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@ARTICLE{Bhowmik:154875,
author = {Bhowmik, D. and Pomposo, J. A. and Juranyi, F. and García
Sakai, V. and Zamponi, M. and Arbe, A. and Colmenero, J.},
title = {{I}nvestigation of a {N}anocomposite of 75 wt $\%$
{P}oly(methyl methacrylate) {N}anoparticles with 25 wt $\%$
{P}oly(ethylene oxide) {L}inear {C}hains: {A} {Q}uasielatic
{N}eutron {S}cattering, {C}alorimetric, and {WAXS} {S}tudy},
journal = {Macromolecules},
volume = {47},
number = {9},
issn = {1520-5835},
address = {Washington, DC},
publisher = {Soc.},
reportid = {FZJ-2014-04118},
pages = {3005 - 3016},
year = {2014},
abstract = {We have investigated the thermal behavior, local structure,
and dynamics in a system where 25 wt $\%$ PEO [poly(ethylene
oxide)] linear chains are mixed with 75 wt $\%$ PMMA
[poly(methyl methacrylate)] soft nanoparticles. Calorimetric
and wide-angle X-ray scattering experiments point to a weak
penetration of the PEO chains in the nanoparticles,
qualifying the mixture as a nanocomposite. Quasi-elastic
neutron scattering (QENS) experiments on partially
deuterated samples has selectively revealed the component
dynamics in the system. The α-methyl group dynamics of
PMMA, which fall within the QENS time scale in the
temperature range investigated, are hardly affected by the
presence of PEO except for hints of a more heterogeneous
environment in the nanocomposite than in bulk PMMA. The
effects on the dynamics of PEO are more interesting. The
observation of dynamics in the microseconds range for the
PEO component of the nanocomposite at temperatures at which
the calorimetric experiments indicate the freezing of its
segmental relaxation provides evidence for confined dynamics
below the main glass transition of the
mixture—attributable to the effective glass transition of
the slow component. A parallel study on an equivalent blend
of PEO and linear PMMA chains shows that these effects are
independent of the topology of the PMMA. However, well above
the effective glass transition of the slow component, the
dynamics of PEO differ in both systems. In the linear blend,
PEO segments move with the typical features of supercooled
polymers in metastable equilibrium, while in the
nanocomposite PEO dynamics exhibit an anomalously strong
deviation from Gaussian behavior. This deviation grows with
increased mobility of the nanoparticles. PEO segments are
seemingly trapped in effective cages imposed by the
nanoparticles for a very long time—more than 2 orders of
magnitude longer than in bulk or when surrounded by linear
PMMA chains—before the subdiffusive process leading to
segmental relaxation sets in. We speculate that local loops
in the surface of the nanoparticles may play an important
role in this trapping mechanism.},
cin = {Neutronenstreuung ; JCNS-1 / JCNS (München) ; Jülich
Centre for Neutron Science JCNS (München) ; JCNS-FRM-II /
ICS-1},
ddc = {540},
cid = {I:(DE-Juel1)JCNS-1-20110106 /
I:(DE-Juel1)JCNS-FRM-II-20110218 /
I:(DE-Juel1)ICS-1-20110106},
pnm = {451 - Soft Matter Composites (POF2-451) / 54G - JCNS
(POF2-54G24)},
pid = {G:(DE-HGF)POF2-451 / G:(DE-HGF)POF2-54G24},
experiment = {EXP:(DE-MLZ)SPHERES-20140101},
typ = {PUB:(DE-HGF)16},
UT = {WOS:000336020900028},
doi = {10.1021/ma500215f},
url = {https://juser.fz-juelich.de/record/154875},
}