Alice
Pyne‡
ab,
Marc-Philipp
Pfeil‡
ac,
Isabel
Bennett
b,
Jascindra
Ravi
a,
Patrizia
Iavicoli
d,
Baptiste
Lamarre
a,
Anita
Roethke
e,
Santanu
Ray
a,
Haibo
Jiang
f,
Angelo
Bella
a,
Bernd
Reisinger
e,
Daniel
Yin
ac,
Benjamin
Little
g,
Juan C.
Muñoz-García
c,
Eleonora
Cerasoli
a,
Peter J.
Judge
c,
Nilofar
Faruqui
a,
Luigi
Calzolai
d,
Andre
Henrion
e,
Glenn J.
Martyna
h,
Chris R. M.
Grovenor
i,
Jason
Crain
ag,
Bart W.
Hoogenboom
b,
Anthony
Watts
c and
Maxim G.
Ryadnov
*a
aNational Physical Laboratory, Teddington, Middlesex TW11 0LW, UK. E-mail: max.ryadnov@npl.co.uk
bLondon Centre for Nanotechnology and Department of Physics and Astronomy, University College London, London WC1E 6BT, UK
cDepartment of Biochemistry, University of Oxford, Oxford OX1 3QU, UK
dEuropean Commission, Joint Research Centre, Institute for Health and Consumer Protection, Ispra (VA), Italy
ePhysikalisch-Technische Bundesanstalt, 38116 Braunschweig, Germany
fCentre for Microscopy, Characterisation and Analysis, The University of Western Australia, Crawley, Western Australia 6009, Australia
gSchool of Physics and Astronomy, University of Edinburgh, Edinburgh EH9 3JZ, UK
hIBM T. J. Watson Research Center, Yorktown Heights, NY 10598, USA
iDepartment of Materials, University of Oxford, Oxford OX1 3PH, UK
First published on 26th September 2016
The spread of bacterial resistance to traditional antibiotics continues to stimulate the search for alternative antimicrobial strategies. All forms of life, from bacteria to humans, are postulated to rely on a fundamental host defense mechanism, which exploits the formation of open pores in microbial phospholipid bilayers. Here we predict that transmembrane poration is not necessary for antimicrobial activity and reveal a distinct poration mechanism that targets the outer leaflet of phospholipid bilayers. Using a combination of molecular-scale and real-time imaging, spectroscopy and spectrometry approaches, we introduce a structural motif with a universal insertion mode in reconstituted membranes and live bacteria. We demonstrate that this motif rapidly assembles into monolayer pits that coalesce during progressive membrane exfoliation, leading to bacterial cell death within minutes. The findings offer a new physical basis for designing effective antibiotics.
These peptide–phospholipid charge interplays derive from differences between cationic lysine and arginine residues, which are primary electrostatic binders to anionic microbial membranes. These amino acids have different chemistries and different free energies of hydration, but both have to overcome the same free energy barrier when crossing membranes in protonated forms. For neutral lysine, which in membranes can remain deprotonated, the barrier is lower than that for neutral arginine.25 Therefore, protonated arginines are favored at all stages of membrane insertion, and starting with surface binding they maintain extensive hydrogen-bonding networks that trap more phosphate and water.16,25 Each arginyl residue can provide five hydrogen-bond donors stabilizing peptide–phosphate clusters and thereby enhancing the affinity between the peptide and the membrane. To enable the formation of electrostatic networks along the helix while inserting in membranes, arginines were evenly distributed in the tilamin sequence. A high concentration of arginines was allowed in the central part of the peptide to arrest its interfacial binding, which was further stabilized by the short hydrophobic face (Fig. 1A).10 To avoid undesired hemolytic effects common for venom peptides (melittin) that have broad hydrophobic faces,7,10 the charge-hydrophobic contributions to the binding were balanced at a 1.5:1 ratio by splitting the polar face into two unequal sub-faces via a neutral alanyl cluster placed opposite to the hydrophobic face. A bulky and hydrophobic tyrosine with propensity for slight β-bends was incorporated into the alanyl cluster in the central part of the helix to help the termini adapt to membrane curvature. The resulting sequence comprises three helical heptads, CNCHNCH, which arrange the same-type residues (i and i + 7 spacing) next to one another when viewed along the helical axis. This spacing contains i, i + 3 and i, i + 4 helical patterns characteristic of canonical coiled coils, known to maintain interfacial contacts in a highly cooperative manner,24 and thus able to support cooperative tilamin assembly in lipid bilayers. Since tilamin is a helical design, all amino acids used have high helical propensity. Finally, an anionic version of tilamin was designed as a non-AMP control (Fig. 1A). This control is important for two reasons. Firstly, the peptide has helical propensity that is comparable to that of tilamin. But, secondly, it lacks the ability to bind to membranes and thence cannot undergo folding-mediated insertion into bacterial lipid bilayers, which renders it non-antimicrobial. Thus, all three designed peptides are cross-referenced controls, with each responsible for a specific mode of interactions with microbial membranes: from no interactions (non-AMP) to folding-mediated transmembrane (amhelin) and monolayer (tilamin) poration.
