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Small Methods

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Online ISSN: 2366-9608

Disciplines: Materials science

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Schematic illustration of the data acquisition protocol. a) 4D‐SPED technique where a precessed nano‐sized beam is scanned over a needle‐shaped sample and electron diffraction patterns are recorded pixel by pixel using a pixelated detector. b) The 4D‐SPED dataset is acquired tilt by tilt in the range from −80° to +80° at a tilt step of 10° using an on‐axis rotation tomographic holder. The sample is cleaned in a low‐kV Argon ion shower before being loaded into the APT chamber. c) The sample is field evaporated using electric and laser pulses and atoms are collected on a position sensitive detector.
a) ACOM illustration demonstrating the correlation between the best‐matched diffraction template (open red circle) and an experimental diffraction pattern extracted from 60° tilt dataset. b) The orientation‐specific virtual dark field image calculated using these virtual apertures (open red circle). c) Orientation‐specific virtual dark field images of a grain tracked through the entire tilt series. d) The 3D reconstructed isosurface rendering of this grain in two different view angles. e) The 3D reconstructed isosurface rendering of the Ni‐W nanocrystalline alloy in two different view angles. Each grain is colored by its average orientation projected along the z‐axis. f) GB habit planes were reconstructed from the 3D reconstructed volume shown in (e) and segmented into triangular mesh. Mesh faces are colored according to their crystallographic plane orientation in inverse pole figure (IPF) color. g) The GBs from the highlighted (black dashed line) region in (f) and its GB habit plane normal distribution plot. Scale bars are 50 nm.
a) The voltage curve for the sample until fracture. The region highlighted by the black rectangle was used to generate the detector event histogram in (b). b) The detector event histogram with multiple ion events revealing a crystallographic pole, here <111>, along the tip axis (z‐axis). c) z‐SDM of all ions in the selected sub‐volume enabling to refinement the reconstruction parameters to match the spacing of the lattice planes to {111} fcc of Ni. d) 3D atom map of the reconstructed volume displaying the distribution of Ni, Cu, and Si atoms. e) Overlay of iso‐concentration surfaces of Cu (10 at.%, orange) and Si (1 at.%, blue) obtained by APT on the GB surface network (gray surface) reconstructed from 4D‐SPEDT (shown in Figure 2e) for two different view angles. The corresponding 3D crystal orientation map is shown for comparison. Scale bars are 50 nm.
a) 3D crystal orientation of the tip of the needle‐shaped sample with indicated GB types, their corresponding misorientation angle, and global GB habit plane. b) GB habit plane map colored according to the IPF color code. The GB habit plane map consists of two closely spaced surfaces corresponding to the GB plane normal of the adjacent crystals. c) Exploded view of the GB habit plane map showing the two surfaces superimposed on the corresponding 3D atom map of Cu and Si obtained by APT. d) The same explosion view as in (c) in a different view angle showing the GB between G1 and G3 plane on. e) Concentration profile extracted across the high angle GB G3‐G4 showing strong Cu enrichment. The Si profile is not shown here since it does not show any significant sign of segregation. f) Concentration profile extracted across the high angle GB G1‐G3 with a slight indication of Cu and Si segregation.
a) A cropped region from 3D reconstructed grains highlights the front (translucent) and back (solid) grains colored according to the IPFcolor code pointing along z‐axis. b) GBs of interest (coherent and incoherent twin boundaries, and incommensurate GB) are marked. c) and d) shows Cu atoms and Si atoms density map respectively, on a 2D plane perpendicular to its iso‐concentration surface placed such that the decoration of Cu and Si atoms can be visualized. In (d), a discontinuous enrichment up to 3 atoms nm⁻³ of Si can be visualized. e) 1D compositional profile measured across the incommensurate GbB in the direction of white arrow in (d) showing the maximum enrichment of Cu and Si at this boundary.
Correlating Grain Boundary Character and Composition in 3‐Dimensions Using 4D‐Scanning Precession Electron Diffraction and Atom Probe Tomography

February 2025

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Advances in Microfluidic Paper‐Based Analytical Devices (µPADs): Design, Fabrication, and Applications

May 2024

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378 Reads

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11 Citations

Aims and scope


Small Methods focuses on significant advances in any and all methods applicable to nano- and microscale research from all areas of chemistry, physical and materials science, biomedical and life sciences featuring cutting-edge technical and methodological developments.
The Small titles from Wiley serve as high impact forums for nano and microscale research across all scientific disciplines, ensuring that we are all best equipped to understand the foundations and fundamental pieces of our everyday lives.

