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Journal Name ! ChemComm 2?%&*-;(@$.-;'+(A-%B0 !Page 4 of 8 !"#$%&'()&*+ ,-.+(./-01(2341(5675689:;6<<66666< ===7$0;7"$>:<<<<<< !"#$%&'(#)*' Self-Assembly in the Electrical Double Layer of Ionic Liquids Susan Perkin,*a Lorna Crowhurst,b Heiko Niedermeyer, b Tom Welton, b Alexander M. Smith a and Nitya Nand Gosvamia Received (in XXX, XXX) Xth XXXXXXXXX 20XX, Accepted Xth XXXXXXXXX 20XX 5 DOI: 10.1039/b000000x We have studied the structure of two ionic liquids confined layering structure is observed for the two ILs, despite their between negatively charged mica sheets. Both liquids exhibit 50 similar chemical structures, which differ only in the length of interfacial layering, however the repeat distance is hydrocarbon chain on the cation. We propose that the more dramatically different for the two liquids. Our results suggest amphiphilic nature of the [C6C1im] cation causes self-assembly 10 a transition from alternating cation-anion monolayers to tail- into tail-to-tail cation bilayers at the mica surface, driven by the to-tail cation bilayers when the length of the cation need to sequester the hydrocarbon chains away from the ionic hydrocarbon chain is increased. 55 regions. Many applications of ionic liquids (ILs) involve their use as electrolytes in electrochemical applications such as solar cells and 15 electrical double-layer capacitors (EDLCs, also called supercapacitors)1, 2. Currently there is relatively little understanding of the interfacial behaviour of ILs at charged surfaces, although recent experimental and theoretical work have revealed that the electrical double layer in IL is dramatically 20 different to that in dilute electrolyte solutions. Experiments using Figure 1: Chemical structures and approximate dimensions in nm, a Surface Force Apparatus (SFA)3, 4 and AFM5 suggest that next calculated from the van der Waals radii, of the ions used in this study. to a negative surface lies a monolayer of cations, (C), followed by The force, F , between two atomically smooth mica sheets (in alternating monolayers of anions (A) and cations (C) repeating for N crossed cylinder configuration with radius R) was measured as a 3-8 repeat units (i.e. C(AC)n where n = 3-8) away from the 60 function of their separation distance, D, across the IL using an 25 surface. This alternating cation-anion layer structure was also SFA according to procedures described previously11. By the observed at a single sapphire surface probed by x-ray Derjaguin approximation F /R is proportional to the interaction reflectometry6. Molecular dynamics (MD) simulations of IL in N energy per unit area between parallel plates, E . Ionic liquids the region near an electrode surface reveal oscillations in cation ll were synthesised according to a method described elsewhere12 and anion density with distance from the surface7. 65 and kept in a desiccator until used. P2O5 powder inside the SFA 30 The space-filling nature of the ions near the electrode also chamber prevented moisture entering the IL during the leads to a qualitatively different dependence of double layer experiment, as verified by the reproducibility of results over the capacitance on electrode potential: a local maximum (or ‘camel first 5-10 hours of each experiment. When water vapour was shape’ with two maxima for non-spherical ions) at the potential intentionally allowed to enter the SFA chamber the oscillatory of zero charge (PZT) is predicted and observed for an ionic 8 70 forces were observed to decrease in magnitude over a similar 35 liquid , in contrast to the minimum expected for dilute timescale and finally to disappear entirely. The data presented electrolytes9. For applications in EDLCs, where the electrode is represents many force runs at different contact points on the mica composed of micro- or nano-porous materials in order to sheets and from three separate experiments (different mica maximise the surface area2, the effect on capacitance of confining sheets) for each IL. the electrolyte to nanoscopic geometries is important. For 75 Measurements of FN as a function of film thickness, D, for 40 example it has been shown that optimal capacitance can be [C C im][NTf ] and [C C im][NTf ] are shown in Figure 2. Both achieved when the pore size is less than 1nm within which only a 4 1 2 6 1 2 ILs show clear oscillatory forces with alternating repulsive and single ion can be trapped between the electrode surfaces10. attractive regions of increasing amplitude with decreasing D. Here we present high resolution force measurements which Each minimum corresponds to a stable configuration of ions reveal the interfacial structure of two ILs, 1-butyl-3- 80 between the surfaces, and the maxima represent the force 45 methylimidazolium bis(trifluoromethylsulfonyl)imide, required to squeeze out ions from between the surfaces to reach [C C im][NTf ], and 1-hexyl-3-methylimidazolium 4 1 2 the next stable configuration. However the period of the bis(trifluoromethylsulfonyl)imide, [C C im][NTf ] (Figure 1), 6 1 2 oscillations is significantly