Tilamin exhibited comparably strong activities against all the bacteria tested with no apparent preference for Gram positive or Gram negative bacteria. By contrast, the activities of amhelin and a naturally occurring AMP, cecropin B,26 were less consistent across different bacteria: Gram positive bacteria tended to be more tolerant to these two peptides and both these peptides were inactive against S. aureus (Table S1†). The differences did not appear systematic and varied from one bacterium type to another, which may be attributed to reversible or phenotypic tolerance to antibiotics.27,28 Similar trends were observed for commercial membrane-active polypeptide antibiotics, daptomycin and polymyxin B, which can preferentially target Gram positive and Gram negative membranes, respectively (Table S1†). Although daptomycin was inactive against Gram negative bacteria, while polymyxin B was toxic to all of these, E. faecalis proved to be tolerant to both antibiotics (Table S1†). Further, tilamin and daptomycin were the only agents with appreciable activity against S. aureus, though daptomycin proved to be marginally hemolytic (Table S1†). Given that among the tested antibiotics only tilamin was non-differentially antimicrobial, the observed variations suggest that the peptide should exhibit a distinctive antimicrobial mechanism.7 In native environments AMPs are secreted to respond to microbial challenge within their proteolytic life time (minutes). Therefore, the mechanism should become apparent within the same timescale. MIC assays are not suitable in this regard as these are optical density measurements performed over much longer periods of time (24 hours) and take no account of changes at the cellular level. To mitigate this, we sought additional evidence.
Firstly, we monitored bacterial cell death by live-dead assays using fluorescence microscopy.10,26 Tilamin caused up to 80% lysis rates at the MIC within the first 30 min for E. coli (Fig. S1†). These were noticeably faster than those of cecropin B and amhelin (both <30%) in the same timeframe, while comparable rates were only seen for amhelin at concentrations three times above MIC (Fig. S1†). Secondly, to better understand the mechanistic basis of the killing kinetics we monitored individual cell lysis by time-lapse atomic force microscopy (AFM) in water. Gram negative bacteria, such as E. coli, present ideal models for this purpose.29 These cells have two distinct membranes (outer and inner or cytoplasmic) with the bilayer thicknesses of 3.7–4.1 nm.23 A thin and highly porous peptidoglycan layer (4 nm) separates the two membranes,30 but cannot protect the inner membrane.31 Moreover, the layer exhibits high affinity to cationic AMPs thereby facilitating their entry to the cytoplasmic membrane.32
Therefore, if tilamin causes poration it should affect both membranes. Consequently, in the context of monolayer poration, one should distinguish the effect of the peptide on the outer leaflets, which are present in both outer and inner membranes, from that on the outer membranes. This may prove to be important as the outer membranes are affected first, which is likely to be associated with their more apparent or advanced removal during tilamin treatment.