Recent articles


Schematics of next‐generation sequencing‐based spatial transcriptomics. a) Array‐based and bead‐based spatial transcriptomics using arrayed probes on the glass slide or beads to capture mRNA. b) DNA nanoball‐based and polony‐based spatial transcriptomics. Reproduced with permission.[²¹] Copyright 2021, Elsevier. c) Microfluidic‐based spatial transcriptomics by in situ ligation of the spatial barcodes. d) LCM‐based and light activation‐based spatial transcriptomics in a direct way to choose the region of interest.
Schematics of image‐based spatial transcriptomics. a) ISH‐based spatial transcriptomics capture target RNA via in situ hybridization. b) ISS‐based spatial transcriptomics capture transcripts information through rolling cycle amplification and in situ sequencing.
Schematics of spatial omics technologies beyond transcriptomics. a) MS‐based and antibody‐based spatial proteomics using antibody‐conjugated metal isotopes, fluorophores and DNA splints. b) Spatial genomics focusing on chromatin tracing using imaging‐based techniques. c) Spatial epigenomics, chromatin accessibility, and histone modifications mapped using the protein A‐Tn5 transposase for the ligation of barcodes or adapters. d) Spatial metabolomics using ion beams, laser beams, or electrospray droplets to perform mass spectrometry imaging analysis of pre‐treated samples.
Applications of spatial omics in neurobiology, developmental biology, and cancer biology. a) Brain atlas in regular states or in neurological diseases mapped by spatial omics technologies. b) Spatial neural connecting pattern and neural projection mapping. Reproduced with permission.[¹⁵⁴] Copyright 2019, Elsevier. c) Spatial atlas of early embryogenesis and organogenesis. d) Spatial tumor heterogeneity and complexity of tumor microenvironment resolved by spatial multi‐omics.
Advances in Spatial Omics Technologies
  • Literature Review
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March 2025

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5 Reads

Tianxiao Hui

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Jian Zhou

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Muchen Yao

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Hu Zeng

Rapidly developing spatial omics technologies provide us with new approaches to deeply understanding the diversity and functions of cell types within organisms. Unlike traditional approaches, spatial omics technologies enable researchers to dissect the complex relationships between tissue structure and function at the cellular or even subcellular level. The application of spatial omics technologies provides new perspectives on key biological processes such as nervous system development, organ development, and tumor microenvironment. This review focuses on the advancements and strategies of spatial omics technologies, summarizes their applications in biomedical research, and highlights the power of spatial omics technologies in advancing the understanding of life sciences related to development and disease.


Emerging Liquid‐Based Memristive Devices for Neuromorphic Computation

Qinyang Fan

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Jianyu Shang

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Xiaoxuan Yuan

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Jingjie Sha

To mimic the neural functions of the human brain, developing hardware with natural similarities to the human nervous system is crucial for realizing neuromorphic computing architectures. Owing to their capability to emulate artificial neurons and synapses, memristors are widely regarded as a leading candidate for achieving neuromorphic computing. However, most current memristor devices are solid‐state. In contrast, biological nervous systems operate within an aqueous environment, and the human brain accomplishes intelligent behaviors such as information generation, transmission, and memory by regulating ion transport in neuronal cells. To achieve computing systems that are more analogous to biological systems and more energy‐efficient, memristor devices based on liquid environments are developed. In contrast to traditional solid‐state memristors, liquid‐based memristors possess advantages such as anti‐interference, low energy consumption, and low heat generation. Simultaneously, they demonstrate excellent biocompatibility, rendering them an ideal option for the next generation of artificial intelligence systems. Numerous experimental demonstrations of liquid‐based memristors are reported, showcasing their unique memristive properties and novel neuromorphic functionalities. This review focuses on the recent developments in liquid‐based memristors, discussing their operating mechanisms, structures, and functional characteristics. Additionally, the potential applications and development directions of liquid‐based memristors in neuromorphic computing systems are proposed.


Advanced Characterization of Perovskite Thin Films for Solar Cell Applications Using Time‐Resolved Microwave Photoconductivity and Time‐Resolved Photoluminescence

March 2025

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1 Read

Emmanuel V. Péan

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Jiashang Zhao

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Alexander J. Doolin

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Thanks to their direct band‐gap, high absorption coefficient, low manufacturing cost, and relative abundance of component materials, perovskite materials are strong candidates for the next generation of photovoltaic devices. However, their complex photochemistry and photophysics are hindering their development. This is due, in part, to the complex charge carrier recombination pathways in these materials, as well as their instability during measurements. Here, a new characterization methodology is detailed that allows the measurement, with high certainty, of the intrinsic parameters of a single perovskite sample, such as the trap state concentration and carrier mobilities. This methodology is based on a combination of time‐resolved microwave photoconductivity (TRMC) and time‐resolved photoluminescence (TRPL) spectroscopy. Compared to TRPL only, this methodology is faster, does not lead to significant changes in the perovskite properties over time, and increases the certainty of the parameters retrieved. Using this methodology, green solvent systems are studied to replace the traditional harmful solvents usually used when spin–coating perovskites. Although devices made using the greener solvents presented lower efficiencies, TRMC and TRPL measurements highlighted that the perovskites made with these solvents can achieve the same performance compared to the traditional solvent system.


Synthesis and structure of MCZCB scintillator films. a) Illustration of the doping process of Cs2ZrCl6‐based scintillators. b) Schematic of the MSVD process for preparing CZC, CZCB, and MCZCB scintillator films. c) Transparent CZC‐based scintillator films with fluorescence images d) XRD patterns of MCZCB(x%MABr) (x = 3–12). e) SEM image and EDS‐mapping of MCZCB scintillator film.
Luminescence, scintillation properties and structural distortion of MCZCB(x%MABr) (x = 3–12). a) PL spectra. b) Luminescence decay lifetime. c) Examination of the distortion caused in the [ZrCl5Br]²⁻ octahedra by the introduction of the organic large molecule MABr, with a calculated distortion index of 0.02. d) A comparison of Br 3d XPS peaks for CZC and MCZCB. e) Temperature dependence of FWHM (dots) with fitting (line) of MCZCB(6%MABr). f) RL spectra.
A comparison in theoretical modeling for MCZCB and CZC. a,b) The CBM and VBM of MCZCB and CZC. c,d) The band structure of MCZCB with a direct bandgap of 3.38 eV and pristine CZC with an indirect bandgap of 3.71 eV. e,f) The DOS of MCZCB and CZC.
X‐ray imaging performance of MCZCB scintillator films. a) X‐ray images of a standard resolution card. b) Contrast curve. c) Image of a 100 cm² scintillator film produced through MSVD. d) X‐ray imaging of electronic components. e) Visual information analysis of scintillator film. f) X‐ray imaging of a mobile phone and mouse. The scale bar represents 2 cm.
Composition Modulation of Cs2ZrCl6‐based Scintillator Film via Vapor Deposition for Large‐Area X‐Ray Imaging

