Studies of devices of organic mixed ionic-electronic conductors (OMIECs) have unearthed a discrepancy; unlike other organic semiconductors, OMIECs tend to exhibit high charge carrier mobility despite a large energetic disorder. This has been attributed to the dynamic disorder observed in OMIECs, whereby the energy levels of frontier orbitals are not constant but undergo shifts as a function of time due to interactions with the ionic medium. We develop a method to simulate the dynamic energetic disorder as has been observed for OMIECs. We demonstrate that the mobility of a polymer material undergoing hopping transport increases significantly in the presence of dynamic disorder and further extend the model to explore effects of dynamic disorder on the interactions and delocalisation of electronic states. We parametrized the model to match known OMIEC systems and show that incorporating the dynamic disorder in a charge transport model is essential to compute their mobility.
{"title":"Dynamic disorder as an advantage for charge transport in organic mixed ionic-electronic conductors.","authors":"Kalyani Patrikar, Colm Burke, Alessandro Troisi","doi":"10.1039/d6tc02271e","DOIUrl":"10.1039/d6tc02271e","url":null,"abstract":"<p><p>Studies of devices of organic mixed ionic-electronic conductors (OMIECs) have unearthed a discrepancy; unlike other organic semiconductors, OMIECs tend to exhibit high charge carrier mobility despite a large energetic disorder. This has been attributed to the dynamic disorder observed in OMIECs, whereby the energy levels of frontier orbitals are not constant but undergo shifts as a function of time due to interactions with the ionic medium. We develop a method to simulate the dynamic energetic disorder as has been observed for OMIECs. We demonstrate that the mobility of a polymer material undergoing hopping transport increases significantly in the presence of dynamic disorder and further extend the model to explore effects of dynamic disorder on the interactions and delocalisation of electronic states. We parametrized the model to match known OMIEC systems and show that incorporating the dynamic disorder in a charge transport model is essential to compute their mobility.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-10-08","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13647152/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149134408","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Theresa K Mautz, Fabian Gasser, Roland Resel, Fernando G Warchomicka, Christian Slugovc, Sergey M Borisov
Thin metal-organic framework (MOF) films, known as surface-anchored metal-organic frameworks (SURMOFs), offer convenient handling and a variety of new applications due to the direct immobilization of porous crystalline materials on various substrates. In this study, we demonstrate the feasibility of using luminescent SURMOFs for optical sensing of oxygen both in the gas phase and in organic solvents. Luminescent SURMOFs were prepared from indium(iii) chloride and platinum(ii) tetrakis(4-carboxyphenyl)porphyrin on pre-treated transparent substrates, such as rigid glass or flexible poly(ethylene terephthalate). These SURMOFs have an average thickness of ∼310 nm and exhibit room-temperature phosphorescence (λmax = 645-676 nm). This phosphorescence is efficiently quenched by molecular oxygen in the gas phase (I0/Iair ∼50, Stern-Volmer constant KSV ∼4-13 kPa-1). For the SURMOFs fabricated under similar conditions, the sensitivity does not correlate with the morphology (revealed by scanning electron microscopy) or degree of crystallinity (accessed by grazing-incidence wide angle X-ray scattering) of the porous films. Additionally, it has been demonstrated that the SURMOFs exhibit luminescence in toluene, which is quenched by oxygen (I0/Iair ∼ 2.5, KSV ∼ 0.18 kPa-1). While optical oxygen sensing in organic solvents remains a significant challenge, the presented approach offers a viable solution, provided that future research can mitigate fast photodegradation of the SURMOFs under continuous irradiation.