Fig. 3 Monolayer poration and progressive membrane removal in live bacteria. (A) Topographic (height) and phase AFM images of live E. coli in water taken at the first 780 s incubation with tilamin. Inset in height image: a height profile taken along the black dotted line on the back of the bacterium, showing 8 nm-deep steps from the outer cell-wall layer to the inner membrane. The outer layer includes the outer membrane (3.7–4.1 nm)23 and a periplasmic peptidoglycan layer (4 nm). (B) High resolution topographic and phase images of the areas marked by white boxes in (A), after correction for background curvature in the height data (see ESI†). These images show exfoliation of the outer membrane and poration in both outer and inner membrane. (C) Height profiles taken along the highlighted lines in (B) (top), and after additional local background subtraction (bottom). These data show the depth profiles of individual pores. (D) High resolution phase images of E. coli during incubation with tilamin, as a function of time (for the corresponding height images, see Fig. S2†). Two different areas are shown. Time-point labels indicate time since injection. Colour scale for height data, see (A) 140 nm (A) and 19 nm (B). Incubation conditions: 3.5 μM, pH 7.4, room temperature (rt). |
Up to this point, tilamin was shown to porate both membranes, but had to affect the outer membranes to induce visible poration in the inner membranes. As a result, the outer membranes underwent a more rapid disintegration, prompting a question of exact pore dynamics in isolated lipid bilayers. Similarly, the impact of affecting intracellular processes that are crucial to cell viability cannot be fully excluded in live bacteria measurements.7 It should be noted however that intracellular targeting is the consequence of membrane permeabilization and may not outcompete poration within the observed timescale of membrane rupture. Indeed, traditional antibiotics, which typically engage with intracellular targets, exhibit much slower killing kinetics that are strictly proportional to the rate of bacterial growth.33 This is unlike membrane-permeabilizing AMPs, which attack both growing and mature bacteria.7
Considering the two points together, it was deemed appropriate to relate the killing and poration rates in live bacteria with the membrane-porating effects of tilamin in isolation from inter-membrane and intracellular processes. To achieve that, we probed the action of tilamin in reconstituted membranes using lipid compositions that yield fluid-phase membranes at booth room and physiological temperatures.34
To visualize the process, supported lipid bilayers (SLBs) were prepared by the surface deposition of the dilauroyl (DLPC/DLPG, 3:1 molar ratio) AUVs on appropriate substrates.10 These preparations had the additional advantage – compared to whole bacteria – of being flat (to within ∼0.1 nm) in their unperturbed state, allowing more accurate depth measurements for tilamin-induced pores by AFM. AFM analyses of SLBs that were fixed after the 15 minutes of tilamin treatment revealed pore-like structures of varying diameters (Fig. 4A). The pores tended to fuse into heterogeneous networks suggesting much faster diffusion through the supported membrane matrix than that of expanding transmembrane pores of amhelin.10
Complementary to these findings, AFM in aqueous solution and in real time showed that the networks were complete within the first 15 min of incubation at the concentrations used (Fig. 4B). The pore depths of ∼1.4 nm were remarkably consistent in the networks and appeared independent of pore sizes and incubation times (>2 hours) (Fig. 4A, B, S5A and B†). This was in contrast to amhelin (Fig. 1A and B) serving for tilamin as a transmembrane control, which can bind to and fold in the microbial membranes, but which porates them by spanning the whole bilayer (Fig. S6†).10 Comparable results of monolayer poration were obtained for thicker SLBs (∼4 nm) assembled as 3:1 molar mixtures of 1-palmitoyl-2-oleoyl-sn-glycero-3-phosphocholine (POPC) and 1-hexadecanoyl-2-(9Z-octadecenoyl)-sn-glycero-3-phospho-(1′-rac-glycerol) (POPG) lipids (Fig. S5C†). In these SLBs, similarly sized pores of 1.2–1.8 nm in depth were formed in abundance at the same time scales as observed on live bacteria and for the DLPC/DLPG (3:1, molar ratio) SLBs. Quantitative analyses of pore size dynamics measured at different depth thresholds showed close distributions of overlapping pore diameters supporting the coalescence of individual pores into larger structures and networks (Fig. S7†). In addition, the coalescence did not have an appreciable effect on pore depths, with depth values being universal across all pores, individual and coalescing (Fig. S7†). These depths agree with the expected difference between a bilayer surface and the hydrophobic surface of an inner monolayer as measured by AFM,37 and thus indicate the local removal of the outer leaflet of the membrane (Fig. 1B).
