Abstract:Acrylate-based polymerized ionic liquids (PILs) with ammonium (Am) or imidazolium (Im) cations and tetrafluoroborate (BF 4 ) or bis(trifluoromethanesulfonyl)imide (TFSI) anions were synthesized and spin coated onto gold interdigitated electrodes on silica to investigate nanoconfinement effects on ion transport. The film thickness ranged from 23 to 313 nm. A significant reduction of the inplane conductivity was observed in some PIL thin films with thickness below 100 nm. Specifically, Am BF 4 PIL showed the lar… Show more
“…Understanding the structural characteristics of polymer thin films is critical to numerous emerging technologies. , For example, self-assembly of block copolymer ( e.g. , layer and cylinder) in thin films is essential to using these materials for nanolithography because the phase behavior can be significantly perturbed relative to the bulk behavior due to interfacial and confinement effects. − Also, conjugated polymers are widely studied in thin-film geometries because the alkyl chain crystallinity and π–π stacked assemblies impact the electron transport properties, , which are valuable for transistors, light-emitting diodes, and photovoltaics. − Similarly, structure–property relationships of ion-containing polymer thin films have received significant interest for their ion transport abilities. − The perfluorinated sulfonic acid polymers ( e.g. , Nafion) are among the most extensively studied ionomers for their applications in the catalyst layer of fuel cells and solar-fuel generators. , Specifically, the studies of Nafion have indicated that producing aligned morphologies of phase-separated sulfonic acid aggregates in a thin film can improve the proton transport properties or catalytic performance. ,− …”
Section: Introductionmentioning
confidence: 76%
“… 8 − 11 Similarly, structure–property relationships of ion-containing polymer thin films have received significant interest for their ion transport abilities. 12 − 15 The perfluorinated sulfonic acid polymers ( e.g. , Nafion) are among the most extensively studied ionomers for their applications in the catalyst layer of fuel cells and solar-fuel generators.…”
We demonstrate that
ionic functionality in a multiblock architecture
produces highly ordered and sub-3 nm nanostructures in thin films,
including bicontinuous double gyroids. At 40 °C, precise ion-containing
multiblock copolymers of poly(ethylene-
b
-lithium
sulfosuccinate ester)
n
(PES
x
Li,
x
= 12 or 18) exhibit layered ionic assemblies
parallel to the substrate. These ionic layers are separated by crystalline
polyethylene blocks with the polymer backbones perpendicular to the
substrate. Notably, above the melting temperature (
T
m
) of the polyethylene blocks, layered PES18Li thin films
transform into a highly oriented double-gyroid morphology with the
(211) plane (
d
211
= 2.5 nm) aligned parallel
to the substrate. The cubic lattice parameter (
a
gyr
) of the double gyroid is 6.1 nm. Upon heating further above
T
m
, the double-gyroid morphology in PES18Li transitions
into hexagonally packed cylinders with cylinders parallel to the substrate.
These layered, double-gyroid, and cylinder nanostructures form epitaxially
and spontaneously without secondary treatment, such as interfacial
layers and solvent vapor annealing. When the film thickness is less
than ∼3
a
gyr
, double gyroids and
cylinders coexist due to the increased confinement. For PES12Li above
T
m
, the layered ionic assemblies simply transform
into disordered morphology. Given the chemical tunability of ion-functionalized
multiblock copolymers, this study reveals a versatile pathway to fabricating
ordered nanostructures in thin films.