{"title":"Phosphorescent surface-anchored metal-organic frameworks for optical sensing of oxygen.","authors":"Theresa K Mautz, Fabian Gasser, Roland Resel, Fernando G Warchomicka, Christian Slugovc, Sergey M Borisov","doi":"10.1039/d6tc02088g","DOIUrl":"https://doi.org/10.1039/d6tc02088g","url":null,"abstract":"<p><p>Thin metal-organic framework (MOF) films, known as surface-anchored metal-organic frameworks (SURMOFs), offer convenient handling and a variety of new applications due to the direct immobilization of porous crystalline materials on various substrates. In this study, we demonstrate the feasibility of using luminescent SURMOFs for optical sensing of oxygen both in the gas phase and in organic solvents. Luminescent SURMOFs were prepared from indium(iii) chloride and platinum(ii) tetrakis(4-carboxyphenyl)porphyrin on pre-treated transparent substrates, such as rigid glass or flexible poly(ethylene terephthalate). These SURMOFs have an average thickness of ∼310 nm and exhibit room-temperature phosphorescence (<i>λ</i> <sub>max</sub> = 645-676 nm). This phosphorescence is efficiently quenched by molecular oxygen in the gas phase (<i>I</i> <sub>0</sub>/<i>I</i> <sub>air</sub> ∼50, Stern-Volmer constant <i>K</i> <sub>SV</sub> ∼4-13 kPa<sup>-1</sup>). For the SURMOFs fabricated under similar conditions, the sensitivity does not correlate with the morphology (revealed by scanning electron microscopy) or degree of crystallinity (accessed by grazing-incidence wide angle X-ray scattering) of the porous films. Additionally, it has been demonstrated that the SURMOFs exhibit luminescence in toluene, which is quenched by oxygen (<i>I</i> <sub>0</sub>/<i>I</i> <sub>air</sub> ∼ 2.5, <i>K</i> <sub>SV</sub> ∼ 0.18 kPa<sup>-1</sup>). While optical oxygen sensing in organic solvents remains a significant challenge, the presented approach offers a viable solution, provided that future research can mitigate fast photodegradation of the SURMOFs under continuous irradiation.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-10-05","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13659863/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149178075","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Broderick K Johnson, Nicholas Pogharian, Suitu Wang, Yang Yang, Simon A Egner, Liam C Palmer, Monica Olvera de la Cruz, Samuel I Stupp
Hybrid bonding polymers chemically integrate supramolecular assemblies and covalent macromolecules and can therefore exhibit synergistic functionalities that can impact mechanical properties, catalytic activity, and robotic behavior, among others. In these materials, structural units are connected through both covalent and noncovalent bonds, and this hybrid bonding nature can lead to alterations in nanoscale morphology and internal ordering relative to purely supramolecular or purely covalent polymer systems. We report here on a hybrid bonding polymer in which an ionizable covalent polymer was partially functionalized with electron donor-acceptor dyads and co-assembled with similar dyad small molecules that could form supramolecular polymers on their own. Characterization with UV/Vis spectroscopy revealed charge-transfer interactions among the donor-acceptor dyads in the covalent polymer, the hybrids, and the supramolecular polymer, and wide-angle X-ray scattering indicated a gradual loss of internal order as more covalent polymer was incorporated into the hybrid structures. Interestingly, second harmonic generation confocal microscopy revealed the formation of noncentrosymmetric structures in the hybrid materials but not in the supramolecular polymer. Furthermore, measurements of polarization as a function of applied electric field yielded hysteresis loops characteristic of ferroelectric materials for the hybrid materials, but not for the pure covalent polymer or the pure supramolecular polymer. We found evidence of symmetry breaking and ferroelectricity in the hybrid assemblies only when the covalent polymer was moderately ionized, which suggested that electrostatic interactions played a key role in breaking the centrosymmetry of the donor-acceptor assemblies. Coarse-grained simulations further indicated that electrostatic repulsions between charged groups on the covalent polymers and the donor-acceptor dyad small molecules led to symmetry-breaking defects in these materials and that this effect was most prevalent at moderate degrees of covalent polymer ionization. Such defect-induced ferroelectricity has not been previously reported in other supramolecular ferroelectrics, and further investigation of this symmetry-breaking mechanism could enable simpler fabrication of flexible, lightweight ferroelectric materials.
