Mater., 2009, 21, 4105-4107.
25 E. Muthuswamy, A. Iskandar, M. Amador and S. Kauzlarich,
Chem. Mater., 2013, 25, 1416-1422.
26 M. Rodio, A. Scarpellini, A. Diaspro and R. Intartaglia, J.
Mater. Chem. C, 2017, 5, 12264-12271.
Conclusions
In summary, we found a new process involving Si-H bond
activation by electron deficient boranes such as B(C6F5)3. The
discovered reaction of Ge(OBu)4 with Si-H functional silanes in
the presence of B(C6F5)3 carried out at temperatures above 100
°C produces Ge0 in high yield, which spontaneously aggregates
to amorphous Ge NPs. This process provides a simple one-pot
method for Ge NPs synthesis from readily available substrates
under mild conditions. We continue to study this new process
to answer intriguing mechanistic questions about the formation
of Ge NPs, the nature of photoluminescence observed, and
ways to optimize the Ge NPs synthesis. The results obtained will
be published in the full paper under development.
27 D. Vaughn, J. Bondi and R. Schaak, Chem. Mater., 2010, 22,
6103-6108.
Conflicts of interest
28 B. Pescara, K. A. Mazzio, K. Lips and S. Raoux, Inorg. Chem.,
2019, 58, 4802-4811.
There are no conflicts to declare.
29 D. Wang, Y.-L. Chang, Q. Wang, J. Cao, D. B. Farmer, R. G.
Gordon and H. Dai, J. Am. Chem. Soc., 2004, 126, 11602-
11611.
Acknowledgments
30 J. Hu, Q. Lu, C. Wu, M. Liu, H. Li, Y. Zhang and S. Yao,
Langmuir, 2018, 34, 8932-8938.
31 F. Li, J. Wang, S. Sun, H. Wang, Z. Tang and G. Nie, Small,
2015, 11, 1954-1961.
32 N. Shirahata, D. Hirakawa, Y. Masuda and Y. Sakka,
Langmuir, 2013, 29, 7401-7410.
The authors are grateful to Wacker Chemie AG for financial
support and permission to publish their results. DFT
calculations were supported by the PL-Grid infrastructure. We
thank Dr. Torsten Gottschalk-Gaudig for valuable discussions.
33 D. Carolan, Prog. Mater. Sci., 2017, 90, 128-158.
34 M. Zacharias and P. Fauchet, Appl. Phys. Lett., 1997, 71, 380-
382.
35 M. Zacharias and P. Fauchet, J. Non-Cryst. Solids, 1998, 227,
1058-1062.
36 H. Wu, M. Ge, C. Yao, Y. Wang, Y. Zeng, L. Wang, G. Zhang
and J. Jiang, Nanotechnology, 2006, 17, 5339.
37 A. Guleria, S. Neogy, D. K. Maurya and S. Adhikari, J. Phys.
Chem. C, 2017, 121, 24302-24316.
38 X. Lu, J. T. Harris, J. n. E. Villarreal, A. M. Chockla and B. A.
Korgel, Chem. Mater., 2013, 25, 2172-2177.
Notes and references
1
M. Brook, J. Grande, F. Ganachaud and A. Muzafarov, Silicon
Polymers, 2011, 235, 161-183.
2
3
M. Brook, Chem. Eur. J., 2018, 24, 8458-8469.
R. Wakabayashi and K. Kuroda, ChemPlusChem, 2013, 78,
764-774.
4
5
S. Rubinsztajn and J. Cella, Macromolecules, 2005, 38, 1061-
1063.
J. Cella and S. Rubinsztajn, Macromolecules, 2008, 41, 6965-
6971.
4 | J. Name., 2012, 00, 1-3
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