The pore networks were prone to convert into regions of higher pore densities, the component specificity of which was explicitly confirmed by nanoscale resolution secondary-ion mass spectrometry (NanoSIMS). Fig. 4C shows 12C15N−/12C14N− ratio images obtained from the surfaces of the DLPC/DLPG (3:1, molar ratio) SLBs treated with a 15N-labelled tilamin. Ratios above natural abundance values (0.37%) were evident for larger pore clusters where the peptide content was the highest (10%). The lateral resolution of NanoSIMS, <100 nm38 did not permit the detailed visualization of smaller pores. Outside of the larger clusters, these appeared as high ratio constellations spread across the imaged areas thus supporting the mechanism of continuous and heterogeneous peptide migration (Fig. 4C). Consistent with this, mass spectrometry and gel electrophoresis analyses of tilamin-treated DLPC/DLPG (3:1) AUVs that were subjected to amine-specific cross-linking returned broad mass distributions (Fig. S8A–C†).39 The lowest oligomeric forms that could be assigned comprised 4–7 monomers. These oligomers correlated well with the constellations observed by NanoSIMS and the smallest pores of 5–10 nm measured by AFM in aqueous solution (Fig. S8D†). Quantified size distributions at different depths below the membrane surface to ensure consistency in measurements gave mean radii of the smallest pores in the range of 1–6 nm, i.e. mean diameters of 2–12 nm (Fig. S9†).
Fig. 5 Tilamin-induced lysis of giant unilamellar vesicles. Fluorescence micrograph of GUVs assembled from POPC/POPG (3:1, molar ratio) and incubated in phosphate-buffered saline without (upper) and with (lower) tilamin (10 μM, L/P 100). Key: violet is CellMask™ Deep Red staining GUV membranes, red is for sulforhodamine B staining the interior of the GUVs, green is for carboxyfluorescein-labelled tilamin. See also corresponding Videos S1 and S3.† |
Fig. 6 Tilamin insertion mode. (A) Oriented 2H NMR quadrupolar splittings (ΔvQ) in palmitoyl (POPC/POPG, 3:1 molar ratio) membranes for tilamin deuterated (Ala-d3) at positions 19, 16, 9, 5 at a lipid-peptide (L/P) ratio 25. (B) A GALA-derived and MD-derived ensemble of helix tilt angles for tilamin in the outer leaflet of the phospholipid bilayer showing tilt angles with corresponding insertion depths and horizontal spans of the tilted helix. The helices are not to scale. The helix insertion by the C-terminus (solution 2) is shown (Table S4†). (C) A rudimentary low-oligomer pore constructed by coarse-grained molecular dynamics simulations and converted to atomistic coordinates in a newly equilibrated palmitoyl (POPC/POPG, 3:1 molar ratio) membrane. Membrane slabs are oriented to view the peptide tilts. Peptides, POPC and POPG lipids are in blue, green and red, respectively. (D) Oriented 2H NMR quadrupolar splittings (ΔvQ) in palmitoyl (POPC/POPG, 3:1 molar ratio) membranes for tilamin deuterated (Ala-d3) at position 9 at L/P ratios 100 and 50. |
The root-mean-square deviation (RMSD) plots combining the 2H data with 15N spectra for tilamin labelled at the central tyrosine residue, which provided additional orientational constraints,44 gave overlapping regions of orientational and tilt angles revealing two possible solutions of tilamin insertion (Fig. S13A, B and Table S4†). Both solutions tilted by ∼20° relative to the bilayer plane, which makes helix insertion by the N- or C-terminus equally possible. The inserting end of tilamin for solution 1 (110°) is the N-terminus, whereas for solution 2 (70°) it is reversed (Fig. S13C and Table S4†). Simulated 2H quadrupolar splittings using Spinach software45 returned close fits with the experimental data confirming the solutions (Table S5, Fig. S14A and B†). Complementary to this, atomistic molecular dynamics simulations of a single tilamin helix inserted into the DLPC/DLPG (3:1) bilayer produced similar angle distributions (110–130°) after simulations of 500 ns (Fig. S14C†). Taken together these results are notable for two reasons.
Firstly, the NMR-derived insertion angles match the depth profiles of monolayer pores measured by AFM. With the tilamin helix (3.15 nm) at tilts of 70°, 60° and 50° (or, equivalently, 110°, 120° and 130° for the opposite terminus) with the respect to the membrane normal, its projection onto the membrane normal gives the insertion depths of 1.1, 1.6 and 2 nm, respectively (Fig. 6B and S15†). These orientations yield helix projections of 2.4–3 nm in length in the membrane plane (Fig. 6B), thus giving a minimum of 5–6 nm for a pore with two opposing helices spanning its diameter. The span constitutes a half of a minimal pore facing an opposite helix, i.e. 5–6 nm (Fig. 6B and S15†), which is consistent with the smallest pores of 5–10 nm assembled from low peptide oligomers (Fig. S8†). Such low-oligomer tilamin pores in POPC/POPG (3:1 molar ratio) bilayers were simulated by coarse-grained molecular dynamics, which revealed that transmembrane configurations were not stable: individual peptides tended to move towards one leaflet generating relatively symmetrical monolayer pores, which in newly equilibrated atomistic model membranes46 appeared as partially stabilized in the upper leaflet (Fig. 6C).