{"title":"Electron donor-acceptor hybrid bonding polymers exhibit symmetry breaking and ferroelectricity.","authors":"Broderick K Johnson, Nicholas Pogharian, Suitu Wang, Yang Yang, Simon A Egner, Liam C Palmer, Monica Olvera de la Cruz, Samuel I Stupp","doi":"10.1039/d6tc01300g","DOIUrl":"https://doi.org/10.1039/d6tc01300g","url":null,"abstract":"<p><p>Hybrid bonding polymers chemically integrate supramolecular assemblies and covalent macromolecules and can therefore exhibit synergistic functionalities that can impact mechanical properties, catalytic activity, and robotic behavior, among others. In these materials, structural units are connected through both covalent and noncovalent bonds, and this hybrid bonding nature can lead to alterations in nanoscale morphology and internal ordering relative to purely supramolecular or purely covalent polymer systems. We report here on a hybrid bonding polymer in which an ionizable covalent polymer was partially functionalized with electron donor-acceptor dyads and co-assembled with similar dyad small molecules that could form supramolecular polymers on their own. Characterization with UV/Vis spectroscopy revealed charge-transfer interactions among the donor-acceptor dyads in the covalent polymer, the hybrids, and the supramolecular polymer, and wide-angle X-ray scattering indicated a gradual loss of internal order as more covalent polymer was incorporated into the hybrid structures. Interestingly, second harmonic generation confocal microscopy revealed the formation of noncentrosymmetric structures in the hybrid materials but not in the supramolecular polymer. Furthermore, measurements of polarization as a function of applied electric field yielded hysteresis loops characteristic of ferroelectric materials for the hybrid materials, but not for the pure covalent polymer or the pure supramolecular polymer. We found evidence of symmetry breaking and ferroelectricity in the hybrid assemblies only when the covalent polymer was moderately ionized, which suggested that electrostatic interactions played a key role in breaking the centrosymmetry of the donor-acceptor assemblies. Coarse-grained simulations further indicated that electrostatic repulsions between charged groups on the covalent polymers and the donor-acceptor dyad small molecules led to symmetry-breaking defects in these materials and that this effect was most prevalent at moderate degrees of covalent polymer ionization. Such defect-induced ferroelectricity has not been previously reported in other supramolecular ferroelectrics, and further investigation of this symmetry-breaking mechanism could enable simpler fabrication of flexible, lightweight ferroelectric materials.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-09-28","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13650462/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149163543","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Brendan F M Healy, Kelsey J Hall, Sophie L Pain, Nicholas E Grant, John D Murphy
With a direct bandgap and strong photoluminescence (PL) emission, monolayer molybdenum disulfide (1L MoS2) is a promising material for next-generation optoelectronic technologies. However, the intrinsically low PL quantum yield (PLQY) and the requirement for dielectric integration present significant challenges in the realisation of practical MoS2-based devices. Chemical treatment with the superacid bis(trifluoromethanesulfonyl)amide (TFSA) is known to enhance dramatically the PL emission of 1L MoS2 through defect passivation and p-type doping. Conversely, atomic layer deposition (ALD) of a dielectric material can introduce defect states and induce n-type doping, thus degrading the MoS2 optical performance. Despite the competing effects of these two processing routes, the combined impact of superacid treatment and ALD dielectric growth on 1L MoS2 has not been thoroughly studied. In this work, we reveal the instability of the TFSA-enhanced MoS2 PL intensity during subsequent ALD of aluminium oxide (Al2O3), due to thermal exposure and precursor interaction. In contrast, we demonstrate that TFSA treatment of thermal Al2O3-encapsulated 1L MoS2 can successfully enhance the PL intensity by up to two orders of magnitude, even for dielectric films of up to ∼96% surface coverage. This enhancement is suppressed only when the Al2O3 layer becomes sufficiently thick (>∼40 nm) and approaches complete coalescence, preventing access of TFSA-derived species to the underlying MoS2. This work establishes an effective encapsulation/passivation strategy for enhancing the optical performance of dielectric-covered 1L MoS2, offering a practical pathway for integrating chemical passivation into device-relevant architectures.