Metal halide scintillators for X‐ray imaging have shown remarkable potential, however, achieving large‐area film has been hindered by challenges in materials design and fabrication methods, particularly regarding composition uniformity for high‐resolution imaging applications. Here, a multi‐source vapor deposition (MSVD) method is employed to realize the facile composition modulation by designing MA⁺ and Br⁻ (MA⁺ = methylammonium) co‐doped Cs2ZrCl6 (MCZCB) and further synthesizing a uniform and large‐area scintillator film. The incorporation of MA⁺ and Br⁻ ions, with their slightly larger ionic radius, induces lattice distortion, enhancing the self‐trapped excitons (STEs) luminescence of the MCZCB and significantly boosting the photoluminescence quantum yield (PLQY) from 70% in pristine Cs2ZrCl6 (CZC) to an impressive 95%. Finally, a large‐area of 100 cm² and 95% visible light transparent scintillator film is fabricated, achieving a spatial resolution of 25.1 lp mm⁻¹. This result demonstrates that MSVD technology is promising as a practical strategy for fabricating large‐area X‐ray imaging film.


Development of Electrostatic Dual‐Carbon‐Fiber Microgrippers for Precise 2D Patterning and 3D Stacking of Single Microparticles

This study presents the development of electrostatic dual‐carbon‐fiber (CF) microgrippers for the precise manipulation of single SiO2 microparticles (diameters >3 µm) at low operating voltages of 5 to 15 V. Theoretical calculations and finite element analysis (FEA) simulations demonstrate that the microgrippers utilize a non‐uniform electric field generated by dual CF electrodes to create a dielectrophoresis force for the pick‐and‐place manipulation of microparticle. After the removal of dielectrophoresis force by turning off the voltage, particle release is facilitated by van der Waals forces from the substrate surface. This approach eliminates the need for additional corona discharge fields or vibrational separators for particle release, ensuring accurate 2D patterning and 3D stacking of SiO2 microparticles. The microgrippers show significant potential for applications in the individual separation and assembly of microparticles, such as lunar soil and interstellar dust, as well as single‐cell extraction and positioning. Additionally, the developed microgrippers offer broad utility in micro/nano‐manufacturing, micro/nano‐electronic circuits, physics, chemistry, and biomedicine.


hSRS imaging of GEVI‐expressing cells. A–E) SRS images at 2913, 1652, 1595, and 1525 cm⁻¹, along with TPEF images of wildtype (WT), Ace2N, Arclight, ASAP3 and Archon‐expressing HEK293T cells with or without retinal supplement. F–J) Normalized SRS spectra extracted from regions of interest (ROI) indicated by yellow dashed line in (A–E). The characteristic peaks are labeled and highlighted. The red arrow indicating peak shift. K,L) Ratio and correlation analysis of SRS signal intensity at 1525 cm⁻¹ and fluorescence intensity in 15 ROIs indicated in the GFP image of Archon‐retinal group. Scale bar: 10 µm.
Induced transmembrane voltage (∆Ψ) mapping of Archon‐expressing HEK293T cells under ITV stimulation. A) Simulation of intracellular ∆Ψ distribution of induced by ITV stimulation, with red and blue indicating depolarization and hyperpolarization, respectively. B) Plot of ∆Ψ values under ITV stimulation measured at voxels corresponding to the depolarization and hyperpolarization regions of the cell. C) Representative color mapping of percentage change in fluorescence signals of Archon in HEK293T cells upon ITV stimulation (7 continuous square pulses at 2 Hz with 40 V amplitude, 50 ms duration, 50 V/cm DC electric field density). D) Fluorescence image of HEK293T cells expressing Archon with ROIs indicated. E) Fluorescence time traces from ROIs indicated in (D). F) Zoomed‐in view of a fluorescence intensity trace from a single ITV stimulation as indicated in (E). G) ∆Ψ distribution and corresponding percentage change mapping images of fluorescence signals obtained from five time points (t0‐t4). Scale bar: 10 µm.
SRS intensity change in Archon‐expressing HEK293T cells under ITV stimulation. A) Fluorescence image of HEK293T cells. B) SRS image at 1525 cm⁻¹ during ITV stimulation. Dashed line indicates the scanning trace. Scale bar: 10 µm. C) Time‐series image along the scanning trace shown in (B). D) Percentage change in SRS intensity time traces at 1525 cm⁻¹ from the ROIs indicated in (C). E) Overlay of seven peaks from blue trace in (D). F) Comparison of trial‐averaged and single‐trial SRS traces. G) Plot of percentage change in SRS intensity at 1525 cm⁻¹ as a function of the number of trial averages. H) Plot of signal‐to‐noise ratio as a function of the number of trial averages.
Experimental workflow diagram. A) Transfection of GEVI plasmids (Archon, Ace2N, Arclight or ASAP3) into HEK293T cells. B) GEVIs expressed on the cell membrane. C) Exogenously added retinal bound to GEVIs to form Schiff base. D) Screening for a suitable GEVI for spectroscopic imaging. E) Synchronization of ITV setup and multimodal imaging system. F) Hyperspectral SRS image stacks of standard samples and GEVI‐expressing HEK293T cells in fingerprint window.
Screening of Vibrational Spectroscopic Voltage Indicator by Stimulated Raman Scattering Microscopy

