Wiley

Advanced Materials

Published by Wiley

Online ISSN: 1521-4095

·

Print ISSN: 0935-9648

Disciplines: Materials science

Journal websiteAuthor guidelines

Top read articles

622 reads in the past 30 days

Assembly of SPNs in solution. a) Photograph of Si–TA solutions showing color changes as a function of solution aging time. b) In situ growth of catecholate silicate complexes as measured by WAXS. UV–vis spectra of Si–TA solutions at c,d) different aging times and e) different Si:TA molar ratios after 2 h of aging. f) Possible structures of catecholate silicate complexes in solution (the ionic charge and counterions are not shown for simplicity).
Assembly of SPN coatings. a) Deposition of an SPN coating (on planar Au), as monitored by QCM. b) Frequency shifts upon SPN coating formation using precursor solutions at different pHs. c) Raman spectra of an SPN coating and sodium metasilicate. d) Micro‐CT image of an SPN coating on a urea granule. The normalized color map indicates the relative density of the coatings, with red representing higher density, green medium density, and blue lower density. e) False colored cross‐sectional image (original image included in Figure S21d, Supporting Information) and surface image (inset) of urea@SPN. False‐colored processing was performed to facilitate distinction between the coating and the substrate (urea granule). f) Thickness of SPN coating on urea (urea@SPN) prepared at different pH values and photographs of urea granules and urea@SPN (insets). Scale bars are 5 mm. g) Changes in Si:TA molar ratio of SPN coatings assembled at different pH values. h) WAXS spectra of SPN coatings assembled at different molar ratios of Si:TA. i) Thickness of SPN coatings assembled on urea granules with different phenolic ligands, as measured by SEM, and the coating content in the urea@SPN samples (yellow line). The SPN coatings on urea granules were obtained after 10 deposition steps using a solution with a Si:TA molar ratio of 3:1 and pH 8, unless mentioned otherwise. Data are shown as the mean ± standard deviation, with three specimens being analyzed for each sample, where applicable.
Stability of SPN capsules (after removal of urea granules). a,b) Heat maps showing the percentage of SPN coating remaining after incubation in a) different media or b) different pH solutions over 14 days. c) UV–vis spectra of SPN coatings incubated in water at different pH values. d) Mechanism of the oxidation of catechol groups to quinone species. e) Dual pH responsiveness of SPN coatings incubated in different pH solutions for 7 days. f) Schematic representation of SPN states at different pH values. g) UV–vis spectra of SPN coatings incubated in water at pH 12 before and after heating at 90 °C (inset shown photographs of the solutions). Figure 3f was created using BioRender.
Hydrophobic functionalization of SPN coatings. a) Binding kinetics of SPN with LG, as measured by QCM. b) Schematic of the interfacial interactions between the SPN layer and hydrophobic layer (i.e., hydrophobic gallates); inset shows the cross‐sectional SEM view of urea@SPN‐LG. c) ΔD–Δf plot illustrating the adhesion dynamics between SPN and LG. Regime I represents the dynamic adsorption of SPN coatings onto the QCM chip. Regime II represents the dynamic adsorption of LG onto the SPN coatings. d) Frequency shifts upon deposition of hydrophobic gallates on the SPN coating. e) FTIR spectra and f–i) SEM images of SPN coatings with TA (f) and functionalized with different hydrophobic gallates (g–i). j) Micro‐CT image of urea@SPN‐LG. k) WCA of SPN coatings (Si–TA) and SPN coatings functionalized with different hydrophobic gallates. The inset in (k) shows a water droplet on an SPN‐LG coating. l) Thickness of urea@SPN and urea@SPN functionalized with different hydrophobic gallates, as measured from cross‐sectional SEM images. Three specimens were analyzed for each sample, with the data shown as the mean ± standard deviation, where applicable. Figure 4b was partially created using BioRender.
Application of urea@SPN and urea@SPN‐HG as controlled‐release fertilizers. a) Cumulative release of urea from urea@SPN at different pH levels of soils at 25 °C. b,c) Cumulative release rate urea from urea@SPN samples prepared using different deposition cycles (b) and functionalized with different hydrophobic gallates (c). d) Cumulative release of Si⁴⁺ from SPN coatings in soil. e) EDX images of urea@SPN samples post‐functionalized with different metal ions. f) Cumulative release of metal ions in soil from urea@SPN samples functionalized with different metal ions. Release was measured by a colorimetric method for urea and ICP for Si and metal ions. Data are shown as the mean ± standard deviation, and three specimens were analyzed for each sample.

+1

Assembly of Silicate–Phenolic Network Coatings with Tunable Properties for Controlled Release of Small Molecules

November 2024

·

623 Reads

·

·

·

[...]

·

Frank Caruso
View access options

Aims and scope


Advanced Materials, one of the world's most prestigious journals and the foundation of the Advanced portfolio, is the home of choice for best-in-class materials science for more than 30 years.
Following this fast-growing and interdisciplinary field, we are considering and publishing the most important discoveries on any and all materials from materials scientists, chemists, physicists, engineers as well as health and life scientists and bringing you the latest results and trends in modern materials-related research every week.
The Advanced portfolio from Wiley is a family of globally respected, high-impact journals that disseminates the best science from well-established and emerging researchers so they can fulfill their mission and maximize the reach of their scientific discoveries.

Recent articles


An Adaptive Metal–Organic Framework Discriminates Xylene Isomers by Shape‐Responsive Deformation
  • Article

December 2024

Jiaqi Li

·

Bin Sheng

·

Rundao Chen

·

[...]

·

Zongbi Bao

The separation of xylene isomers, especially para‐xylene, is a crucial but challenging process in the chemical industry due to their similar molecular dimensions. Here, a flexible metal–organic framework, Ni(ina)2, (ina = isonicotinic acid) is employed to effectively discriminate xylene isomers. The adsorbent with adaptive deformation accommodates the shapes of isomer molecules, thereby translating their subtle shape differences into characteristic framework deformation energies. Through a combination of multiple local flexibility behaviors, Ni(ina)2 exhibits guest‐specific structural transformations that energetically favor para‐xylene over other isomers. Single‐crystal X‐ray diffraction, in situ powder X‐ray diffraction, and theoretical investigations validate this “adaptive fitting” mechanism, where the degree of structural deformation scales with the mismatch between the molecular shape and pore geometry. As a result, Ni(ina)2 achieves exceptional para‐xylene selectivity in both liquid and vapor phase separations, maintaining a high para‐xylene purity and productivity. This work demonstrates a novel strategy of exploiting framework flexibility to address challenging molecular separations and provides fresh insights into the design of selective adsorbents.


Modulation in Spin State of Co3O4 Decorated Fe Single Atom Enables a Superior Rechargeable Zinc‐Air Battery Performance

December 2024

Yuhua Xie

·

Yumei Feng

·

Shiao Zhu

·

[...]

·

Zehui Yang

High‐performance bifunctional electrocatalyst for oxygen evolution reaction (OER) and oxygen reduction reaction (ORR) is the keystone for the industrialization of rechargeable zinc‐air battery (ZAB). In this work, the modulation in the spin state of Fe single atom on nitrogen doped carbon (Fe1‐NC) is devised by Co3O4 (Co3O4@Fe1‐NC), and a mediate spin state is recorded. Besides, the d band center of Fe is downshifted associated with the increment in eg filling revealing the weakened interaction with OH* moiety, resulting in a boosted ORR performance. The ORR kinetic current density of Co3O4@Fe1‐NC is 2.0‐ and 5.6 times higher than Fe1‐NC and commercial Pt/C, respectively. Moreover, high spin state is found for Co in Co3O4@Fe1‐NC contributing to the accelerated surface reconstruction of Co3O4 witnessed by operando Raman and electrochemical impedance spectroscopies. A robust OER activity with overpotential of 352 mV at 50 mA cm⁻² is achieved, decreased by 18 and 60 mV by comparison with Co3O4@NC and IrO2. The operando Raman reveals a balanced adsorption of OH* species and its deprotonation leading to robust stability. The ZAB performance of Co3O4@Fe1‐NC is 193.2 mW cm⁻² and maintains for 200 h. Furthermore, the all‐solid‐state ZAB shows a promising battery performance of 163.1 mW cm⁻².