{"title":"Superacid treatment of dielectric-encapsulated monolayer molybdenum disulfide for enhanced photoluminescence.","authors":"Brendan F M Healy, Kelsey J Hall, Sophie L Pain, Nicholas E Grant, John D Murphy","doi":"10.1039/d6tc02199a","DOIUrl":"10.1039/d6tc02199a","url":null,"abstract":"<p><p>With a direct bandgap and strong photoluminescence (PL) emission, monolayer molybdenum disulfide (1L MoS<sub>2</sub>) is a promising material for next-generation optoelectronic technologies. However, the intrinsically low PL quantum yield (PLQY) and the requirement for dielectric integration present significant challenges in the realisation of practical MoS<sub>2</sub>-based devices. Chemical treatment with the superacid bis(trifluoromethanesulfonyl)amide (TFSA) is known to enhance dramatically the PL emission of 1L MoS<sub>2</sub> through defect passivation and p-type doping. Conversely, atomic layer deposition (ALD) of a dielectric material can introduce defect states and induce n-type doping, thus degrading the MoS<sub>2</sub> optical performance. Despite the competing effects of these two processing routes, the combined impact of superacid treatment and ALD dielectric growth on 1L MoS<sub>2</sub> has not been thoroughly studied. In this work, we reveal the instability of the TFSA-enhanced MoS<sub>2</sub> PL intensity during subsequent ALD of aluminium oxide (Al<sub>2</sub>O<sub>3</sub>), due to thermal exposure and precursor interaction. In contrast, we demonstrate that TFSA treatment of thermal Al<sub>2</sub>O<sub>3</sub>-encapsulated 1L MoS<sub>2</sub> can successfully enhance the PL intensity by up to two orders of magnitude, even for dielectric films of up to ∼96% surface coverage. This enhancement is suppressed only when the Al<sub>2</sub>O<sub>3</sub> layer becomes sufficiently thick (>∼40 nm) and approaches complete coalescence, preventing access of TFSA-derived species to the underlying MoS<sub>2</sub>. This work establishes an effective encapsulation/passivation strategy for enhancing the optical performance of dielectric-covered 1L MoS<sub>2</sub>, offering a practical pathway for integrating chemical passivation into device-relevant architectures.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-09-25","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13613486/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149056581","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
High-mobility organic molecular crystals such as rubrene are important materials for organic electronics, yet a quantitatively predictive description of their charge transport properties remains challenging. Direct mixed quantum-classical nonadiabatic molecular dynamics simulations provide a promising route by explicitly propagating the charge carrier wavefunction, without assuming a specific transport mechanism. However, previous large-scale simulations of apolar molecular crystals have commonly neglected dynamic electrostatic disorder, since evaluation of electrostatic interactions is computationally demanding and the approximation appears plausible for apolar systems. Here, we use the damped shifted-force (DSF) real-space electrostatic summation method, combined with an efficient addition-subtraction scheme, to include dynamic electrostatic disorder in fragment orbital-based surface hopping (FOB-SH) simulations of room-temperature hole transport in rubrene. We find that electrostatic interactions increase the reorganization energy for (hypothetical) nearest neighbour hopping by 29 and 39 meV along the a and b-directions, respectively, relative to a baseline value of 152 meV obtained without electrostatics. In FOB-SH simulations, electrostatic interactions lead to increased site energy disorder, reducing the spatial extent of the hole wavefunction, as measured by a decrease in the inverse participation ratio from 13 to 9, and lowering the predicted mobility along the high-mobility direction from 35 to 21 cm2 V-1 s-1, in close agreement with experiment.