Genetically encoded voltage indicators (GEVIs) have significantly advanced voltage imaging, offering spatial details at cellular and subcellular levels not easily accessible with electrophysiology. In addition to fluorescence imaging, certain chemical bond vibrations are sensitive to membrane potential changes, presenting an alternative imaging strategy; however, challenges in signal sensitivity and membrane specificity highlight the need to develop vibrational spectroscopic GEVIs (vGEVIs) in mammalian cells. To address this need, a vGEVI screening approach is developed that employs hyperspectral stimulated Raman scattering (hSRS) imaging synchronized with an induced transmembrane voltage (ITV) stimulation, revealing unique spectroscopic signatures of sensors expressed on membranes. Specifically, by screening various rhodopsin‐based voltage sensors in live mammalian cells, a characteristic peak associated with retinal bound to the sensor is identified in one of the GEVIs, Archon, which exhibited a 70 cm⁻¹ red shift relative to the membrane‐bound retinal. Notably, this peak is responsive to changes in membrane potential. Overall, hSRS‐ITV presents a promising platform for screening vGEVIs, paving the way for advancements in vibrational spectroscopic voltage imaging.


Characterization of perovskite precursor solutions. DLS results for a) NMP‐based and b) DMPU‐based perovskite precursor solution. c) Photograph of the NMP and DMPU solution containing 0.1 g mL⁻¹ PbI2. d) Binding energies of different solvent‐PbI2 coordination adduct from theoretical calculations. FTIR spectra of e) NMP‐PbI2 and f) DMPU‐PbI2 coordination complexes.
In situ PL analysis of nucleation. In situ PL spectra during gas quenching for a) NMP‐based and d) DMPU‐based films. b,e) Temporal evolution of PL intensity and peak position during initial nucleation. c,f) Full‐stage analysis of PL intensity and peak position. g) Schematic of the impact of NMP and DMPU on the growth of perovskite nanocrystals and the morphology of perovskite films.
Solvent effects on crystallization kinetics. In situ PL spectra during thermal annealing for a) NMP‐based and d) DMPU‐based films. b) Absorption intensity of perovskite film at 550 nm versus annealing time. c) TG curves of blade‐coated wet perovskite films without MACl. e) Schematic of N2 knife‐assisted blade‐coating for NMP‐based and DMPU‐based perovskite films. f,g) XRD pattern of unannealed perovskite films prepared by using different solvents. h) XRD pattern of annealed perovskite films.
Defect characterization of perovskite films. a) Steady‐state PL spectra and b) TRPL decay curves measured on glass substrates. c) J–V curves of the hole‐only devices measured under dark conditions. Inset: structure of the hole‐only device. d) Dark J–V curves and e) EIS curves of complete perovskite solar cells. f) XPS Pb 4f core‐level spectra of perovskite films.
Photovoltaic performance of devices. a) Schematic device architecture of the inverted p–i–n PSCs. b) J–V curves of NMP‐based and DMPU‐based champion p–i–n PSCs with an aperture area of 0.08 cm².c) EQE spectra and integrated JSC curves of the NMP‐based and DMPU‐based devices. d) Schematic of perovskite mini module interconnection of the subcells with P1, P2, P3 scribing. e) J–V curves of the mini solar module of champion PCE. f) MPP tracking of non‐encapsulated PSCs under continuous light illumination at 40 °C in N2.
Nonvolatile and Strongly Coordinating Solvent Enables Blade‐coating of Efficient FACs‐based Perovskite Solar Cells

Blade‐coating has emerges as a critical route for scalable manufacturing of perovskite solar cells. However, the N2 knife‐assisted blade‐coating process under ambient conditions typically yields inferior‐quality perovskite films due to inadequate nucleation control and disorderly rapid crystallization. To address this challenge, a novel solvent engineering strategy is developed through the substitution of N‐methyl‐2‐pyrrolidone (NMP) with 1,3‐dimethyl‐1,3‐diazinan‐2‐one (DMPU). The unique physicochemical properties of DMPU, characterized by low vapor pressure, strong coordination capability, and limited PbI2 solubility, synergistically regulate nucleation and crystallization kinetics. This enables rapid nucleation, stabilization of intermediate phases in wet films, and controlled crystal growth, ultimately producing phase‐pure perovskite films with reduced defect density. Moreover, the feasibility and superiority of the mixed solvent strategy are demonstrated. The optimized blade‐coated PSCs achieve a power conversion efficiency of 21.74% with enhanced operational stability, retaining 84% initial efficiency under continuous 1‐sun illumination for 1,000 h. This work provides new insights into solvent design for preparing blade‐coated perovskite films.