Controlling Ion Uptake in Carboxylated Mixed Conductors

December 2024

Zeyuan Sun

·

Mengting Sun

·

Siyu Qin

·

[...]

·

Elsa Reichmanis

Organic mixed ionic‐electronic conductors (OMIECs) have garnered significant attention due to their capacity to transport both ions and electrons, making them ideal for applications in energy storage, neuromorphics, and bioelectronics. However, charge compensation mechanisms during the polymer redox process remain poorly understood, and are often oversimplified as single‐ion injection with little attention to counterion effects. To advance understanding and design strategies toward next‐generation OMIEC systems, a series of p‐channel carboxylated mixed conductors is investigated. Varying side‐chain functionality, distinctive swelling character is uncovered during electrochemical doping/dedoping with model chao‐/kosmotropic electrolytes. Carboxylic acid functionalized polymers demonstrate strong deswelling and mass reduction during doping, indicating cation expulsion, while ethoxycarbonyl counterparts exhibit prominent mass increase, pointing to an anion‐driven doping mechanism. By employing operando grazing incidence X‐ray fluorescence (GIXRF), it is revealed that the carboxyl functionalized polymer engages in robust cation interaction, whereas ester functionalization shifts the mechanism towards no cation involvement. It is demonstrated that cations are pivotal in mitigating swelling by counterbalancing anions, enabling efficient anion uptake without compromising performance. These findings underscore the transformative influence of functionality‐driven factors and side‐chain chemistry in governing ion dynamics and conduction, providing new frameworks for designing OMIECs with enhanced performance and reduced swelling.


Asymmetric Structural MXene/PBO Aerogels for High‐Performance Electromagnetic Interference Shielding with Ultra‐Low Reflection

December 2024

An Liu

·

Hua Qiu

·

Xinghan Lu

·

[...]

·

Junwei Gu

Electromagnetic interference (EMI) shielding materials with low electromagnetic (EM) waves reflection characteristics are ideal materials for blocking EM radiation and pollution. Materials with low reflectivity must be constructed using materials with excellent EM waves absorption properties. However, materials simultaneously possessing both low reflectivity and excellent EMI shielding performance remain scarce, consequently, multilayer structures need to be developed. Poly(p‐phenylene–2,6–benzobisoxazole) nanofibers (PNF) are prepared by deprotonation. PNF are combined with MXene and heterostructure MXene@Ni prepared by in‐situ growth; MXene@Ni/PNF acts as an EM absorption layer while MXene/PNF acts as an EM reflective layer. Finally, (MXene@Ni/PNF)–(MXene/PNF) aerogels are prepared by layer‐by‐layer freeze‐drying based on the layered modular design concept. Experimental characterizations revealed that (MXene@Ni/PNF)–(MXene/PNF) aerogels enable the efficient absorption‐reflection‐reabsorption of EM waves, effectively eliminating EMI. When the mass ratio of MXene to Ni in MXene@Ni is 1:6 and the mass fraction of MXene in the reflective layer is 80 wt.%, the (MXene@Ni/PNF)–(MXene/PNF) aerogels exhibit excellent EMI shielding performance (71 dB) and a very low reflection coefficient (R = 0.10). Finite element simulations verified that the developed asymmetric structural aerogels achieve high EMI shielding performance with low reflection characteristics. In addition, (MXene@Ni/PNF)–(MXene/PNF) aerogels display excellent infrared camouflage ability.


Synergistic Degradation of Durable Polymer Networks by Light and Acid Enabled by Pyrenylsilicon Crosslinks

December 2024

Yutaro Kawano

·

Hiroshi Masai

·

Takuya Tsubokawa

·

[...]

·

Jun Terao

Material photocontrol has gained importance in process engineering and biomedical applications. However, highly photoreactive materials are intrinsically unstable to light, which limits their continuous use in lit environments owing to their gradual deterioration. Herein, synergistically photocontrollable materials in the presence of acid are developed to overcome the conventional trade‐off between their photoreactivity and photostability. Pyrenylsilicon derivatives are designed as synergistically cleavable moieties on C–Si bonds under simultaneous treatment with light and acid through photoinduced dearomatization and protonation to generate the Wheland intermediate, whereas the derivatives are highly stable to light or acid alone. The unique reactivity of pyrenylsilicon derivatives is applied to various polymer network crosslinkers, enabling synergistic control and degradation of materials with light and acids. Because of their high photostability in the absence of acids, these materials can be utilized as optical materials, robust elastomers, and 3D photoprinted gels.


The First Kr‐Selective Carbon Molecular Sieve for Inverse Adsorption of Krypton Over Xenon at Ambient Temperature

December 2024

Fuqiang Chen

·

Fang Zheng

·

Xinlei Huang

·

[...]

·

Zongbi Bao

The efficient adsorption‐based separation of krypton (Kr) and xenon (Xe) is of paramount importance but is challenged by their similar physicochemical properties. While carbon adsorbents are theoretically promising for Kr/Xe sieving, practical success has remained elusive. Here, a series of ultramicroporous carbon molecular sieves synthesized from sucrose‐derived hydrochar is reported. The study employs careful characterization and controlled thermal pyrolysis to tailor ultramicropore formation and elucidate the evolution of the carbon framework. The leading material, C‐Suc‐750, has an ideal pore size of ≈4.0 Å. In particular, C‐Suc‐750 has achieved a remarkable Kr/Xe uptake ratio of 39.3 at ambient conditions, setting a new benchmark for selective Kr adsorption and molecular sieving of Kr/Xe. Breakthrough experiments further confirm the superior molecular sieving performance of C‐Suc‐750, highlighting its potential for Kr recovery in nuclear waste treatment. Moreover, molecular dynamics (MD) simulations demonstrate the critical role of narrow slit‐pore of the carbon molecular sieve in molecular sieving separation of Kr/Xe, providing insights into the mechanism driving this selectivity.


Engineering Semiconducting Polymeric Nanoagonists Potentiate cGAS‐STING Pathway Activation and Elicit Long Term Memory Against Recurrence in Breast Cancer

December 2024

Haitao Yuan

·

Chong Qiu

·

Xiaoxian Wang

·

[...]

·

Jigang Wang

Triple‐negative breast cancer has an immunologically “cold” microenvironment, which leads to resistance to current immunotherapy. The activation of stimulator of interferon genes (STING) pathway has been thought a promising strategy to enhance immunotherapy efficacy. In this study, we adopted a comprehensive strategy that integrates innate immune responses with tumor‐targeting photothermal therapy (PTT) to simultaneously tackle multiple immune‐suppressive mechanisms in breast cancer. This semiconducting polymeric nanoagonists (DPTT‐Mn Lipo NPs) mediated PTT can effectively initiate tumor cell apoptosis and induce ICD, thereby reprogramming the immunosuppressive TME and activating STING. We confirmed the modulation of the TME through the PTT‐mediated ICD effect and the transactivation of the cGAS‐STING pathway in immune cells of the TME due to the released dsDNA via ICD, such as macrophages and DCs. Indeed, DPTT‐Mn Lipo NPs‐mediated PTT promoted M1 polarization of tumor‐associated macrophages, augmented T‐cell infiltration, facilitated dendritic cell (DC) maturation, and regulated type I interferon factor secretion, leading to efficient tumor suppression. Most importantly, the combination of DPTT‐Mn Lipo NPs‐based PTT with a checkpoint blockade therapy (anti‐PD‐1) can elicit long‐term immune memory besides tumor eradication. Collectively, this nano‐system can systemically activate antitumor immunity through STING activation and potentially establish long‐term memory against tumor recurrence.