{"title":"Impact of dynamic electrostatic disorder on hole mobility in rubrene: a nonadiabatic molecular dynamics investigation.","authors":"Jan Elsner, Samuele Giannini, Jochen Blumberger","doi":"10.1039/d6tc01991a","DOIUrl":"https://doi.org/10.1039/d6tc01991a","url":null,"abstract":"<p><p>High-mobility organic molecular crystals such as rubrene are important materials for organic electronics, yet a quantitatively predictive description of their charge transport properties remains challenging. Direct mixed quantum-classical nonadiabatic molecular dynamics simulations provide a promising route by explicitly propagating the charge carrier wavefunction, without assuming a specific transport mechanism. However, previous large-scale simulations of apolar molecular crystals have commonly neglected dynamic electrostatic disorder, since evaluation of electrostatic interactions is computationally demanding and the approximation appears plausible for apolar systems. Here, we use the damped shifted-force (DSF) real-space electrostatic summation method, combined with an efficient addition-subtraction scheme, to include dynamic electrostatic disorder in fragment orbital-based surface hopping (FOB-SH) simulations of room-temperature hole transport in rubrene. We find that electrostatic interactions increase the reorganization energy for (hypothetical) nearest neighbour hopping by 29 and 39 meV along the <i>a</i> and <i>b</i>-directions, respectively, relative to a baseline value of 152 meV obtained without electrostatics. In FOB-SH simulations, electrostatic interactions lead to increased site energy disorder, reducing the spatial extent of the hole wavefunction, as measured by a decrease in the inverse participation ratio from 13 to 9, and lowering the predicted mobility along the high-mobility direction from 35 to 21 cm<sup>2</sup> V<sup>-1</sup> s<sup>-1</sup>, in close agreement with experiment.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-09-23","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13628186/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149101233","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Sadi Ege Parim, Thomas E Hooper, Lewis R Owen, Derek C Sinclair
A combination of variable temperature X-ray diffraction, thermal analysis, and electrical measurements by fixed frequency dielectric spectroscopy, impedance spectroscopy, and electro-motive force measurements are used to establish the structure-electrical properties of SrNb2O6 ceramics prepared by the conventional solid state reaction technique. A polymorphic phase transition from a monoclinic, m, (space group P21/c) to an orthorhombic, o, (space group, Pmcn that is isomorphic with Pnma, CaTa2O6) cell occurs at ∼420 °C, accompanied by a negative thermal expansion effect (NTE) along the a-axis. The NTE in the monoclinic phase is driven primarily by a buckling of Nb2O10 dimers linked by corners sharing anions along the b-axis combined with a switch in their canting arrangement along the c-axis across the m- to o-transition. SrNb2O6 ceramics show no evidence of ferroelectricity; however, they display dielectric behaviour below ∼300 °C with m-SrNb2O6 exhibiting a room temperature permittivity of ∼30 that approximately doubles on transformation to o-SrNb2O6. There is significant leakage conductivity associated with adsorption of moisture near room temperature and mixed oxide-ion and p-type electronic conductivity at >300 °C. Both of these space charge related mechanisms are possible origins of the anomalous behaviour in the dielectric spectroscopy measurements that give rise to the apparent ferroelectric behaviour and mask the intrinsic electrical properties of SrNb2O6.