Secondly, the palmitoyl POPC/POPG (3:1 molar ratio) and live cell membranes contain unsaturated lipids, which alone cannot support an orientational order,40,41 and their thicknesses exceed the span of the folded tilamin. Therefore, the membranes are unable to fully support transmembrane orientation of the peptide without distorting the bilayer. The dilauroyl DLPC/DLPG (3:1, molar ratio) membranes comprise saturated lipids, are more densely packed and their thickness (3.2 nm) can match the complete transmembrane span of the folded tilamin.10,22 Despite such differences, tilamin promotes the same poration mechanism in all the membranes used. The tilted helix thus appears as an equilibrium configuration that adapts in the outer layer of the bilayer by maintaining close charge interplays with phospholipids. Supportive of this conjecture ssNMR spectra obtained in deuterated palmitoyl POPC/POPG (3:1 molar ratio) membranes showed greater disordering effects in lipid headgroup regions compared to tail regions (Fig. S16†). In accord with this, continuous wave electron paramagnetic resonance (cwEPR) showed appreciable reduction in amplitude of motion about the lipid chain axis at the headgroup regions (Fig. S17†). At decreasing L/P ratios (increasing peptide) tilamin induced clear segmental ordering in lipids that were spin-labelled at the carboxyl ends (nitroxide spin labelled phosphatidylcholine at position 5, 5-PCSL, versus 12-PCSL) (Fig. S17†). Similarly, the same decreasing L/P ratios led to reduced 2H quadrupolar splittings reflecting a more pronounced membrane disruption upon binding more peptide (Table S2, Fig. 6D, S16 and S18†).
Taken together the reduced amplitude of motion, observed at the nanosecond timescale of cwEPR, and the disordering of acyl chains, occurring at the microsecond timescale of 2H NMR, suggest that tilamin tilts into the bilayer and perturbs its upper leaflet across a range of bio-molecular timescales. Atomistic molecular dynamics simulations performed over 500 ns confirmed the nature of tilamin binding as preferential interactions between cationic residues and the anionic (PG) components of the leaflet (Fig. S19†). The simulations also inferred a relative position of the tyrosine side chain in the bilayer interface, which was consistent with the tilamin conformation: the residue showed binding preferences similar to those of the adjacent cationic residues (Fig. 1A, S20A†). Given its central location in the peptide and in the tilt (0.55–1 nm depth; and 1.2–1.5 nm span) the tyrosine should be buried in the upper leaflet (Fig. 6B). Gratifyingly, the intrinsic fluorescence of tyrosine in both membrane types gave characteristic red-shifted increases suggesting a mixed type of interactions in the distorted leaflet, likely involving hydrogen bonding to phosphate groups, hydrophobic interactions to tail regions and cation–π interactions with the choline moieties of DLPC (Fig. S20B†).
In this light, the mechanism of tilamin supports a distinct antimicrobial process. This process is manifested in the rapid assembly of antimicrobial peptides in the outer leaflet of the bilayer forming pore-like structures by inserting in a tilted orientation. The resulting shallow pores impose energy penalties that bacterial membranes cannot accommodate, but which are compensated for by rapid membrane thinning and exfoliation at the sites of pore formation. Such a state of monolayer poration, an “M” state, is distinguished from hydrophilic transmembrane pores, which can equilibrate, stabilize and develop laterally (Fig. 7).