High Efficiency (>10%) AgBiS2 Colloidal Nanocrystal Solar Cells with Diketopyrrolopyrrole‐Based Polymer Hole Transport Layer

December 2024

Jihyung Lee

·

Cheng Sun

·

Junho Park

·

[...]

·

Jung‐Yong Lee

Silver bismuth disulfide (AgBiS2) colloidal nanocrystals (CNCs) have emerged as ecofriendly photoactive materials with excellent photoconductivity and high absorption coefficients, in compliance with the restriction of hazardous substances (RoHS) guidelines. To maximize the theoretical potential of AgBiS2 CNC solar cells, a new diketopyrrolopyrrole (DPP)‐based polymer, BD2FCT, optimized as a hole transport layer (HTL), is developed. This asymmetric thiophene‐rich polymer HTL effectively complements the optical absorption spectrum of CNCs and forms a homogeneous layer atop the CNCs, facilitating favorable vertical charge transfer through intrinsic molecular packing. Furthermore, the BD2FCT HTL aligns energetically with AgBiS2, significantly reducing charge recombination at the CNC/HTL interfaces and enhancing charge extraction and photocurrent generation across the entire optical absorption spectrum. These characteristics are further optimized through precise molecular engineering. Additionally, a low‐bandgap acceptor, IEICO‐4F, is structurally incorporated with the BD2FCT polymer to further improve charge funneling and complementary absorption. Transient absorption spectroscopy reveals enhanced hole transfer from CNC to BD2FCT‐29DPP:IEICO‐4F, resulting in reduced charge recombination and efficient charge extraction. Consequently, a BD2FCT‐based AgBiS2 CNC solar cell achieves a power conversion efficiency (PCE) of 10.1%, demonstrating significant improvements in short‐circuit current density (JSC) and fill factor (FF).


In‐Plane Adaptive Heteroepitaxy of 2D Cesium Bismuth Halides with Engineered Bandgaps on c‐Sapphire

December 2024

Zhenyu Liu

·

Wei Ju

·

Yongzheng Fang

·

[...]

·

Yufeng Liu

The heteroepitaxy of 2D materials with engineered bandgaps are crucial to broaden the spectral response for their integrated optoelectronic devices. However, it is a challenge to achieve the high‐oriented epitaxy and integration of multicomponent 2D materials with varying lattice constants on the same substrate due to the limitation of lattice matching. Here, in‐plane adaptive heteroepitaxy of a series of high‐oriented 2D cesium bismuth halide (Cs3Bi2X9, X = I, Br, Cl) single crystals with varying lattice constants from 8.41 to 7.71 Å is achieved on c‐plane sapphire with distinct lattice constant of 4.76 Å at a low temperature of 160 °C in an air ambient, benefiting from tolerable interfacial strain by switching compressive stress to tensile stress during a 30° rotation of crystal orientation. First‐principles calculation demonstrates that those are all thermodynamically stable phases, deriving from multiple minima of interfacial energy between single crystals and sapphire substrate. The detectivity of Cs3Bi2I9 photodetector reaches up to 3.7 × 10¹² Jones, deriving from high single‐crystal quality. This work provides a promising experimental strategy and basic theory to boost the heteroepitaxy and integration of 2D single crystals with varying lattice constants on low‐cost dielectric substrate, paving the way for their applications in integrated optoelectronics.


Tailoring Non‐Covalent Interaction Via Single Atom to Boost Interfacial Charge Transfer Toward Photoelectrochemical Water Oxidation

December 2024

Chuanqi Zhang

·

Yueyue Wang

·

Wenming Sun

·

[...]

·

Yang Tian

Photoelectrochemical (PEC) water splitting for hydrogen generation holds immense potential for addressing environmental and energy crises. Tailoring non‐covalent interaction via a single atom is anticipated to realize prominent hole extracting facilitating PEC performance, but it has never been reported. In this study, single atom Co‐N4 is coordinated with 5‐fluoroanthranilic acid (FAA) molecules, then used as a non‐covalent hole‐extracting layer on a BiVO4 substrate. Experiments including X‐ray absorption fine spectra, Kelvin probe force microscopy, transient absorption, and theoretical calculation demonstrate the FAA coordination alters the local configuration of the central Co atom, adjusting the interfacial non‐covalent interaction, thereby reducing the barrier of charge transfer between BiVO4 and the hole‐extracting layer. Consequently, photogenerated carriers are more effectively separated, and the PEC water oxidation performance is significantly enhanced with the photocurrent density of 5.47 mA cm⁻² at 1.23 V versus RHE, much higher than those of previously reported BiVO4 photoanodes composited with porphyrin‐based compounds. Experiments and theoretical simulation confirm that the boosted PEC performance originates from exceptional interfacial charge transfer rather than surface catalysis dynamic. This study provides an efficient strategy for tailoring non‐covalent interaction by regulating single‐atom coordination and promoting hole extract to boost PEC water oxidation activity.


Interfacial Metal‐Solvent Chelation for Direct Regeneration of LiFePO4 Cathode Black Mass

December 2024

Junfeng Li

·

Ruyu Shi

·

Junxiong Wang

·

[...]

·

Guangmin Zhou

Direct regeneration of spent lithium‐ion batteries presents a promising approach to effectively reuse valuable resources and benefit the environment. Unlike controlled laboratory conditions that commonly facilitate impurity purification and minimize structural damage, the LiFePO4 cathode black mass faces significant interfacial challenges, including structure deterioration, cathode‐electrolyte interphase residues, and damage from storage procedures, which hinder lithium replenishment and structure regeneration. Here, a metal‐solvent chelation reaction using a lithium acetylacetonate solution is introduced to address these challenges under ambient conditions. This method regulates the near‐surface structure through strong chelation between Acac‒ anions and Fe (III) elements, thus effectively eliminating the degraded amorphous phase and residual fluorine compounds. By direct lithium connection and reducing diffusion barriers, the reconstructed surface facilitates the re‐lithiation process. The regenerated LiFePO4 cathodes demonstrate a capacity retention of 88.5% after 400 cycles at 1 C, while also outperforming traditional recycling methods in terms of environmental and economic benefits. This approach provides a promising solution for regenerating degraded LiFePO4 cathodes from actual dismantled black mass, thereby accelerating the practical application of battery recycling.


Metal Doping Enabling Defective CoMo‐Layered Double Hydroxide Nanosheets as Highly Efficient Photosensitizers for NIR‐II Photodynamic Cancer Therapy

December 2024

Yu Yang

·

Tingting Hu

·

Kexin Zhao

·

[...]

·

Ruizheng Liang

Photodynamic therapy (PDT) is attracting widespread attention as a promising strategy for tumor treatment. However, the efficacy of PDT is severely limited by the insufficient tissue penetration depth of the light source and low reactive oxygen species (ROS) generation efficiency. Herein, the metal doping strategy is reported to construct a series of defect‐rich M‐doped amorphous CoMo‐layered double hydroxide (a‐M‐CoMo‐LDH, M = Mn, Cu, Al, Ni, Mg, Zn) photosensitizers (PSs) for NIR‐II PDT. Especially, M‐doped CoMo‐LDH nanosheets are synthesized through a simple hydrothermal method and then etched by acid treatment to prepare defect‐rich a‐M‐CoMo‐LDH nanosheets. Under NIR‐II 1270 nm laser irradiation, the defect‐rich a‐Zn‐CoMo‐LDH nanosheets exhibit the optimal PDT performance compared with other a‐M‐CoMo‐LDH nanosheets, and also possess much higher ROS production activity (3.9 times) than that of the pristine a‐CoMo‐LDH, with a singlet oxygen quantum yield up to 1.86, which is the highest among all the reported PSs. After polyethylene glycol (PEG) modification, the a‐Zn‐CoMo‐LDH‐PEG nanosheets can function as an effective inorganic PS for PDT, effectively inducing cell apoptosis in vitro and eradicating tumors in vivo. Notably, transcriptome sequencing analysis and further molecular validation highlight the critical role of the apoptotic/p53/AMPK/oxidative phosphorylation signaling pathways in a‐Zn‐CoMo‐LDH‐PEG‐induced cancer cell apoptosis.