“…Understanding the structural characteristics of polymer thin films is critical to numerous emerging technologies. , For example, self-assembly of block copolymer ( e.g. , layer and cylinder) in thin films is essential to using these materials for nanolithography because the phase behavior can be significantly perturbed relative to the bulk behavior due to interfacial and confinement effects. − Also, conjugated polymers are widely studied in thin-film geometries because the alkyl chain crystallinity and π–π stacked assemblies impact the electron transport properties, , which are valuable for transistors, light-emitting diodes, and photovoltaics. − Similarly, structure–property relationships of ion-containing polymer thin films have received significant interest for their ion transport abilities. − The perfluorinated sulfonic acid polymers ( e.g. , Nafion) are among the most extensively studied ionomers for their applications in the catalyst layer of fuel cells and solar-fuel generators. , Specifically, the studies of Nafion have indicated that producing aligned morphologies of phase-separated sulfonic acid aggregates in a thin film can improve the proton transport properties or catalytic performance. ,− …”
Section: Introductionmentioning
confidence: 76%
“… 8 − 11 Similarly, structure–property relationships of ion-containing polymer thin films have received significant interest for their ion transport abilities. 12 − 15 The perfluorinated sulfonic acid polymers ( e.g. , Nafion) are among the most extensively studied ionomers for their applications in the catalyst layer of fuel cells and solar-fuel generators.…”
We demonstrate that
ionic functionality in a multiblock architecture
produces highly ordered and sub-3 nm nanostructures in thin films,
including bicontinuous double gyroids. At 40 °C, precise ion-containing
multiblock copolymers of poly(ethylene-
b
-lithium
sulfosuccinate ester)
n
(PES
x
Li,
x
= 12 or 18) exhibit layered ionic assemblies
parallel to the substrate. These ionic layers are separated by crystalline
polyethylene blocks with the polymer backbones perpendicular to the
substrate. Notably, above the melting temperature (
T
m
) of the polyethylene blocks, layered PES18Li thin films
transform into a highly oriented double-gyroid morphology with the
(211) plane (
d
211
= 2.5 nm) aligned parallel
to the substrate. The cubic lattice parameter (
a
gyr
) of the double gyroid is 6.1 nm. Upon heating further above
T
m
, the double-gyroid morphology in PES18Li transitions
into hexagonally packed cylinders with cylinders parallel to the substrate.
These layered, double-gyroid, and cylinder nanostructures form epitaxially
and spontaneously without secondary treatment, such as interfacial
layers and solvent vapor annealing. When the film thickness is less
than ∼3
a
gyr
, double gyroids and
cylinders coexist due to the increased confinement. For PES12Li above
T
m
, the layered ionic assemblies simply transform
into disordered morphology. Given the chemical tunability of ion-functionalized
multiblock copolymers, this study reveals a versatile pathway to fabricating
ordered nanostructures in thin films.
“…The glass transition temperature, T g , is a key characteristic of polymer materials because many physical and mechanical properties change markedly when a polymer undergoes a glass transition from a rubbery state to a glassy state or vice versa. , For polymer films confined at the nanoscale, perturbations originating at the polymer/free surface and the polymer/solid interfaces often result in deviations of the measured T g from the bulk T g . − Such nanoconfinement behavior is important because it can affect the commercial application of ultrathin polymer films and may aid in understanding the underlying mechanisms of glass transition behavior, which has been a long-standing, unresolved challenge. − Indeed, the T g -confinement behavior of polymers has been the subject of intense research since 1994 when Keddie et al , first reported that, relative to bulk T g , the T g s of polystyrene (PS) and poly(methyl methacrylate) ultrathin films supported on silicon decrease and increase, respectively, with decreasing nanoscale thickness.…”
Nanoconfined polystyrene (PS) films exhibit substantial
reductions
in glass transition temperature (T
g) from
bulk T
g. By incorporating 2–6 mol
% 2-ethylhexyl acrylate (EHA) into styrene (S)-based random copolymers
and characterization via ellipsometry, we show that the T
g-confinement effect for films supported on silicon wafers
is eliminated within experimental uncertainty down to a 15 nm thickness.
Previous studies have neutralized this confinement effect by the copolymerization
of minority levels of styrene with majority levels of a comonomer
that can undergo hydrogen bonding with hydroxyl groups on a substrate
surface, thus counteracting the free-surface-based T
g reduction with a T
g increase
near the substrate interface. In contrast, the T
g-confinement effect is eliminated in our 2–6 mol %
EHA copolymers independent of the presence of substrate surface hydroxyl
groups. Thus, polymer–substrate interfacial hydrogen bonds
play no significant role in neutralizing the T
g-confinement effect in the S-based copolymers with 2–6
mol % EHA. Instead, the neutralization must come from suppressing
free-surface effects via very low levels of an EHA monomer in the
copolymer. Importantly, this simple approach to eliminate the T
g-confinement effects with as little as 2 mol
% EHA is accompanied by only a minor change in bulk T
g and no change in thermal expansivity within the experimental
error relative to PS. Furthermore, this approach cannot be generalized
to other acrylate comonomers, such as n-butyl acrylate.