A transmembrane pore can also be viewed as a combination of two porated monolayer interfaces merging into the more favourable configuration of a hydrophilic hole.14 However, this process would require peptides to attack from both the extra- and intra-cellular sides of the bilayer, implying that peptide translocation and engagement with the inner leaflet should occur at rates faster than those necessary for disrupting the outer leaflet – the first and primary target of antimicrobial peptides. Although possible at non-antimicrobial concentrations,14 this scenario may not reflect the biological rationale of AMPs, which are overexpressed by cells at inflammatory sites,50 and whose primary role is to kill microbial cells before proteolytic degradation. The faster AMPs rupture microbial membranes, the more efficient they are. Shallow pores formed in the outer leaflet need not expand or stabilize to lyse microbial cells. The energetically unfavourable configuration they cause by exposing the hydrophobic core of the bilayer to water is unlikely to be mitigated by resealing51 or trans-bilayer (flip-flop) lipid re-arrangements52 observed for transmembrane pores in synthetic bilayers, because the exfoliation of the outer leaflet leaves only an inner leaflet, both sides of which, intra- and extracellular, are exposed to water. Subsequently, this causes the localised membrane rupture, accompanied by the formation of larger and deeper lesions and holes, which constitute the functional hallmark of monolayer poration. For this reason, in live cells monolayer pores appeared as short-lived, but forming continuously and in abundance. Pores in SLBs can be expected to form within the same timescale, which they did, but their stability is defined by a higher activation barrier needed to flip or remove lipids of the lower leaflet from the substrate. Indeed, supported lipid monolayers can remain stable over days in water despite it not being an equilibrium configuration,37 which suggests that monolayer pores in SLBs become kinetically arrested in a sub-gel phase.38
Nonetheless, in all cases – live cells, SLBs and GUVs – tilamin helices are likely to disrupt not only the membrane but also the hydrogen-bond network of associated water, which may also be reflected in the central doublet in the 2H NMR spectra being less resolved with decreasing L/P ratios (Fig. 6D). The helices then can be viewed as hydration shells that progressively intercalate in the outer leaflet and cause orientational correlations between lipids in the areas of increased tilamin concentrations – shallow pores (Fig. 4 and 5). By contrast, phospholipid bilayers alone, and particularly those composed of unsaturated lipids that have a greater variety of configurations, lack such long-range correlations.40 Hydrated tilamin helices might lower the free energy penalty for exposing the hydrophobic core in shallow pores, which may explain the relative stability of these pores within the timescales observed. However, the pores form with abundance and coalesce triggering sharp increases in positive membrane curvature that lead to significant membrane thinning and bulging.41 The abrupt and total rupture of the membrane is an invariable consequence.
With respect to the mode of action, the rates of monolayer poration appeared to directly correlate with bacterial kill rates showing appreciable membrane thinning and exfoliation and antimicrobial effects in the same timescales. The action proved to be folding-dependent and, as seen by NMR spectroscopy, involves molecular dynamics at faster timescales, supporting monolayer poration as a rapid and non-specific antimicrobial mechanism. Upon reaching critical concentrations on the membrane surfaces tilamin splays the lipids in the outer leaflet of the bilayer, where it oligomerizes with the formation of abundant shallow pores. Tilamin oligomers instantaneously remove the outer layer of Gram negative cell walls, while progressively porating their cytoplasmic membranes. Thicker peptidoglycans on the surface of Gram positive bacteria, which lack an outer membrane, might be expected to induce the partial folding and pre-oligomerisation of the peptide before it can reach the cytoplasmic membrane.53 Yet, this had no effect on antimicrobial activity, as tilamin did not differentiate between Gram positive and Gram negative types (Table S1†). In this regard, the non-differentiating mechanism of tilamin that proved to be equally effective in live bacteria and reconstituted anionic membranes can present a generic mode of action that is independent of bacterial lipid compositions. Indeed, lipids in different microbial membranes can vary significantly.54 This underlies an intrinsic limitation of synthetic membranes regardless of the chosen lipids and therefore requires complementary live-bacteria measurements. Most bacterial cells tend to maintain anionic PG components in their membranes, whereas the choice for zwitterionic lipids to distribute the negative charge is seemingly arbitrary among different organisms. For example, E. coli is known to prefer phosphatidylethanolamine (PE), but S. aureus is lacking the lipid completely.55 In P. aeruginosa it mixes with phosphatidylcholines (PC), while double-membrane spirochetes (B. burgdorferi) opt it out for PC.54 Perhaps even more importantly, emerging resistant strains learn to incorporate lipids that are alien to their wild types thus exploiting combinations that may provide them with a competitive advantage.56
Footnotes |
† Electronic supplementary information (ESI) available: Materials and methods, microscopy, spectroscopy, molecular dynamics and spectrometry data. See DOI: 10.1039/c6sc02925f |
‡ Contributed equally to this work. |
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