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@ARTICLE{OteroMato:863374,
author = {Otero-Mato, José M. and Montes-Campos, Hadrián and
Cabeza, Oscar and Diddens, Diddo and Ciach, Alina and
Gallego, Luis J. and Varela, Luis M.},
title = {3{D} structure of the electric double layer of ionic
liquid–alcohol mixtures at the electrochemical interface},
journal = {Physical chemistry, chemical physics},
volume = {20},
number = {48},
issn = {1463-9084},
address = {Cambridge},
publisher = {RSC Publ.66479},
reportid = {FZJ-2019-03447},
pages = {30412 - 30427},
year = {2018},
abstract = {Mixtures of the ionic liquid 1-butyl-3-methylimidazolium
tetrafluoroborate with amphiphilic cosolvents, such as
methanol and ethanol, nanoconfined between graphene walls
are studied by means of molecular dynamics simulations and
the results are compared with those of the pure ionic liquid
and its mixtures with water confined in the same conditions.
We investigate the adsorption of cosolvent molecules at the
graphene walls as well as their distribution across the
system. The results show that, due to a higher affinity of
the polar groups to be close to the anions in combination
with the electrostatic and excluded volume interactions,
there exists a high tendency of the OH groups to lie close
to the anode, inducing small changes in the first cation
layer. The orientation of cosolvent molecules is found to be
closely related to the alignment of the molecular dipole
moment. We also investigate the lateral ionic distribution
in the layers close to the electrodes, which shows a
structural transition from liquid-like lamellar ordering to
solid-like hexagonal patterns as the size of the cosolvent
molecules increases leading to smaller position fluctuations
of the ions. The dependence of the specific patterns on the
nature of the electrodes is also studied. This study
strongly suggests that the ionic patterns formed in the
first ionic layers next to the charged interfaces are
universal since their existence does not crucially depend on
the atomic composition of the interfacial material, but only
on the net charge density of the considered ionic layer,
which significantly changes the ionic mobility in this
region.},
cin = {IEK-12},
ddc = {540},
cid = {I:(DE-Juel1)IEK-12-20141217},
pnm = {131 - Electrochemical Storage (POF3-131)},
pid = {G:(DE-HGF)POF3-131},
typ = {PUB:(DE-HGF)16},
pubmed = {pmid:30500015},
UT = {WOS:000453231100031},
doi = {10.1039/C8CP05632C},
url = {https://juser.fz-juelich.de/record/863374},
}