Abstract:A common feature of ionic liquids composed of cations with long aliphatic side chains is structural heterogeneities on the nanometer length scale. This so-called microphase separation arises from the clustering of aliphatic moieties. The temperature dependence of the liquid bulk structure was studied by small-angle X-ray and neutron scattering for a set of methylimidazolium ([CCim], [CCim]) based ionic liquids with tris(pentafluoroethyl)trifluorophosphate ([FAP]), bis(trifluoromethylsulfonyl)imide ([NTf]), and… Show more
“…1A shows, the typical R/RF shape of n = 16 to 20 is recovered also for n = 22 at high temperatures. The new phase of n = 22 is tentatively identified as the surface equivalent of the bulk liquid-crystal phase reported recently for this compound (38,39). Indeed, the qz positions of the two peaks of n = 22 in Fig.…”
Section: Resultssupporting
confidence: 71%
“…of the chains by introducing gauche defects, the interdigitation motif may largely survive in the RTILs' liquid phase as well, similar to that found in molten alcohols (63,64). The facts that the layer spacing d for all n ≥ 8 is intermediate between ln + 5Å and 2ln + 5Å, that, in the bulk, it increases with n by more than the projected C-C bond length, 1.27Å/CH2, but by less than 2 × 1.27Å/CH2 (6, 7), and that it decreases with increasing temperature despite the overall volume expansion (17,39) are taken, in this approach, as support for chain interdigitation.…”
Section: Discussionsupporting
confidence: 68%
“…The dξ/dn parallels therefore the expected increase in the vdW interaction due to the added methylenes, implying that the layering range is determined by that interaction, with negligible contribution from interactions between the polar headgroups' layers. This, in turn, suggests that the anomalously negative thermal expansion coefficients found for the surface d of [C18mim][FAP] (17), and for the bulk dI of n = 18 and n = 22 (39), originate in the alkyl layer, not in the interaction between the polar headgroups' layers. Finally, we also note that, since d increases with n with a much smaller slope than ξ, ξ/d still increases, reaching values of 1 for n ≥ 18.…”
Interfaces of room temperature ionic liquids (RTILs) are important for both applications and basic science and are therefore intensely studied. However, the evolution of their interface structure with the cation's alkyl chain length [Formula: see text] from Coulomb to van der Waals interaction domination has not yet been studied for even a single broad homologous RTIL series. We present here such a study of the liquid-air interface for [Formula: see text], using angstrom-resolution X-ray methods. For [Formula: see text], a typical "simple liquid" monotonic surface-normal electron density profile [Formula: see text] is obtained, like those of water and organic solvents. For [Formula: see text], increasingly more pronounced nanoscale self-segregation of the molecules' charged moieties and apolar chains yields surface layering with alternating regions of headgroups and chains. The layering decays into the bulk over a few, to a few tens, of nanometers. The layering periods and decay lengths, their linear [Formula: see text] dependence, and slopes are discussed within two models, one with partial-chain interdigitation and the other with liquid-like chains. No surface-parallel long-range order is found within the surface layer. For [Formula: see text], a different surface phase is observed above melting. Our results also impact general liquid-phase issues like supramolecular self-aggregation and bulk-surface structure relations.
“…1A shows, the typical R/RF shape of n = 16 to 20 is recovered also for n = 22 at high temperatures. The new phase of n = 22 is tentatively identified as the surface equivalent of the bulk liquid-crystal phase reported recently for this compound (38,39). Indeed, the qz positions of the two peaks of n = 22 in Fig.…”
Section: Resultssupporting
confidence: 71%
“…of the chains by introducing gauche defects, the interdigitation motif may largely survive in the RTILs' liquid phase as well, similar to that found in molten alcohols (63,64). The facts that the layer spacing d for all n ≥ 8 is intermediate between ln + 5Å and 2ln + 5Å, that, in the bulk, it increases with n by more than the projected C-C bond length, 1.27Å/CH2, but by less than 2 × 1.27Å/CH2 (6, 7), and that it decreases with increasing temperature despite the overall volume expansion (17,39) are taken, in this approach, as support for chain interdigitation.…”
Section: Discussionsupporting
confidence: 68%
“…The dξ/dn parallels therefore the expected increase in the vdW interaction due to the added methylenes, implying that the layering range is determined by that interaction, with negligible contribution from interactions between the polar headgroups' layers. This, in turn, suggests that the anomalously negative thermal expansion coefficients found for the surface d of [C18mim][FAP] (17), and for the bulk dI of n = 18 and n = 22 (39), originate in the alkyl layer, not in the interaction between the polar headgroups' layers. Finally, we also note that, since d increases with n with a much smaller slope than ξ, ξ/d still increases, reaching values of 1 for n ≥ 18.…”
Interfaces of room temperature ionic liquids (RTILs) are important for both applications and basic science and are therefore intensely studied. However, the evolution of their interface structure with the cation's alkyl chain length [Formula: see text] from Coulomb to van der Waals interaction domination has not yet been studied for even a single broad homologous RTIL series. We present here such a study of the liquid-air interface for [Formula: see text], using angstrom-resolution X-ray methods. For [Formula: see text], a typical "simple liquid" monotonic surface-normal electron density profile [Formula: see text] is obtained, like those of water and organic solvents. For [Formula: see text], increasingly more pronounced nanoscale self-segregation of the molecules' charged moieties and apolar chains yields surface layering with alternating regions of headgroups and chains. The layering decays into the bulk over a few, to a few tens, of nanometers. The layering periods and decay lengths, their linear [Formula: see text] dependence, and slopes are discussed within two models, one with partial-chain interdigitation and the other with liquid-like chains. No surface-parallel long-range order is found within the surface layer. For [Formula: see text], a different surface phase is observed above melting. Our results also impact general liquid-phase issues like supramolecular self-aggregation and bulk-surface structure relations.