It neither requires complex syntheses to achieve dense brush, bottlebrush,
or cyclic or ring polymer topologies nor the addition of a plasticizer
or a surfactant to the polymer, earlier approaches that suppressed
the T
g-confinement effect in PS. For a
99:1 mol % S/EHA copolymer, the confinement effect is nearly identical
to that of PS, indicating that a critical yet low EHA level is needed
to eliminate the effect.
“…Conductivity in specific thin-film systems is influenced by solvation-segmental dynamics of ethylene-oxide side chains [23]. The same study that drew connections between substrate properties also concluded that conductivity is affected by confinement [17].…”
Section: Filmsmentioning
confidence: 91%
“…In some cases, the manufacturing of film substrates requires glass transition temperatures greater than the annealing temperature ≈ 150 • C [12]. Moreover, properties of the thin-film substrate, such as the conductivity, are also dominated by dynamics [17].…”
Star polymers represent the case where linear polymers are attached to a central core particle. The molecular weight of a star-polymer can be varied by altering the number of arms and/or the length of each arm. Star-polymers are similar to polymer-tethered nanoparticles in the limit where the nanoparticle size is very small. We study how the properties of pure-polymer melts are altered by adding a small fraction of star-polymers.We study star-polymer/polymer composites by employing molecular dynamics simulations. We quantify how a small fraction of added star-polymer changes the dynamics and glass transition of a bulk pure-polymer material and how these changes depend on the number and length of star arms, as well as intra-star molecular interactions. We find star-polymers are most effective at altering the polymer dynamics when the stars adopt expanded "fluffy" conformations, which can be affected by topology and the internal star interactions. We rationalize these effects by relating the glass transition temperatures to high-temperature activation energy parameters. We extend these observations to the case of ultra-thin composite films, where the stars potentially preferentially segregate to one of the interfaces, which can enhance or diminish the changes that arise from confinement in the film geometry. Thus, star-polymers appear to be a promising route to rationally control property changes in bulk and confined polymer materials. I'm not sure words exist for the degree of appreciation I have for those who have made this thesis possible. My friend and mentor Professor Francis W. Starr never stopped pushing me beyond what I thought I was capable of. His unending patience, encouragement, and support has shaped who I am today. Thanks to him, I have become a better writer, science communicator, and critical thinker. So if you're reading this man, you have really made a huge impact in my life as a role model. I'd also like to thank two professors who have ignited a flame in my soul. Professor Blümel's continued enthusiasm while teaching Quantum Mechanics II made me rediscover my love for physics. Professor Personick's expertise in nanotechnology and guidance in applying for graduate school solidified my choice to pursue a career in science. Both of you made it possible for me to attend graduate school. Thank you to my readers, Professor Paily and Brian. I have had the pleasure of taking courses with the both of you. Professor Paily was my first physics professor at Wesleyan. Your kindness and enthusiasm is recognized by all physics majors I know. Brian, your yearly earth rants are events I don't want to miss. Your support and insights also motivated me to pursue graduate school. I'd also like to give a big shout out to Starr Lab. Thank you Hongjia Z, Rakib H, Tom MS, and Tom A for the deep philosophical conversations, moments shared in Chicago, insights, and friendship. I look forward to continuing work with you all in the future. Thank you Jinpeng Fan for early guidance. Thank you to my dearest friends and housema...
scite is a Brooklyn-based organization that helps researchers better discover and understand research articles through Smart Citations–citations that display the context of the citation and describe whether the article provides supporting or contrasting evidence. scite is used by students and researchers from around the world and is funded in part by the National Science Foundation and the National Institute on Drug Abuse of the National Institutes of Health.