Bonding Optimization Strategies for Flexibly Preparing Multi‐Component Piezoelectric Crystals

December 2024

Yuan Bai

·

Gang Tang

·

Lei Xie

·

[...]

·

Zhou Li

Flexible films with optimal piezoelectric performance and water‐triggered dissolution behavior are fabricated using the co‐dissolution–evaporation method by mixing trimethylchloromethyl ammonium chloride (TMCM‐Cl), CdCl2, and polyethylene oxide (PEO, a water‐soluble polymer). The resultant TMCM trichlorocadmium (TMCM‐CdCl3) crystal/PEO film exhibited the highest piezoelectric coefficient (d33) compared to the films employing other polymers because PEO lacks electrophilic or nucleophilic side‐chain groups and therefore exhibits relatively weaker and fewer bonding interactions with the crystal components. Furthermore, upon slightly increasing the amount of one precursor of TMCM‐CdCl3 during co‐dissolution, this component gained an advantage in the competition against PEO for bonding with the other precursor. This in turn improved the co‐crystallization yield of TMCM‐CdCl3 and further enhanced d33 to ≈71 pC/N, exceeding that of polyvinylidene fluoride (a commercial flexible piezoelectric) and most other molecular ferroelectric crystal‐based flexible films. This study presents an important innovation and progress in the methodology and theory for maintaining a high piezoelectric performance during the preparation of flexible multi‐component piezoelectric crystal films.


High‐Throughput Single‐Cell Analysis of Local Nascent Protein Deposition in 3D Microenvironments via Extracellular Protein Identification Cytometry (EPIC)

December 2024

Marieke Meteling

·

Castro Johnbosco

·

Alexis Wolfel

·

[...]

·

Jeroen Leijten

Extracellular matrix (ECM) guides cell behavior and tissue fate. Cell populations are notoriously heterogeneous leading to large variations in cell behavior at the single‐cell level. Although insights into population heterogeneity are valuable for fundamental biology, regenerative medicine, and drug testing, current ECM analysis techniques only provide either averaged population‐level data or single‐cell data from a limited number of cells. Here, extracellular protein identification cytometry (EPIC) is presented as a novel platform technology that enables high‐throughput measurements of local nascent protein deposition at single‐cell level. Specifically, human primary chondrocytes are microfluidically encapsulated in enzymatically crosslinked microgels of 16 picoliter at kHz rates, forming large libraries of discrete 3D single‐cell microniches in which ECM can be deposited. ECM proteins are labeled using fluorescence immunostaining to allow for nondestructive analysis via flow cytometry. This approach reveals population heterogeneity in matrix deposition at unprecedented throughput, allowing for the identification and fluorescent activated cell sorting‐mediated isolation of cellular subpopulations. Additionally, it is demonstrated that inclusion of a second cell into microgels allows for studying the effect of cell‐cell contact on matrix deposition. In summary, EPIC enables high‐throughput single‐cell analysis of nascent proteins in 3D microenvironments, which is anticipated to advance fundamental knowledge and tissue engineering applications.


a) Chemical structure of LPCMP and the protonated form P‐LPCMP and b) PTPA and P‐PTPA; c) FTIR d) XPS data for LPCMP and P‐LPCMP. e) Protonation was also confirmed through peak deconvolution for nitrogen and compared to LPCMP; f) a clear shift in binding energies toward the higher end is observed in P‐LPCMP.
a) CV analysis and b) rate performance for LPCMP and P‐LPCMP measured in the potential window of 2.5–4.5 V with 70% of active material content in the electrode c) Charge–discharge curve for the LPCMP and P‐LPCMP showing the average potential. Electrostatic potential surface and band gap analysis using the DFT calculation for the original d) and protonated e) structures. Static charge density on different elements for original f) and protonated g) structures.
The FTIR spectra of a) LPCMP and b) P‐LPCMP at different potentials. c) The structural representation of P‐LPCMP and its active sites shows the possible reaction mechanism; d) the mechanism of PF6− insertion in the typical P‐PTPA structures as confirmed by DFT and experiments.
a) EIS analysis of LPCMP and P‐LPCMP at the open circuit voltage of 3.1 V with simulated curves; b) cyclic performance analysis of both LPCMP and P‐LPCMP at the current density of 500 mA g⁻¹ and potential window of 2.5–4.5 V; c) graph showing the position of this work in number of cycles versus capacity retention.
a) Structure of PTPA. b) Rate performance of PTPA and P‐PTPA. c) Rate performance of commercially available PANI before and after protonation. d) Capacity retention comparison with published results, demonstrating that no previous paper approaches our high current density of 20 A g⁻¹. e) Ragone plot showing energy and power density, highlighting that even at an ultra‐high power density of 90 kW, our material retains a very high energy density of 250 Wh kg⁻¹. f) Energy density comparison with reported results at different current densities.
Triphenylamine‐Based Conjugated Microporous Polymers as the Next Generation Organic Cathode Materials
  • Article
  • Publisher preview available

December 2024

·

8 Reads

Kamran Amin

·

Benjamin C. Baker

·

Long Pan

·

[...]

·

Charl F. J. Faul

This paper presents a study on a novel porous polymer based on triphenylamine (LPCMP) as an excellent cathode material for lithium‐ion batteries. Through structural design and a scalable post‐synthesis approach, improvements in intrinsic conductivity, practical capacity, and redox potential in an organic cathode material is reported. The designed cathode achieves a notable capacity of 146 mAh g⁻¹ with an average potential of 3.6 V, using 70% active material content in the electrode. Additionally, through appropriate structural design, the capacity can increase to 160 mAh g⁻¹. Even at a high current density of 20 A g⁻¹ (360C), the cathode maintains a capacity of 74 mAh g⁻¹, enabling full charge within 10 s. A high specific energy density of 569 Wh kg⁻¹ (at 0.1 A g⁻¹) is combined with a very high power density of 94.5 kW kg⁻¹ (at 20 A g⁻¹ corresponding to a specific energy density of 263 Wh kg⁻¹) surpassing the power density of graphene‐based supercapacitors. It exhibits highly stable cyclic performance across various current densities, retaining almost 95% of its initial capacity after 1000 cycles at 5.5C. This work presents a significant breakthrough in developing high‐capacity, high‐potential organic materials for sustainable, high‐energy, and high‐power lithium‐ion batteries.