A Fluorinated Zinc‐based Metal‐Organic Framework for Efficient Separation of Butane Isomers via Pore Engineering

Separating n‐butane/iso‐butane is a challenging and energy‐intensive task in the petrochemical industry. There have been only several adsorbents reported for C4 paraffins separation while they are confronted in real‐world applications with either poor selectivity or low n‐butane uptake capacity. In this study, a fluorinated zinc‐based metal‐organic framework (MOF), Znpyc‐CF3, derived from Znpyc‐CH3 is developed, which has fluorine‐containing functional groups on the pore surface that can enhance the interaction with the linear n‐butane. Remarkably, this fluorinated porous material demonstrates both high n‐butane uptake (55.5 cm³ g⁻¹) and excellent selectivity (IAST selectivity = 187) at ambient temperature. Multicycle breakthrough experiments confirmed its practical performance for real gas mixtures. Znpyc‐CF3 exhibits outstanding stability, maintaining its structural integrity after repeated sorption cycles and dynamic breakthrough tests under both dry and highly humid conditions. The preferential adsorption mechanism of n‐butane is further elucidated through Grand Canonical Monte Carlo (GCMC) simulations and Density Functional Theory (DFT) calculations. Overall, this research presents an efficient and stable adsorbent for the separation of butane isomers.


Dielectric Integrations and Advanced Interface Engineering for 2D Field‐Effect Transistors

As silicon‐based transistors approach their physical limits, the challenge of further increasing chip integration intensifies. 2D semiconductors, with their atomically thin thickness, ultraflat surfaces, and van der Waals (vdW) integration capability, are seen as a key candidate for sub‐1 nm nodes in the post‐Moore era. However, the low dielectric integration quality, including discontinuity and substantial leakage currents due to the lack of nucleation sites during deposition, interfacial states causing serious charge scattering, uncontrolled threshold shifts, and bad uniformity from dielectric doping and damage, have become critical barriers to their real applications. This review focuses on this challenge and the possible solutions. The functions of dielectric materials in transistors and their criteria for 2D devices are first elucidated. The methods for high‐quality dielectric integration with 2D channels, such as surface pretreatment, using 2D materials with native oxides, buffer layer insertion, vdW dielectric transfer, and new dielectric materials, are then reviewed. Additionally, the dielectric integration for advanced 3D integration of 2D materials is also discussed. Finally, this paper is concluded with a comparative summary and outlook, highlighting the importance of interfacial state control, dielectric integration for 2D p‐type channels, and compatibility with silicon processes.


Responsive Microneedles for Diagnostic and Therapeutic Applications of Ocular Diseases

Traditional ophthalmic formulations are characterized by low bioavailability, short intraocular retention time, strong irritation, and failure to achieve the expected therapeutic effect due to the special physiological structure of the eye and the existence of many barriers. Microneedle drug delivery is a novel transdermal drug delivery modality. Responsive microneedles are defined as controllably releasing the drug payloads in response to physiological stimuli, including pH levels, temperature, enzymes, and reactive oxygen species (ROS), as well as external stimuli such as magnetic fields and light. In addition to inheriting the advantages of traditional microneedles, which include enhanced targeting and permeability, non‐invasiveness, and painless application, the integration with stimulus‐responsive materials enables responsive microneedles to achieve a personalized precision drug delivery process, which further increases the accuracy and efficiency of ocular treatments, making on‐demand drug delivery possible. This article systematically reviews the classification, mechanisms, and characteristics of responsive microneedles and provides a detailed introduction to their diagnostic and therapeutic applications as well as real‐time monitoring potential in ocular diseases, aiming to offer insights for the precision treatment of ocular diseases in the future.


Direct Measurement of the Local Electrocaloric Effect in 2D α‐In2Se3 by Scanning Electrocaloric Thermometry

The electrocaloric effect refers to the temperature change in a material when an electric field is applied or removed. Significant breakthroughs revealed its potential for solid‐state cooling technologies in past decades. These devices offer a sustainable alternative to traditional vapor compression refrigeration, with advantages such as compactness, silent operation, and the absence of moving parts or refrigerants. Electrocaloric effects are typically studied using indirect methods based on polarization data, which suffer from inaccuracies related to assumptions about heat capacity. Direct methods, although more precise, require device fabrication and face challenges in studying meso‐ or nanoscale systems, like 2D materials, and materials with non‐uniform polarization textures where high spatial resolution is required. In this study, a novel technique, Scanning Electrocaloric Thermometry, is introduced for characterizing the local electrocaloric effect in nanomaterials. This approach achieves high spatial resolution by locally applying electric fields and by simultaneously measuring the resulting temperature change. By employing AC excitation, the measurement sensitivity is further enhanced and the electrocaloric effect is disentangled from other heating mechanisms such as Joule heating and dielectric losses. The effectiveness of the method is demonstrated by examining electrocaloric and heat dissipation phenomena in 2D In2Se3 micrometer‐sized flakes poly(vinylidene fluoride‐trifluoroethylene) films.