{"title":"Polymorphism, negative thermal expansion and electrical properties of SrNb<sub>2</sub>O<sub>6</sub>.","authors":"Sadi Ege Parim, Thomas E Hooper, Lewis R Owen, Derek C Sinclair","doi":"10.1039/d6tc01467d","DOIUrl":"https://doi.org/10.1039/d6tc01467d","url":null,"abstract":"<p><p>A combination of variable temperature X-ray diffraction, thermal analysis, and electrical measurements by fixed frequency dielectric spectroscopy, impedance spectroscopy, and electro-motive force measurements are used to establish the structure-electrical properties of SrNb<sub>2</sub>O<sub>6</sub> ceramics prepared by the conventional solid state reaction technique. A polymorphic phase transition from a monoclinic, m, (space group <i>P</i>2<sub>1</sub>/<i>c</i>) to an orthorhombic, o, (space group, <i>Pmcn</i> that is isomorphic with <i>Pnma</i>, CaTa<sub>2</sub>O<sub>6</sub>) cell occurs at ∼420 °C, accompanied by a negative thermal expansion effect (NTE) along the <i>a</i>-axis. The NTE in the monoclinic phase is driven primarily by a buckling of Nb<sub>2</sub>O<sub>10</sub> dimers linked by corners sharing anions along the <i>b</i>-axis combined with a switch in their canting arrangement along the <i>c</i>-axis across the m- to o-transition. SrNb<sub>2</sub>O<sub>6</sub> ceramics show no evidence of ferroelectricity; however, they display dielectric behaviour below ∼300 °C with m-SrNb<sub>2</sub>O<sub>6</sub> exhibiting a room temperature permittivity of ∼30 that approximately doubles on transformation to o-SrNb<sub>2</sub>O<sub>6</sub>. There is significant leakage conductivity associated with adsorption of moisture near room temperature and mixed oxide-ion and p-type electronic conductivity at >300 °C. Both of these space charge related mechanisms are possible origins of the anomalous behaviour in the dielectric spectroscopy measurements that give rise to the apparent ferroelectric behaviour and mask the intrinsic electrical properties of SrNb<sub>2</sub>O<sub>6</sub>.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":""},"PeriodicalIF":5.1,"publicationDate":"2026-09-16","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13637028/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149101309","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-08-21eCollection Date: 2026-10-08DOI: 10.1039/d6tc01521b
Dylan Wilkinson, Madeleine McRoberts, Abdul-Wasir Shaka, Sarah K Dugmore, Claire Wilson, Pablo Docampo, Malcolm Kadodwala, Graeme Cooke
Precise control of solid-state fluorescence through molecular design is central to the development of advanced functional materials for sensing, imaging, and optical information storage. In particular, aggregation-induced emission (AIE) and mechanochromic luminogens have emerged as promising platforms for stimuli-responsive photonic applications. Herein, four constitutional isomers of carbonyl-bridged tetraphenylethylene (TPE)-carbazole derivatives were synthesised to systematically investigate how molecular connectivity governs their optoelectronic, aggregation, and mechanoresponsive properties. Distinct structure-property relationships were established, demonstrating that subtle variations in connectivity produce significant differences in electronic structure, molecular packing, aggregation-induced emission, and mechanochromic behaviour. Compounds 1, 3, and 4 exhibit AIE characteristics, whereas compound 2 displays aggregation-caused quenching-like behaviour arising from differences in accessible conformational and solid-state packing states. Among the four isomers, compounds 1 and 2 exhibit mechanochromism, with compound 1 showing highly reversible fluorescence switching, while compound 2 undergoes an irreversible pressure-induced transition associated with a metastable amorphous phase. Fluorescence microscopy revealed an exceptionally low pressure-sensing threshold of 0.2 MPa for compound 1 deposited on paper substrates, enabling sensitive detection of gentle mechanical stimuli and reversible invisible-ink write-erase cycles. These findings establish constitutional isomerism as an effective strategy for controlling aggregation, solid-state organisation, pressure sensitivity, and mechanochromic reversibility, providing molecular design principles for next-generation low-force pressure sensors and stimulus-responsive organic materials.