Growth and structural characterization of Hf/AlN metal/semiconductor superlattice. a) A list of 25 different elemental transition and rare‐earth metals exhibiting hexagonal crystal structure and traditional wurtzite III‐nitride semiconductors are shown along with the mismatches in their in‐plane lattice constant (a) in a colour schematic. The colour contrast scales identify the closely lattice‐matched metal/semiconductor combination. b) The schematic crystal structure and unit cell of the hexagonal elemental metal/III‐A semiconductor superlattices. c) Symmetric 2θ‐ω X‐ray diffraction pattern of Hf/AlN superlattices deposited on (0001) Al2O3 substrates with 50 nm AlN buffer layer. Interference fringes are visible along with the main (0002) superlattice diffraction peak. d) The in‐plane XRD of the superlattices showing the diffraction peaks from (112¯$\bar 2$0) and (202¯$\bar 2$0) planes of Hf/AlN superlattices. e) X‐ray reflectivity (XRR) of the superlattice, showing sharp Kiessig fringes that highlight atomically sharp and abrupt interfaces. f) X‐ray reciprocal space map (RSM) of the superlattices showing pseudomorphic growth and interference fringes that evidence the nominally single‐crystalline and epitaxial nature of the superlattices.
High‐resolution transmission electron microscopy imaging of Hf/AlN metal/semiconductor superlattices. a) TEM micrograph of Hf/AlN superlattice showing distinct layer‐by‐layer Hf and AlN growth on AlN buffer layer deposited on c‐Al2O3. The electron diffraction pattern of the superlattice consists of two sets of diffraction spots corresponding to the superlattice and the substrate. b) HAADF‐STEM micrograph of the superlattice reveals wavy layers bending around the threading dislocations originating at the AlN/c‐Al2O3 interface and high brightness contrast among the Hf and AlN layers. c) Atomic‐resolution imaging of Hf/AlN superlattice at the interface, marked with ABAB hexagonal stacking in Hf layers as shown by the golden colour Hf atoms. The AlN layer appears to begin with an Al‐terminated plane (blue colour of Al atoms) bonded with nitrogen in green colour. d) STEM‐EDS map of the Hf, Al, and N shows the distribution of different elements in the superlattice. The micrograph shows Hf and Al atoms are well‐separated. e) HAADF‐STEM micrograph of Hf layer showing 10 different points, where individual EELS spectra were collected. f) The EELS spectra at the 10 marked points corresponding to the unscreened plasmon exaction are presented. g) The systematic shift of the EELS peak from higher energy at point 1 (Hf/AlN interface) to lower energy at point 5 (centre of Hf layer) matches with the simulated bulk plasmon peaks suggesting slight nitridation at the interface. With respect to the interfaces, the core of the Hf layer contains a lesser amount of diffused nitrogen.
Electrical characterization of Hf/AlN superlattice devices. a) Schematic of Hf/AlN metal/semiconductor superlattice with bottom Hf metallic layer and top aluminium layer. b) The schematic of superlattice devices after the nanofabrication and etching process. c) The optical image of the devices during the electrical measurements. d) The I–V characteristics of the measured superlattice structure are modelled by considering the superlattice as an effective medium consisting of a single metal/semiconductor/metal structure with one forward and one backward Schottky diode. e) Room‐temperature I–V characteristics of the Hf/AlN superlattice exhibit a symmetric nature. The measured I–V curve is fitted with the analytically calculated I–V expression for an MSM diode, as shown in Equation 1 f) Temperature‐dependent I–V characteristics of the superlattice show an increase in the device current at higher temperatures. g) Temperature‐dependent barrier height extracted from the I–V characteristics of superlattice. Barrier height increases with increasing temperature due to the inhomogeneous distribution of barrier height. h) CV characteristics of superlattice devices, where the relative capacitance (Cr) is defined as (CV‐C0)/C0.
Thermoreflectance imaging (TRI) and Seebeck coefficient of Hf/AlN superlattices. a) Temperature‐mapping of the Hf/AlN superlattices 50 µm diameter device obtained with TRI technique. b) The slope of the voltage variation with changes in temperature is fitted to obtain the Seebeck coefficient of 140.05 ± 6.28 µV K⁻¹ c) The averaged temperature in ROI on 50 µm Al contact ensures no bias and low variability in the measurement. d) Schematic of the Schottky barrier at the Hf/AlN/Hf interface formed by the Fermi level pinning to the interface‐induced gap states.
Thermionic Emission in Artificially Structured Single‐Crystalline Elemental Metal/Compound Semiconductor Superlattices

December 2024

·

11 Reads

Rahul Singh Rawat

·

Dheemahi Rao

·

·

[...]

·

Bivas Saha

Metal/semiconductor superlattices represent a fascinating frontier in materials science and nanotechnology, where alternating layers of metals and semiconductors are precisely engineered at the atomic and nano‐scales. Traditionally, epitaxial metal/semiconductor superlattice growth requires constituent materials from the same family, exhibiting identical structural symmetry and low lattice mismatch. Here, beyond this conventional constraint, a novel class of epitaxial lattice‐matched metal/semiconductor superlattices is introduced that utilizes refractory hexagonal elemental transition metals and wide‐bandgap III‐nitride semiconductors. Exemplified by the Hf/AlN superlattices exhibiting coherent layer‐by‐layer epitaxial growth, cross‐plane thermionic emission is observed through current–voltage measurements accomplished for the first time in any metal/semiconductor superlattices. Further, thermoreflectance measurements reveal significant enhancement in cross‐plane Seebeck coefficients attributed to carrier energy filtering by Schottky barriers. Demonstration of artificially structured elemental‐metal/wide‐bandgap compound‐semiconductor superlattices promises to usher in new fundamental physics studies and cutting‐edge applications such as tunable hyperbolic metamaterials, quantum computing, and thermionic‐emission‐based thermoelectric and thermophotonic energy conversion devices.


Surface‐Assisted Passivation Growth of 2D Ultrathin β‐Bi2O3 Crystals for High‐Performance Polarization‐Sensitive Photodetectors

Yang Guo

·

Qing Zhang

·

Zebin Ren

·

[...]

·

Wenping Hu

2D nonlayered materials (NLMs) have garnered considerable attention due to unique surface structure and bright application prospect. However, owing to the strong interatomic forces caused by intrinsic isotropic chemical bonds in all directions, the direct synthesis of ultrathin and large area 2D NLMs remains a tremendous challenge. Here, the surface‐assisted passivation growth strategy is designed to synthesize ultrathin and large size β‐Bi2O3 crystals with the thickness down to 0.77 nm and the lateral size up to 163 µm. These results are primarily ascribed to the bonding between Se atoms and the unsaturated Bi atoms on the surface of β‐Bi2O3, resulting in the surface passivation and promoting the obtaining of ultrathin β‐Bi2O3. Strikingly, the photodetectors based on β‐Bi2O3 flakes exhibit a high photoresponsivity of 71.91 A W⁻¹, an excellent detectivity of 6.09 × 10¹³ Jones, a remarkable external quantum efficiency of 2.4 × 10⁴%, an outstanding anisotropic photodetection and excellent UV imaging capability at 365 nm. This work sheds light on the synthesis of 2D ultrathin NLMs and promotes their applications in multifunctional optoelectronics.


A Metal–Polyphenol‐Based Antidepressant for Alleviating Colitis‐Associated Mental Disorders

December 2024

·

11 Reads

Zihao Wang

·

Zi‐Xi Wang

·

Ke‐Fei Xu

·

[...]

·

Fu‐Gen Wu

Emerging evidence suggests that patients with inflammatory bowel diseases (IBDs) are predisposed to psychosocial disturbances, such as depression and anxiety. Regrettably, clinical antidepressants exhibit unsatisfactory therapeutic efficacy in IBD‐associated psychosocial disturbances, primarily attributed to the inherent intestinal disorders and intricate bidirectional relationship between the gut and the brain. Herein, we report a metal–polyphenol‐based antidepressant to alleviate mental disorders in dextran sulfate sodium‐induced experimental acute colitis mice via modulating the microbiota–gut–brain axis. The antidepressant, termed CSMTC, comprises a core of melittin‐encapsulated natural antioxidant enzymes (i.e., catalase and superoxide dismutase) and a protective shell composed of tannic acid–cerium ion network. Upon oral administration to colitis mice, CSMTC can effectively restore colonic redox balance, reinforce the intestinal barrier, modulate gut microbiota composition, maintain the blood–brain barrier integrity, and regulate systemic immune responses. Notably, behavioral test results reveal that CSMTC significantly alleviates the colitis‐associated mental disorder (e.g., depression‐like behavior) via the microbiota–gut–brain axis by reducing neuroinflammation, enhancing hippocampal neural plasticity, modulating hippocampal immune responses, and restoring neurotransmitter homeostasis. This work may have implications for the development of new nanodrugs for treating inflammation‐associated complications.


Solution‐Processable Metal‐Organic Framework Featuring Highly Tunable Dynamic Aggregation States

Lin Geng

·

Yang Qiao

·

Rui Sun

·

[...]