Miniaturized High‐Throughput and High‐Resolution Platform for Continuous Live‐Cell Monitoring via Lens‐Free Imaging and Deep Learning

Monitoring the morphology and dynamics of both individual and collective cells is crucial for understanding the complexities of biological systems, investigating disease mechanisms, and advancing therapeutic strategies. However, traditional live‐cell workstations that rely on microscopy often face inherent trade‐offs between field of view (FOV) and resolution, making it difficult to achieve both high‐throughput and high‐resolution monitoring simultaneously. While existing lens‐free imaging technologies enable high‐throughput cell monitoring, they are often hindered by algorithmic complexity, long processing times that prevent real‐time imaging, or insufficient resolution due to large sensor pixel sizes. To overcome these limitations, here an imaging platform is presented that integrates a custom‐developed 500 nm pixel‐size, 400‐megapixel sensor with lens‐free shadow imaging technology. This platform is capable of achieving imaging at a speed of up to 40s per frame, with a large FOV of 1 cm² and an imaging signal‐to‐noise ratio (SNR) of 42 dB, enabling continuous tracking of individual and cell populations throughout their entire lifecycle. By leveraging deep learning algorithms, the system accurately analyzes cell movement trajectories, while the integration of a K‐means unsupervised clustering algorithm ensures precise evaluation of cellular activity. This platform provides an effective solution for high‐throughput live‐cell morphology monitoring and dynamic analysis.


Boosting Ion Transport Kinetics in Sulfolane‐Modified Aqueous Electrolytes for High‐Performance Zinc‐Ion Batteries with V₂C MXene Cathodes

The advancement of zinc‐ion batteries (ZIBs) is propelled by their inherent safety, cost‐effectiveness, and environmental sustainability. This study investigates the role of sulfolane (SL), a polar aprotic solvent with a high dielectric constant, as an electrolyte additive to enhance ion transport and electrochemical performance in V₂C MXene cathodes for high‐performance ZIBs. The addition of 1% SL optimizes Zn‐ion transport by increasing ionic conductivity, suppressing electrolyte decomposition, and mitigating zinc dendrite formation. Galvanostatic Intermittent Titration Technique (GITT) analysis reveals a reduction in Zn²⁺ diffusion coefficient from 1.54 × 10⁻⁷ cm²/s in 2 m ZnSO₄ to 1.07 × 10⁻⁹ cm² s⁻¹ in the SL‐modified system, indicating a more confined Zn²⁺ transport environment. Electrochemical Impedance Spectroscopy (EIS) further demonstrates a substantial decrease in activation energy from 123.78 to 65.08 kJ mol⁻¹, signifying improved charge transfer kinetics. Ex situ XRD confirms that SL stabilizes the phase transformation of V₂C to Zn₀.₂₉V₂O₅, enhancing structural integrity. The modified system achieves an impressive specific capacity of 545 mAh g⁻¹ at 0.5 A g⁻¹ and exhibits exceptional cycling stability, retaining 91% capacity over 7000 cycles at 20 A g⁻¹. These findings underscore the potential of sulfolane as a key additive for advancing V₂C MXene‐based ZIBs.


Schematic illustration of 3D‐printed EMI shielding carbon brick a) Fabrication process for PANI decorated brick; EMI shielding of b) 0D carbon (CB/PLA) c) 1D carbon (CNT/PLA) and d) PANI decorated 1D carbon.
Surface morphology; SEM image of a) CB/PLA, b) CNT/PLA, c) activated CNT/PLA, and d) PANI@CNT/PLA. e) EDX mapping area and f,h) elemental mapping of N, C and O, respectively, of PANI. Scale (a–d) = 4 µm, inset image (c,d) = 300 nm, (e,f) = 1 µm.
XPS analysis a) survey spectra of CNT/PLA and PANI@CNT/PLA; high‐resolution core level spectra of b) N 1s, c) C 1s, and d) O 1s.
EMI SE efficiency of a) CB/PLA, b) CNT/PLA, c) comparison of 3 mm bricks PLA, CB/PLA, CNT/PLA and PANI@CNT/PLA and d) sheet resistance measurement of CB/PLA, CNT/PLA and PANI@CNT/PLA.
3D‐Printed Nanocarbon Polymer Conductive Structures for Electromagnetic Interference Shielding

March 2025

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3 Reads

Electromagnetic interference (EMI) significantly affects the performance and reliability of electronic devices. Although current metallic shielding materials are effective, they have drawbacks such as high density, limited flexibility, and poor corrosion resistance that limit their wider application in modern electronics. This study investigates the EMI shielding properties of 3D‐printed conductive structures made from polylactic acid (PLA) infused with 0D carbon black (CB) and 1D carbon nanotube (CNT) fillers. This study demonstrates that CNT/PLA composites exhibit superior EMI shielding effectiveness (SE), achieving 43 dB at 10 GHz, compared to 22 dB for CB/PLA structures. Further, conductive coating of polyaniline (PANI) electrodeposition onto the CNT/PLA structures improves the SE to 54.5 dB at 10 GHz. This strategy allows fine control of PANI loading and relevant tuning of SE. Additionally, the 3D‐printed PLA‐based composites offer several advantages, including lightweight construction and enhanced corrosion resistance, positioning them as a sustainable alternative to traditional metal‐based EMI shielding materials. These findings indicate that the SE of 3D‐printed materials can be substantially improved through low‐cost and straightforward PANI electrodeposition, enabling the production of customized EMI shielding materials with enhanced performance. This novel fabrication method offers promising potential for developing advanced shielding solutions in electronic devices.