“…1). [8][9][10][11][12][13][14][15][16][17][18][19][20][21] These studies indicate that CnmimX have some higher-order structures in nanometer scale, which we call "nanostructure." The nanostructure consists of the aggregations of the charged parts of cations and anions and the neutral parts of alkylchains.…”
Section: Introductionmentioning
confidence: 96%
“…c) Electronic mail: yamamuro@issp.u-tokyo.ac.jp During the past decade, great progress has also been made in fundamental scientific studies. [4][5][6] The structural investigations for CnmimX with n < 10 have been performed by using x-ray and neutron diffraction (ND) techniques [7][8][9][10][11][12][13][14][15][16][17][18][19][20][21] and molecular dynamics (MD) simulations. 12,17,[22][23][24][25][26][27][28][29][30] In these studies, a characteristic peak indicative of Q low , which is called "low-Q peak" in this paper, appeared at Q low ≈ 0.3 Å −1 in addition to the peaks at Q ion ≈ 1 Å −1 corresponding to the correlation among ions and at Q alkyl ≈ 1.5 Å −1 corresponding mainly to the correlation among alkylchains (Fig.…”
Alkyl-methyl-imidazolium ionic liquids CnmimX (n: alkyl-carbon number, X: anion) have short-range layer structures consisting of ionic and neutral (alkylchain) domains. To investigate the temperature dependences of the interlayer, interionic group, and inter-alkylchain correlations, we have measured the neutron diffraction (ND) of C16mimPF, C9.5mimPF, and C8mimPF in the temperature region from 4 K to 470 K. The quasielastic neutron scattering (QENS) of C16mimPF was also measured to study the dynamics of each correlation. C16mimPF shows a first-order transition between the liquid (L) and liquid crystalline (LC) phases at T = 394 K. C8mimPF exhibits a glass transition at T = 200 K. C9.5mimPF, which is a 1:3 mixture between C8mimPF and C10mimPF, has both transitions at T = 225 K and T = 203 K. In the ND experiments, all samples exhibit three peaks corresponding to the correlations mentioned above. The widths of the interlayer peak at ca. 0.2 Å changed drastically at the L-LC transitions, while the interionic peaks at ca. 1 Å exhibited a small jump at T. The peak position and area of the three peaks did not change much at the transition. The structural changes were minimal at T. The QENS experiments demonstrated that the relaxation time of the interlayer motion increased tenfold at T, while those of other motions were monotonous in the whole temperature region. The structural and dynamical changes mentioned above are characteristic of the L-LC transition in imidazolium-based ionic liquids.
The temperature (T) and cationic chain length (n) evolution of the nanoscale structure of the sub‐layering‐threshold members of a model family of room temperature ionic liquids (RTILs) is investigated by x‐ray scattering. The measured curves are computer‐resolved into individual Teubner‐Strey‐like lineshapes. The polar‐apolar layering is found to start at n=3
. Opposite n‐trends are found at n≤3
for the spacings and correlation lengths associated with the diffraction patterns’ two main peaks, and assigned to a shift of balance between the two main interactions, Coulomb and van der Waals, and to increasing packing constraints due to the addition of methylenes. The spacings’ thermal expansion coefficients are found to deviate from the macroscopically‐measured values, and to anomalously decrease with increasing temperature. Finally, the reduced temperature scale, t=(T-Tm)/Tm
, (Tm=
melting temperature), is demonstrated to render the observed trends significantly more systematic than those on a conventional T scale.
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