·

Xian‐He Bu

The limited processability of metal‐organic frameworks (MOFs) is hindered flexibility in the manipulation of their aggregation state and applications. Therefore, achieving highly processable MOFs is of great significance but a challenging goal. Herein, a facile strategy is presented for achieving the construction of solution‐processable Mg‐based MOF, NKU‐Mg‐1, allowing for dynamic control of the aggregation state through dynamic self‐assembly (DySA) process and reversible circularly polarized luminescence (CPL) switcher modulation. Notably, micron‐sized crystals of NKU‐Mg‐1 can be readily dispersed in water to form nano‐sized colloids, triggered by the dynamic COO‐Mg coordination bonding interruption by the competitive H2O‐Mg bonding. Accordingly, the aggregation state of the colloid MOF can be readily tuned from 50–80 nm up to 1000 nm, in turn enabling control of aggregation‐dependent emission. Specially, the solid‐phase aggregation can be controlled via structural transitions between 3D NKU‐Mg‐1‐rec‐1 and 2D NKU‐Mg‐1‐rec‐2 nano‐crystals, as confirmed by 3D electron diffraction. Furthermore, benefiting from its highly dynamic tunable aggregation nature, the rational incorporation of the chiral module confers significant CPL activity (glum up to 0.01). Importantly, controllable dynamic aggregation enables reversible switching of the CPL activity by precisely regulating the aggregation states. The solution‐processable and dynamic aggregation‐tunable features endow it highly promising for applications.


Design of smart adaptive textile inspired from the thermal regulation behaviors of army ant nest. a,b) Photographs of army ant (E. hamatum) nest which is made up entirely of the live ants that link together by grasping their tarsal claws. Reproduced with permission, photos by Daniel Kronauer. c) Illustration of thermal adaptive behaviors of army ant nest including structural change of nest and site migration and the inspiration of integrating the thermal adaptive behavior of army ant nest into ANT design. d,e) Comparison of dimensional response and air permeability (µair) between ANT and commercial textile after wetting. f) Illustration of the features of the proposed ANT and the prototype of the thermal adaptive clothing prepared by ANT.
Reversible structural transformation of wool fiber and yarn actuated by water absorption. a) Principle of structural change of wool yarn. b) Microscopic view of wool fiber under wet (immerse into artificial perspiration for 1 min) and dry conditions (60% relative humidity (RH) environment conditioned for 24 h). c) Simulated strain distribution of wool fiber under tension. d) Microscopic view of wool yarn under wet (100% water content) and dry condition (0% water content). e) Simulated strain distribution of wool yarn under tension. f) Cyclic tensile stroke of wool fiber and yarn during drying‐wetting cycles. g) Relationship between the twist angle and yarn diameter under different water contents. h) Stress–strain and twist angle–strain curves of wet (100% water content) and dry (0% water content) yarn. i,j) Schematic diagrams showing the surface change of wool fiber after plasma treatment. k) Photographs and the corresponding SEM images of wool fabrics before and after plasma treatment. l) The effect of plasma treatment duration on the water absorption rate. m) FTIR spectra of wool fabrics after different times of plasma treatment.
Structural design consideration for ANT. a) Comparison of dimensional response between ordinary and developed structure during drying‐wetting circle. b) Illustration of the different structural changes observed in the ordinary and developed structure during practical application. c) Actuation strain of ordinary and developed structure in horizontal and vertical direction under various water contents. d) The fabric dimension change during drying–wetting cyclic test. e) Air permeability (µair) change of ANT when water content increases. f) The variation in average pore area of ANT under different water content fluctuation, n = 15. g and h) The change of porosity and radiation transmission of fabric under wet (100% water content) and dry conditions (21 °C and 60% RH environment conditioned for 24 h).
Health‐related signals detection ability of ANT. a) Color responses of ANT under various real‐life environments including outdoor and indoor environments. AC = air conditioning. b and c) Demonstration of the developed smartphone application which provides the sensing values and feedback to the user. d–f) Spectral reflectance curves of visible light of the ANT integrated with pH, UV and temperature colorimetric sensors under various experimental conditions. g) Spectral reflectance curves of visible light of ANT after laundering test. h) Photographs of the color changes of pH, UV and temperature sensors under different conditions. i) Durability cyclic testing of the pH, UV and temperature sensors regarding their color changes.
Demonstration of ANT through wear trial. a) Schematic of the wear trial and the wireless temperature sensor's location. b) Measurements of heart rate, running speed and skin surface temperature that covered with ANT and control textile during the trial. c) The comparison the sweat pH and temperature obtained by the ANT‐integrated sensors and laboratory testing. d) Color responses of the colorimetric sensors before and after the wear trial. e) Thermal images of the control and ANT sleeves at the end of experiment. f) The structural transformation of the sleeve in different dimensions before and after the wear trial.
Army Ant Nest Inspired Adaptive Textile for Smart Thermal Regulation and Healthcare Monitoring

Lung Chow

·

Qiang Zhang

·

Xingcan Huang

·

[...]

·

Xinge Yu

A textile material that can dynamically adapt to different environments while serving as an immediate alert system for early detection of life‐threatening factors in the surroundings, not only enhances the individual's health management but also contributes to a reduction in energy consumption for space cooling and/or heating. In nature, different species have their own adaptation system to ambient temperature. Inspired by the army ant nest, herein a thermal adaptive textile known as Army ant Nest Textile (ANT) for thermal management and health monitoring is reported. This textile can promptly respond to perspiration, rapidly absorb sweat, and then transform its architecture to facilitate heat dissipation. Simultaneously, the colorimetric sensing function of ANT allows it to emulate the “site migration” behavior of the army ant nest, which empowers individuals to expeditiously identify multiple health‐related signals such as body temperature, UV radiation, and sweat pH values, and warn them to move to a secure environment, thereby effectively reducing the likelihood of physical harm. Together with its excellent scalability and biocompatibility, the ANT offers a promising direction for the development of next‐generation smart e‐textiles for personal thermal and healthcare management, while satisfying the growing demand for energy saving.