{"title":"Molecular connectivity-driven tuning of aggregation-induced emission and mechanoresponsive properties in fused TPE-carbazole materials.","authors":"Dylan Wilkinson, Madeleine McRoberts, Abdul-Wasir Shaka, Sarah K Dugmore, Claire Wilson, Pablo Docampo, Malcolm Kadodwala, Graeme Cooke","doi":"10.1039/d6tc01521b","DOIUrl":"10.1039/d6tc01521b","url":null,"abstract":"<p><p>Precise control of solid-state fluorescence through molecular design is central to the development of advanced functional materials for sensing, imaging, and optical information storage. In particular, aggregation-induced emission (AIE) and mechanochromic luminogens have emerged as promising platforms for stimuli-responsive photonic applications. Herein, four constitutional isomers of carbonyl-bridged tetraphenylethylene (TPE)-carbazole derivatives were synthesised to systematically investigate how molecular connectivity governs their optoelectronic, aggregation, and mechanoresponsive properties. Distinct structure-property relationships were established, demonstrating that subtle variations in connectivity produce significant differences in electronic structure, molecular packing, aggregation-induced emission, and mechanochromic behaviour. Compounds 1, 3, and 4 exhibit AIE characteristics, whereas compound 2 displays aggregation-caused quenching-like behaviour arising from differences in accessible conformational and solid-state packing states. Among the four isomers, compounds 1 and 2 exhibit mechanochromism, with compound 1 showing highly reversible fluorescence switching, while compound 2 undergoes an irreversible pressure-induced transition associated with a metastable amorphous phase. Fluorescence microscopy revealed an exceptionally low pressure-sensing threshold of 0.2 MPa for compound 1 deposited on paper substrates, enabling sensitive detection of gentle mechanical stimuli and reversible invisible-ink write-erase cycles. These findings establish constitutional isomerism as an effective strategy for controlling aggregation, solid-state organisation, pressure sensitivity, and mechanochromic reversibility, providing molecular design principles for next-generation low-force pressure sensors and stimulus-responsive organic materials.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":"14 38","pages":"18154-18164"},"PeriodicalIF":5.1,"publicationDate":"2026-08-21","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13648121/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"149134423","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-07-30eCollection Date: 2026-09-17DOI: 10.1039/d6tc02147f
C Soukaras, J I Echavarria, D J Degeling, J Hernandez-Rueda, S Conesa-Boj
Controlling the topology of curved transition-metal dichalcogenides remains challenging because shell formation, precursor conversion and hollowing occur simultaneously during growth. Here, we show that the thickness of sputtered tungsten (W) films provides a direct handle for selecting WS2 nanotube topology during charcoal-assisted oxide-template sulfurization. Varying the initial W thickness from 1 to 100 nm drives a transition from laterally extended WS2-like domains to hollow nanotubes and, finally, to retained-core nanotubes exhibiting shell-front mismatch and spiral-like shell wrapping. Sulfur-free controls, Raman spectroscopy, grazing-incidence X-ray diffraction, transmission electron microscopy and elemental mapping reveal that this transition is governed by the continuity, accessibility, and recession of WO x -derived precursor structures. As an initial test of functionality, multiphoton microscopy further shows that the oxide-core nanotube assemblies are optically active nonlinear emitters, generating second-harmonic, sum-frequency and four-wave-mixing signals that are readily detected under conditions where a WS2 monolayer reference is near the detection limit. These results establish film thickness as a synthetic handle for curved transition-metal dichalcogenide architectures and identify these self-formed nanostructures as a promising platform for nonlinear nanophotonics.
{"title":"Thickness-directed oxide-templated conversion of sputtered tungsten films into WS<sub>2</sub> nanotubes.","authors":"C Soukaras, J I Echavarria, D J Degeling, J Hernandez-Rueda, S Conesa-Boj","doi":"10.1039/d6tc02147f","DOIUrl":"10.1039/d6tc02147f","url":null,"abstract":"<p><p>Controlling the topology of curved transition-metal dichalcogenides remains challenging because shell formation, precursor conversion and hollowing occur simultaneously during growth. Here, we show that the thickness of sputtered tungsten (W) films provides a direct handle for selecting WS<sub>2</sub> nanotube topology during charcoal-assisted oxide-template sulfurization. Varying the initial W thickness from 1 to 100 nm drives a transition from laterally extended WS<sub>2</sub>-like domains to hollow nanotubes and, finally, to retained-core nanotubes exhibiting shell-front mismatch and