XRD and corresponding enlarged XRD patterns of CNIC, CNHC‐B and CNHC‐D a,b); EPR test results of CNIC, CNHC‐B, and CNHC‐D c); TEM, HRTEM, and EDS mapping patterns of CNHC‐D d–f); TEM and HRTEM patterns of CNHC‐B g,h); TEM and HRTEM patterns of CNIC i,j).
Atomic force microscopy images and the corresponding surface potential measured by Kelvin probe force microscopy and corresponding surface potentials of CNIC, CNHC‐B, and CNHC‐D a–c); Zeta potentials of CNIC, CNHC‐B, and CNHC‐D d); Transient photocurrent of CNIC, CNHC‐B, and CNHC‐D e); Calculated PEF intensity of CNIC, CNHC‐B, and CNHC‐D f).
TA spectra of CNIC a,b), CNHC‐B c,d) and CNHC‐D e,f); Time‐resolved PL spectroscopy g) of CNIC, CNHC‐B, and CNHC‐D; CO2 adsorption isotherms h) and TPD results i) of CNIC, CNHC‐B, and CNHC‐D.
CO2 photoreduction performances of CNIC, CNIC‐B, and CNIC‐D a–c); CH4 and CO selectivity of CNIC, CNIC‐B, and CNIC‐D d,e); Isotope‐labeled CO2 result of CNIC‐D f); In situ FTIR of CO2 photoreduction process of CNIC, CNIC‐B, and CNIC‐D g–i); Photocatalytic mechanisms induced by enhanced polarization j).
Polarization Induced by Chlorine Defect Engineering in High‐Entropy Halide Perovskite to Promote CO2 Photomethanation

The Coulomb electric field formed between positive and negative charges always restricts the generation and separation of photo‐irradiated electrons and holes, resulting in the limited CO2 photoreduction performances of catalysts. Herein, the defect engineering and high‐entropy strategies are used to regulate the crystallinity of Cs2NaInCl6 perovskite materials, thus resulting in an enhanced internal polarization electric field, which overcame the Coulomb electric field and promoting the separation process of charge carriers. Moreover, the Cs2Na{InPrSmGdTb}1Cl6 with Cl vacancies is prepared using the low‐temperature syntheses, which overcame the challenge of extremely high‐temperature requirements for high entropy alloy preparation. Compared with Cs2NaInCl6, Cs2Na{InPrSmGdTb}1Cl6 with Cl vacancies contribute to an 8fold enhanced polarization electric field, suppressing the recombination of photogenerated electrons and holes and thus achieving an enhanced CO2 photomethanation activity with improved product selectivity and structural stability. This work provides a promising strategy for designing and preparing low‐temperature synthesizing modified high‐entropy halide perovskite catalysts used in the field of solar energy conversion.


Chaotic Direct Ink Writing (ChDIW) of Hybrid Hydrogels: Implication for Fabrication of Micro‐ordered Multifunctional Cryogels

March 2025

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23 Reads

The modern era demands multifunctional materials to support advanced technologies and tackle complex environmental issues caused by these innovations. Consequently, material hybridization has garnered significant attention as a strategy to design materials with prescribed multifunctional properties. Drawing inspiration from nature, a multi‐scale material design approach is proposed to produce 3D‐shaped hybrid materials by combining chaotic flows with direct ink writing (ChDIW). This approach enables the formation of predictable multilayered filaments with tunable microscale internal architectures using just a single printhead. By assigning different nanomaterials to each layer, 3D‐printed hydrogels and cryogels with diverse functionalities, such as electrical conductivity and magnetism are successfully produced. Furthermore, control over the microscale pore morphology within each cryogel filament is achieved, resulting in a side‐by‐side dual‐pore network sharing a large interfacial area. The ChDIW is compatible with different types of hydrogels as long as the rheological features of the printing materials are well‐regulated. To showcase the potential of these multilayered cryogels, their electromagnetic interference shielding performance is evaluated, and they reveal an absorption‐dominant mechanism with an excellent absorption coefficient of 0.71. This work opens new avenues in soft matter and cryogel engineering, demonstrating how simplicity can generate complexity.


Recent Advances for Cation‐Anion Aggregates in Solid Polymer Electrolytes: Mechanism, Strategies, and Applications

Solid polymer electrolytes (SPEs) have garnered significant attention from both academic and industrial communities due to their high safety feature and high energy density in combination with lithium(Li) metal anode. Nevertheless, their practical applications remain constrained by the relatively low room‐temperature ionic conductivity and interface issues. Anion‐derived cation‐anion aggregates (AGGs), derived from high‐concentration liquid electrolytes, promote a stable solid‐electrolyte interphase layer, which have gradually propelled their application in SPEs. Meanwhile, the unique ion transport mechanism of AGGs in SPEs also helps to enhance their ionic conductivity. However, the detail mechanism and the application progress of AGGs in SPEs remain poorly understood. Here, it is begin with a concise historical review on the development of AGGs configuration, followed by discussion on the fundamental mechanisms of the ion transport in AGGs‐based SPEs. Then, focused on the recent developments, the design strategies for AGGs‐based SPEs are summarized in detail. Finally, perspectives are provided on the future developments and challenges for high‐performance AGGs‐based SPEs.


Nanoporous Graphene with Encapsulated Multicomponent Carbide as High‐Performance Binder‐Free Lithium‐Ion Battery Anodes

Metal carbides are considered attractive lithium‐ion battery (LIB) anode materials. Their potential practical application, however, still needs nanostructure optimization to further enhance the Li‐storage capacity, especially under large current densities. Herein, a nanoporous structured multi‐metal carbide is designed, which is encapsulated in a 3D free‐standing nanotubular graphene film (MnNiCoFe‐MoC@NG). This free‐standing composite anode with a high surface area not only provides more active Li⁺ storage sites but also effectively prevents the agglomeration or detachment of active material in traditional powder‐based electrodes. Moreover, the free‐standing design does not require additional binders, conductive agents, or even current collectors when used as LIB anode. As a result, the MnNiCoFe‐MoC@NG anode exhibits a high specific capacity of 1129.2 mAh g⁻¹ at 2 A g⁻¹ and maintains a stable capacity of 512.9 mAh g⁻¹ after 2900 cycles of 5 A g⁻¹, which is higher than most reported MoxC‐based anodes. Furthermore, the anode exhibits superb low‐temperature performance at both 0 and −20 °C, especially at large current densities. These properties make the free‐standing anode very promising in fast charging and low‐temperature applications.