Photocatalysts with different processing. 4CzPN molecule processed by ultrasonication dispersion in water, dissolution in THF/H2O (19/1), and stirring nanoprecipitation (SNP), corresponding to the heterogenous, homogenous, and quasi‐homogenous catalysts, respectively. Dual surfactants of DDBAB/SDBS were employed in SNP for the formation of 4CzPN nanoparticles, resulting in a transparent colloidal solution.
The properties and morphology of the quasi‐homogenous nanoparticles. a) Comparison of average size and poly dispersion index (PDI) for 4CzPN powder (ultrasonicated dispersion in water), 4CzPN nanoparticles formed by SNP, 4CzPN nanoparticles formed by SNP with dual surfactants (DDBAB/SDBS), and 4CzPN dissolved in THF/H2O (v/v = 19/1). b,c) Zeta potentials (b) and dynamic light scattering (DLS) results (c) of SNP‐processed 4CzPN nanoparticles, and 4CzPN/DDBAB/SDBS nanoparticles kept for 30 days (inserts are digital photographs, Dh is the average size of nanoparticles). d–f) Scanning electron microscopy (SEM) images of 4CzPN powder (ultrasonicated dispersion, d), SNP processed‐4CzPN (e), and 4CzPN/DDBAB/SDBS nanoparticles (f), respectively, which represents a morphology reshaping from microscale to nanoscale. g–i) Cryo‐transmission electron microscopy (cryo‐TEM) image (g), high‐angle annular dark field‐scanning transmission electron microscopy (HAADF‐STEM) image (h) and element mapping (i) of 4CzPN nanoparticles with DDBAB/SDBS dual surfactants.
Enhanced photocatalytic hydrogen production in 4CzPN/DDBAB/SDBS nanoparticles. a) Chemical structures of hexadecyl trimethyl ammonium bromide (CTAB), sodium dodecyl benzene sulphonate (SDBS), N, N, N‐trimethyl‐1‐dodecanaminium bromide (DTAB), polyethylene glycol (PEG) and dodecyl dimethyl benzyl ammonium bromide (DDBAB) surfactants. b) Transmittance spectra of 4CzPN molecules dissolved in THF/H2O (v/v = 19/1) solution (orange line), 4CzPN/DDBAB/SDBS nanoparticles (red line) and ultrasonication‐dispersed 4CzPN powder in water (blue line). Insets are the photographs of corresponding homogenous and quasi‐homogenous nanoparticles solution, and heterogenous powder suspension with the concentration of 0.55 mg in 25 mL H2O or THF, respectively. c) Comparison of HERs for 4CzPN powder, 4CzPN in THF/H2O (19/1) solution, 4CzPN nanoparticles, and 4CzPN/DDBAB/SDBS nanoparticles under simulated light irradiation (with AM 1.5G filter). Photocatalysis conditions: 0.55 mg photocatalyst, 25 mL H2O, 7 wt.% Pt based on 4CzPN as co‐catalyst and 0.2 m ascorbic acid. d) Average HERs for nanoparticle synthesized with various surfactants of CTAB, SDBS, DTAB, PEG, DDBAB, and DDBAB/SDBS. e) Averaged HERs for 4CzPN nanoparticle synthesized with different DDBAB concentrations. f) Amount of hydrogen evolved and averaged HERs for 4CzPN/DDBAS/SDBS nanoparticles with different catalyst usages. g) AQYs of the optimized 4CzPN/DDBAS/SDBS nanophotocatalysts measured at the wavelength of 350, 365, 400, and 420 nm, respectively.
Mechanism investigation of the enhanced photocatalysis. a) The electrostatic potential (ESP) and molecular dipole of 4CzPN molecule. The red and light blue represent negative and positive charge, respectively. Blue, gray, and light gray balls refer to N, C, and H atoms, respectively. b) Visual frontier orbitals of the calculated HOMO and LUMO of 4CzPN molecule. Blue, gray, and light gray balls refer to N, C, and H atoms, respectively. c) Water contact angles for blank glass, and film fabricated with 4CzPN, and 4CzPN/DDBAB/SDBS nanoparticles. d,e) Fluorescence quenching (d) and time‐resolved photoluminescence (TRPL) spectra (e) for 4CzPN/DDBAB/SDBS nanoparticles, 4CzPN nanoparticles, 4CzPN powder, and 4CzPN in THF/H2O (19/1) solution, with Pt or without Pt addition (excitation wavelength at 375 nm, IRF was excluded). f) Comparison of photocurrents for bare 4CzPN and 4CzPN/DDBAB/SDBS nanoparticles.
Scaled‐up production of quasi‐homogenous nanophotocatalysts. a) Schematic diagram of FNP flow synthesis, which employed a multi‐inlet vortex mixer for continuous production of molecular nanophotocatalysts. b,c) SEM image and particles size of FNP‐processed 4CzPN/DDBAB/SDBS nanoparticles (insets is photograph of colloidal solution produced). d,e) Comparison of zeta potential and hydrogen evolution for nanophotocatalysts synthesized by SNP and FNP method.
Efficient Quasi‐Homogenous Photocatalysis Enabled by Molecular Nanophotocatalysts with Donor‐Acceptor Motif

Xueyan Liu

·

Miaojie Yu

·

Kai Huang

·

[...]

·

Wei‐Hong Zhu

Polymer semiconductors have attracted much attention for photocatalytic hydrogen evolution, but they typically exhibit micrometer‐sized particles in water‐suspension, causing severe loss in light absorption and exciton recombination. Here a molecular nanophotocatalyst featuring a donor‐acceptor motif is presented that solution is processed via a facile stirring nanoprecipitation method assisted by hydrophilic surfactants, enabling an efficient quasi‐homogenous hydrogen evolution. In contrast to the original bulk powder (heterogeneous system), these quasi‐homogenous nanophotocatalysts exhibit significantly improved light‐harvesting, water‐wettability, and exciton dissociation, resulting in distinctly enhanced (by four‐order‐of‐magnitude) photocatalytic hydrogen evolution rate. The optimized nanophotocatalysts (4CzPN/DDBAB/SDBS) generate an outstanding hydrogen evolution rate of 116.42 mmol g⁻¹ h⁻¹ and apparent quantum yield of 30.2% at 365 nm, which are among the highest reported for single‐junction organic photocatalysts. The scalability of the quasi‐homogenous photocatalysts is further demonstrated using a flow‐based flash nanoprecipitation (FNP) processing.


Hot‐pressing method to prepare the AG3Bi2I9 polycrystalline wafer. a) The structure of (NH2)2CNHNH2⁺ (AG⁺) cation and crystal structure of AG3Bi2I9. b) Schematic illustration of the hot‐pressing process. c) Photograph of the AG3Bi2I9 polycrystalline wafer. d,e) Surface and cross‐sectional SEM images of the AG3Bi2I9 polycrystalline wafer.
Characterization of the AG3Bi2I9 polycrystalline wafer. a) XRD patterns of the AG3Bi2I9 powder and wafer. b) Optical absorption spectrum of the AG3Bi2I9 polycrystalline wafer with its Tauc plot (inset). c) TGA curve of the AG3Bi2I9 polycrystalline wafer and the corresponding first derivative. d) Hardness test of the AG3Bi2I9 polycrystalline wafer. e) Bulk resistivity measurement of the AG3Bi2I9 polycrystalline wafer. f) Dark current drift of the AG3Bi2I9 polycrystalline wafer (inset: schematic illustration of dark current measurement).
X‐ray detection performance of the AG3Bi2I9 polycrystalline wafer. a) Absorption coefficients of Si, a‐Se, CdTe, MA3Bi2I9, and AG3Bi2I9 as a function of photon energy. b) Attenuation efficiency of Si, a‐Se, CdTe, MA3Bi2I9, and AG3Bi2I9 for 40 keV X‐ray photons versus thickness. c) Bias‐dependent photoconductivity curve of the AG3Bi2I9 polycrystalline wafer detector (inset: schematic illustration of the Au/AG3Bi2I9 pollycrystalline wafer/Au vertical structure). d) X‐ray response of the AG3Bi2I9 polycrystalline wafer detector at the dose rate in the range of 0.08 to 1.04 µGy s⁻¹ measured under an electric fields of 60 V mm⁻¹. e) X‐ray response current density of the detector versus the dose rate under the various electric fields. f) Calculated sensitivity of the detector under the various electric fields. g) Sensitivity comparison of the lead‐free HP polycrystalline wafer detectors. h) SNR of the detector at different dose rate under an electric field of 50 V mm⁻¹.
Stability of the AG3Bi2I9 polycrystalline wafer detector. a) Repeatability testing of the detector under continuous X‐ray on and off conditions. b) Sensitivity comparison of the detector stored for 10 months with the initial state. c) Continuous working stability of the detector stored for 10 months. d) Repeatability stability of the detector stored for 10 months.
X‐ray imaging based on the AG3Bi2I9 polycrystalline wafer detector. a) Schematic illustration of the ESF measurement. b) ESF and the corresponding LSF of the detector. c) MTF of the detector obtained from its LSF. d) Schematic illustration of the X‐ray imaging system. e) Photograph of the key selected for the imaging. f) X‐ray image of the key. g) The merging diagram of the object and image of the key.
Large Scale Lead‐Free Perovskite Polycrystalline Wafer Achieved by Hot‐Pressed Strategy for High‐Performance X‐Ray Detection

Ji Yu

·

Yinxian Luo

·

Ning Tian

·

[...]