different for the two ILs which cannot confined to nanometrically thin films. A dramatically different This journal is © The Royal Society of Chemistry [year] [journal], [year], [vol], 00–00 | 1 Page 5 of 8 ChemComm Figure 2: Measured force, FN, between two mica surfaces (normalised by R) as a function of film thickness, D, for (a) [C4C1im][ [NTf2] and for (b) [C6C1im][NTf2]. Forces were measured from D ~ 200 nm but only the region between 0 – 15 nm where non-zero forces were observed is shown. Open diamonds indicate points measured on approach of the surfaces (decreasing D) while open circles indicate data measured on retraction of the surfaces. Filled triangles indicate points measured from the jump-apart of the surfaces from an adhesive minimum. The lines are a guide to the eye to show the 5 oscillatory nature of the forces, with solid lines through measured regions and dashed lines through the regions inaccessible to measurement due to the jump-in from the previous energy barrier. The inset tables show, for each graph, the average values of D for each force wall and its standard deviation as well as the inter-wall separations, !D. The columns of the tables are labelled according to our interpretation of the ion structure in the film at that separation: for [C4C1im] the n-value refers to the structure C(AC)n, and for [C6C1im] the n-value refers to (ACCA)n. be accounted for by simply considering the incrementally longer 35 decreasing magnitude of the energy barriers and the small 10 chain length for [C6C1im] compared to [C4C1im]. Instead, this increase in the !D values as D increases suggest that the layering must represent entirely different interfacial structuring for the two structure softens – becomes more disordered in ion arrangement – ILs and we rationalise this striking result as follows. further away from the surfaces. [C4C1im][NTf2]. Figure 2a shows the oscillatory forces [C6C1im][NTf2]. Figure 2b shows the equivalent measurement observed for [C4C1im][NTf2] confined between mica sheets, 40 for [C6C1im][NTf2], showing four oscillations within our force 15 revealing six energy minima within the resolution of our resolution separated by significantly larger distances than for measurement. The period of the oscillations (!D in the inset to [C4C1im][NTf2]. Comparing the inter-wall separations, !D, with Figure 2) is ~0.9 – 1.4 nm, with the lower values for the most the ion sizes (Figure 1) it is clear that these oscillatory forces highly confined films, consistent with the thickness expected for cannot be explained by the squeeze out of one anion–cation one anion monolayer and one cation monolayer, (AC), as long as 45 repeat unit. Nonetheless, the clear oscillations in force indicate 20 the [C4C1im] cations are lying with the hydrocarbon chain that there must be an ordered and repeating structure in the IL parallel rather than normal to the surfaces. Thus we propose, in between the mica surfaces; albeit one with greater repeat line with earlier measurements by us and others3, 4, that distance. In order to explain this observation we look at the [C4C1im][NTf2] is arranged in alternating monolayers of anions chemistry of the cation, [C6C1im], which is distinctly amphiphilic and cations. This effect is likely to be templated by the negative 50 with the positive charge at one end of the ion and a non-polar 4 25 charge of the mica surface , which induces a monolayer of chain to the other end. We propose that a feasible repeating cations (C) to form in the first layer (which is responsible for the structure for this IL consists of bilayers of [C6C1im] ions, formed closest repulsive wall observed at 0.3 nm), followed by a due to aggregation of the non-polar chains, with neutralising counterion layer of anions, and so on. Each oscillation in the layers of anions adjacent to the cationic headgroups, i.e. force profile corresponds to squeeze-out of one cation–anion 55 (ACCA)n. This self-assembly could be driven by the unfavourable 30 repeat unit, (AC), to preserve electroneutrality of the film. Thus interface between hydrocarbon and charged groups relative to only odd numbers of layers are possible – C(AC)n – since the first more favourable ion-ion interactions, similar to the formation of single cation monolayer is responsible for neutralisating the mica bilayers of amphiphiles in aqueous solution. The observed energy charge. This alternation of cation and anion monolayers is shown minima are separated by the large repeat distance between the schematically in Figure 3a for the C(AC)2 film (D = 2.3 nm). The 60 bilayer units, (ACCA), as follows: (a) the wall at D = 0.8 nm This journal is © The Royal Society of Chemistry [year] [journal], [year], [vol], 00–00 | 2 ChemComm Page 6 of 8 Figure 3: Suggested ion orientations in (a) [C4C1im][NTf2] at a film thickness of 2.3 nm showing alternating cation and anion monolayers for C(AC)2; (b) [C6C1im][NTf2] at 3.4 nm showing a single bilayer, (ACCA)1, and (c) [C6C1im][NTf2] at a film thickness of 8.3 nm showing two bilayers, (ACCA)2.
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