spiral-like shell wrapping. Sulfur-free controls, Raman spectroscopy, grazing-incidence X-ray diffraction, transmission electron microscopy and elemental mapping reveal that this transition is governed by the continuity, accessibility, and recession of WO <sub><i>x</i></sub> -derived precursor structures. As an initial test of functionality, multiphoton microscopy further shows that the oxide-core nanotube assemblies are optically active nonlinear emitters, generating second-harmonic, sum-frequency and four-wave-mixing signals that are readily detected under conditions where a WS<sub>2</sub> monolayer reference is near the detection limit. These results establish film thickness as a synthetic handle for curved transition-metal dichalcogenide architectures and identify these self-formed nanostructures as a promising platform for nonlinear nanophotonics.</p>","PeriodicalId":84,"journal":{"name":"Journal of Materials Chemistry C","volume":" ","pages":"16144-16155"},"PeriodicalIF":5.1,"publicationDate":"2026-07-30","publicationTypes":"Journal Article","fieldsOfStudy":null,"isOpenAccess":false,"openAccessPdf":"https://www.ncbi.nlm.nih.gov/pmc/articles/PMC13439266/pdf/","citationCount":null,"resultStr":null,"platform":"Semanticscholar","paperid":"148676122","PeriodicalName":null,"FirstCategoryId":null,"ListUrlMain":null,"RegionNum":2,"RegionCategory":"材料科学","ArticlePicture":[],"TitleCN":null,"AbstractTextCN":null,"PMCID":"OA","EPubDate":null,"PubModel":null,"JCR":null,"JCRName":null,"Score":null,"Total":0}
Pub Date : 2026-07-28eCollection Date: 2026-09-17DOI: 10.1039/d6tc01983h
Hai L Feng, Martha Greenblatt, Nathan P Bentley, Tom Lancaster, Adrian D Hillier, Budhika Mendis, Rebecca Rae, Fabio Orlandi, Emma Suard, Thomas J Hicken, Emma E McCabe
We report here the structural and magnetic characterisation of the high-pressure double perovskite Pb2MgReO6. Our analysis using neutron diffraction demonstrates that the second-order Jahn-Teller Pb2+ cation plays the dominant structural role, preventing the proposed delicate quadrupolar order from emerging. We explore the relationship between related polar and antipolar structural phases in the context of other complex double perovskites. Muon-spin relaxation (µSR) measurements suggest that a short-range ordered state occurs for 11.3 K < T < 30 K, before a collinear AFM state sets in for T < 11.3 K. These findings add to our understanding of the structural behaviour of lead-based perovskites, as well as the sensitivity of multipolar order to site symmetry.
本文报道了高压双钙钛矿Pb2MgReO6的结构和磁性表征。我们的中子衍射分析表明,二阶Jahn-Teller Pb2+阳离子起主要的结构作用,阻止了所提出的微妙的四极序的出现。我们在其他复杂的双钙钛矿的背景下探讨了相关的极性和反极性结构相之间的关系。μ -自旋弛豫(µSR)测量表明,在11.3 K < T < 30 K时出现了一个短程有序态,而在T < 11.3 K时出现共线AFM态。这些发现增加了我们对铅基钙钛矿结构行为的理解,以及多极序对位点对称性的敏感性。
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Pub Date : 2026-07-23eCollection Date: 2026-09-17DOI: 10.1039/d6tc01390b
Jamie Swaine, Cyprien Bone, Prakriti Kayastha, Matthew T Darby, Ewan Galloway, Keith T Butler
MAX phases (M n+1AX n ), precursors to MXenes, span a vast compositional space, motivating efficient computational screening for synthesisable candidates. We employ CrystaLLM-π, a large language model fine-tuned on 6179 double transition-metal MAX phases, and demonstrate its ability to generate novel structures consistent with known experimental trends. Using a conditioning vector with two dimensions (a statistically derived MXene derivative count and a surrogate for A-site binding energy), the model was able to target MXene-favourable regions of phase space for generation. Specific condition vectors double novel stable structure generation rates versus unconditioned baselines. Of ten compositionally novel candidates, five exhibit DFT-validated (meta)stability (Ehull < 0.050 eV per atom). This work showcases the potential for autoregressive generative models to explore targeted materials' spaces, offering a scalable framework for accelerated discovery in compositionally complex systems.
MAX相(mn +1AX n)是MXenes的前体,跨越了广阔的组成空间,对可合成的候选物进行了有效的计算筛选。我们使用crystm -π,一个对6179双过渡金属MAX相进行微调的大型语言模型,并证明了它能够生成与已知实验趋势一致的新结构。使用二维条件向量(统计导出的MXene衍生物计数和a位点结合能的替代品),该模型能够针对MXene有利的相空间区域进行生成。特定条件向量加倍新的稳定结构的生成率与无条件基线。在10个成分新颖的候选材料中,有5个具有dft验证的(元)稳定性(E壳< 0.050 eV /原子)。这项工作展示了自回归生成模型探索目标材料空间的潜力,为在组成复杂的系统中加速发现提供了可扩展的框架。
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