·

Shengzhong (Frank) Liu

Halide perovskites (HPs) have demonstrated excellent direct X‐ray detection performance. Lead‐free perovskite polycrystalline wafers have outstanding advantages in large‐area X‐ray imaging applications due to their area‐scalability, thickness‐controllability, large bulk resistivity, and ease of integration with large‐area thin film transistor arrays. However, currently lead‐free perovskite polycrystalline wafers possess low sensitivity, typically less than 1000 µC Gy⁻¹ cm⁻², which severely limits their X‐ray detection applications. Here, high‐quality and large scale polycrystalline wafers of AG3Bi2I9 (AG: aminoguanidinium) with short intercluster distances are successfully prepared using a hot‐pressing method. The wafers possess high mobility‐lifetime product of 5.66 × 10⁻³ cm² V⁻¹ and therefore achieve high X‐ray sensitivity of 2675 µC Gy⁻¹ cm⁻², which can be comparable to those of the high‐quality single crystal counterpart reported by the previous research (7.94 × 10⁻³ cm² V⁻¹ and 5791 µC Gy⁻¹ cm⁻²), and represent the best results of the currently lead‐free HP polycrystalline wafers. Besides, the wafers exhibit the X‐ray detection limit as low as 11.8 nGy s⁻¹, excellent long‐term working stability, and high spatial resolution of 5.9 lp mm⁻¹ in imaging. The findings demonstrate that AG3Bi2I9 polycrystalline wafers are feasible for high‐performance X‐ray detection and imaging system.


Multifunctional Photonic Nanomaterials and Devices for Digital Photomedicine via Neuro‐Immune Cross‐Talks

December 2024

·

12 Reads

Seong‐Jong Kim

·

Tae Yeon Kim

·

Hyeongkyu Kim

·

[...]

·

Sei Kwang Hahn

The nervous and immune systems are closely interconnected, and influence the onset and progress of various diseases. Accordingly, understanding the interaction of the neural system and the immune system becomes very important for the treatment of intractable diseases with the analysis of therapeutic mechanisms, such as autoimmune diseases, neurodegenerative diseases, cancers, and so on. The conventional immunomodulation treatments have been mainly carried out by drug administration, but they have suffered from systemic negative side‐effects with only limited effects on the specific disease. In this Perspective, photonic nanomaterials and devices are reviewed and discussed for digitally controlled neurostimulating photomedicine via photobiomodulation and optogenetics from the unique viewpoint of neuro‐immune cross‐talks. The prospects and perspectives to integrate photonic nanomaterials with advanced wearable and implantable healthcare devices are also provided and highlighted to revolutionize the therapeutic strategies by the interaction of neural and immune systems, and optimize the treatment protocols for futuristic digital photomedicine. This approach will revolutionize the fields of neurostimulation and immune regulation for further clinical applications.


Structure and physical properties of MnB4 at ambient pressure. a) The crystal structure of MnB4. The blue and green spheres represent the Mn and B atoms, respectively. Right upper panel: The dimerized Mn–Mn atoms along a‐axis. There are two kinds of Mn–Mn distance in this direction, namely 2.7 Å for the shorter bond (gray color) and 3.2 Å for the longer bond (orange color). Right lower panel: B12 cages around Mn atoms. b) Powder x‐ray diffraction pattern (black open circles) and Rietveld fitting curve (red solid curve) of MnB4. The inset shows the photograph of a prepared single crystal. c) Calculated electronic band structures and density of states of MnB4 at ambient pressure. The red and green colors represent the electronic bands contributed by Mn and B, respectively. A pseudogap feature is observed around the Fermi Level (EF). d) The temperature‐dependent normalized resistivity and specific heat data of MnB4 from 2 to 300 K at ambient pressure. The inset shows the temperature‐dependent specific heat coefficient C/T in the temperature region from 2 to 30 K and the fitting to Debye model (red solid curve).
Pressure‐induced superconductivity in MnB4 under high pressure. a,b) R–T curves of MnB4 under various pressures up to 150 GPa. c) Normalized R/R20K‐T curves of MnB4 at selected pressures. The evolution of superconducting transition can be clearly seen. d) Temperature–Pressure phase diagram of MnB4. The solid yellow circles represent the temperature for the minimum value of resistance in low temperature region. Below this temperature, the resistance shows a weak semiconducting‐like upturn. The other colored symbols represent the values of Tc from different runs of experiments. Here, Tc represents the onset transition temperature. Tc0${T}_{\mathrm{c}}^{0}$ represents the temperature for reaching the zero‐resistance state. FL: Fermi liquid behavior.
Upper critical fields of MnB4 under high pressure. a,b) R‐T curves of MnB4 under various magnetic fields up to 9 T at 114 and 150 GPa. c) The temperature‐dependent upper critical field 𝜇0𝐻c2 at different pressures. Tc is determined by using the criterion of temperature for reaching 95% of the normal state resistance. The red and orange solid lines represent the fitting curve by using the Ginzburg–Landau (G–L) equation.
High‐pressure synchrotron X‐ray diffraction data. a) X‐ray diffraction patterns of MnB4 collected at different pressures up to 128 GPa. b) The derived cell volume as a function of pressure from different experimental runs (S1 and S2). The solid red line is the third‐order Birch–Murnaghan (B–M) fitting curve. c) Pressure dependence of lattice parameters of MnB4 obtained from different experimental runs. A crossover of the lattice constant b and c was observed at ≈60–90 GPa.
Superconductivity up to 14.2 K in MnB4 Under Pressure

Zhe‐Ning Xiang

·

Ying‐Jie Zhang

·

Qing Lu

·

[...]

·

Hai‐Hu Wen

The discovery of superconductivity in 3d transition‐metal compounds with strong magnetism is interesting but rare. Especially for Mn‐based compounds, there exist only very limited materials that show superconductivity. Here, the discovery of superconductivity is reported with an onset transition temperature up to 14.2 K in a Mn‐based material MnB4, which is the highest value among the stoichiometric Mn‐based superconductors. By applying high pressure, the continuous suppression of a weak semiconducting behavior and the occurrence of superconductivity after ≈30 GPa are found. With further increasing pressure, the superconducting transition temperature (Tc) is gradually enhanced and reaches the maximum onset transition value of ≈14.2 K at 150 GPa. The synchrotron X‐ray diffraction data reveal the unchanged monoclinic (S.G: P21/c) symmetry but an unusual crossover of the lattice parameters b and c in a certain pressure region as confirmed by the theoretical calculation. The findings show a promising way to explore high Tc superconductivity by combining the 3d‐transition metal magnetic elements and light elements.


3D Nanofabrication via Directed Material Assembly: Mechanism, Method, and Future

Songyun Gu

·

Bingxu Chen

·

Xiayi Xu

·

[...]

·

Shih‐Chi Chen

Fabrication of complex three‐dimensional (3D) structures at nanoscale is the core of nanotechnology, as it enables the creation of various micro‐/nano‐devices such as micro‐robots, metamaterials, sensors, photonic devices, etc. Among most 3D nanofabrication strategies, the guided material assembly, an efficient bottom‐up approach capable of directly constructing designed structures from precise integration of material building blocks, possesses compelling advantages in diverse material compatibility, sufficient driving forces, facile processing steps, and nanoscale resolution. In this review, we focus on assembly‐based fabrication methods capable of creating complex 3D nanostructures (instead of periodic or 2.5D‐only structures). Recent advances are classified based on the different assembly mechanisms, i.e., assembly driven by chemical reactions, physical interactions, and the synergy of multiple microscopic interactions. The design principles of representative fabrication strategies with an emphasis on their respective advantages, e.g., structural design flexibility, material compatibility, resolution, or applications are analyzed. In the summary and outlook, existing challenges, as well as possible paths to solutions for future development are reviewed. We believe that with recent advances in assembly‐based nanofabrication strategies, 3D nanofabrication has achieved tremendous progress in resolution, material generality, and manufacturing cost, for it to make a greater impact in the near future.


Journal metrics


27.4 (2023)

Journal Impact Factor™


21%

Acceptance rate


43.0 (2023)

CiteScore™


14 days

Submission to first decision


$5,780 / £4,360 / €5,040

Article processing charge