Electroactive Organic Molecules Immobilized onto Solid Nanoparticles as a Cathode Material for Lithium-Ion Batteries
Electroactive Organic Molecules Immobilized onto Solid Nanoparticles as a Cathode Material for Lithium-Ion Batteries
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DOI:
10.1002/anie.201001539
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发表时间:
2010-01-01
影响因子:
16.6
通讯作者:
Gaberscek, Miran
中科院分区:
文献类型:
--
作者:
Genorio, Bostjan;Pirnat, Klemen;Gaberscek, Miran
Li-ion batteries are considered very promising energy-storage devices for a variety of applications including large-scale batteries.[1] Given the large quantities of energy to be stored in such applications, the amount of cathode materials will be in the order kilograms per battery unit. This will not only raise concerns about the finite quantity of some resources on the earth and its environmental intolerance but also about overall CO2 management.[2] To overcome such problems efficiently, Armand, Chen, and co-workers [2–4] recently suggested a new class of sustainable lithium batteries based on organic compounds. The other available literature mainly reports on the use of polymers as possible electroactive materials in Liion batteries [5, 6] or totally organic polymer based rechargeable batteries.[7] Indeed, certain redox active centers of organic molecules (and also polymers) offer almost unlimited combinations of atomic arrangements and many possibilities for substitutions; this allows for fine tuning of the desired properties. Herein, our primary focus is the use of “monomer” organic molecules as an active material for Li-ion batteries. The reversible capacity of certain organic compounds, such as LixC6O6, can reach values as high as 580 mA hg À1,[3] but their operating voltage is typically quite low (about 2 V vs. Li). However, the most critical problem associated with utilization of organic materials in batteries is the high solubility of many interesting organic molecules in the aprotic electrolytes commonly used in the Li-ion batteries. Although soluble molecules can act as a charge carrier,[8] the operation of a battery using such molecules is diffusionlimited. Besides that, the use of soluble organic molecules in a long-term cycling process may be questionable. Herein we propose, for the first time, that this problem can be overcome by grafting (anchoring) of soluble electroactive organic molecules onto the surface of an appropriate insoluble substrate. The essence of this approach is the strong attachment of organic molecules to a suitable substrate. This attachment not only makes the organic molecule stable during the electrochemical operation but also allows tuning of its electrochemical properties (eg its redox potential). Unlike in batteries, such an approach is commonly used in the related fields of sensors [9, 10] and supercapacitors.[11] We demonstrate this concept by grafting a quinone derivative of calix [4] arene (CQ) onto the surface of two different substrates: 1) nanosized silica particles with a specific surface area close to 200 m2 gÀ1 and 2) carbon black. The electronic wiring between the grafted CQ and the current collector is established by further addition of carbon black. Scheme 1 shows the hypothetical mechanism of grafting of one CQ on silica nanoparticle and the proposed electrochemical reaction. The proposed binding nature of CQ onto silica is supposed to result in excellent electrochemical stability of such organic–inorganic hybrid system. The choice of CQ was based on proven redox activity of quinone [8] and on its known conformational mobility.[12] That is, although CQ is a relatively large molecule with a molecular weight of 568.5 gmolÀ1, it can accommodate itself on a substrate surface, thus acquiring an optimal geometry. CQ has two quinone units, each having two redox active sites. If the proposed four-electron reaction mechanism [13] can be fully realized, a theoretical capacity of 189 mAhgÀ1 is expected. By grafting CQ to an insoluble substrate, we inevitably lose part of this capacity. A simple estimation shows that if a monolayer of CQ on a 200 m2 gÀ1 specific surface area is formed, a total capacity of 39 mA hg À1 (normalized per 1 g …