Manipulation of Single Nanowire and its Applications

Micro/nano manipulation of single nanowire has emerged as a popular direction of study in the field of nanotechnology, with promising applications in cutting‐edge technologies such as device manufacturing, medical treatment, and nanorobotics. The synthesis of nanowires with controllable length and diameter makes them meet various micro/nano manipulation demands. As manipulation techniques have advanced, including the use of optical tweezers, electric and magnetic fields, mechanical control, and several more control methods, they have demonstrated unique advantages in different application fields. For instance, the application of micro/nano manipulation of single nanowire in device manufacturing, cell drug precision transport, and nanomotors has demonstrated their potential in device development, biomedicine, and precision manufacturing. However, application extension of single nanowire manipulation is still in its infancy. This review systematically sorts out the progress of nanowire synthesis and manipulation and discusses its current research status and prospects in various application fields. It aims to provide a comprehensive reference and guidance for future research and promote the innovative applications of nanowire manipulation technology in a wide range of fields.


Unraveling the Versatility of Carbon Black – Polylactic Acid (CB/PLA) 3D‐Printed Electrodes via Sustainable Electrochemical Activation

March 2025

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43 Reads

Commercially available conductive filaments are not designed for electrochemical applications, resulting in 3D printed electrodes with poor electrochemical behavior, restricting their implementation in energy and sensing technologies. The proper selection of an activation method can unlock their use in advanced applications. In this work, rectangular electrodes made from carbon black – polylactic acid (CB/PLA) filament are 3D printed with different layouts (grid and compact) and then activated using a highly reproducible eco‐compatible electrochemical (EC) treatment. The electrodes are characterized for their morphological, structural, and electrochemical features to obtain insights into the material properties and functionality. Furthermore, the influence of the electrode layout as well as the activation conditions are studied aiming to provide a better understanding of the mechanism driving the electrochemical behavior of the electrodes. The EC activation enhances the electrochemical performance, provides a uniform electrochemical activity in the electrode's interface and allows the manipulation of the electrochemical properties of 3D printed electrodes by adjusting the duration of the treatment. CB/PLA electrodes offer a wide stable potential window that benefits their use in water‐based electrochemical applications. Thus, their suitability for Zn‐ion batteries and electrochemical sensing is explored, followed by their application in hydroquinone determination in water samples.


Comparison data of PbSe QDs with and without PalCl treatment. a) Absorption spectrum at 170 °C b) Absorption spectrum at 210 °C c) XPS spectrum for Se 3d d) XRD patterns. e) TEM images of pristine PbSe QDs at 170 °C f) PalCl treated PbSe QDs at 170 °C g) TEM images of pristine PbSe QDs at 210 °C h) PalCl treated PbSe QDs at 210 °C.
Absorption spectra of PalCl treated PbSe QDs with varying amounts of PalCl and growth temperatures. a) PalCl 0.25 mmol added, b) PalCl 0.5 mmol added, c) PalCl 1 mmol added. Analysis data of Pb‐oleate with the addition of 0.25 mmol of PalCl.
Time‐dependent changes in the absorption spectrum of PbSe QDs. a) Pristine PbSe QDs growth at 170 °C. 0.25 mmol of PalCl treated PbSe QDs, b) growth at 170 °C, c) growth at 210 °C. d) Plot showing the changes in the absorption peaks of the three types of QDs.
a) Device structure, b) J–V curve, c) external quantum efficiency, d) spectral responsivity, and e) specific de‐tectivity of photodetectors using PbSe QDs. f) Comparison of specific detectivities of reported QD‐based PDs.
Schematic diagram of the chemical reaction mechanism occurring during the formation of Pb‐oleate with the addition of PalCl.
High‐Performance PbSe Quantum Dots with Palmitoyl Chloride and Their Application to Short‐Wavelength Infrared Photodetector Devices

Quantum dots (QDs), particularly those in the short‐wavelength infrared (SWIR) range, have garnered significant attention for their unique optical and electrical properties resulting from 3D quantum confinement. Among the various chalcogenide‐based QDs, lead chalcogenides, such as PbS and PbSe, are extensively studied for infrared photodetection applications. While PbSe QDs offer advantages over PbS, including a narrower bandgap and higher carrier mobility, they suffer from stability issues due to surface oxidation and particle aggregation. Conventional synthesis methods require additional post‐synthesis treatments for surface passivation with halides, which complicates the process. In this work, a novel synthesis approach that incorporates palmitoyl chloride (PalCl) into the traditional PbSe QD synthesis is introduced, effectively passivating the surface with Cl⁻ ions during the synthesis process. This method not only enhances the optical performance by producing a sharp exciton peak and allowing precise tuning of the absorption spectrum from 1100 to 1900 nm but also significantly improves the stability of the QDs in solution. The resulting QDs are successfully integrated into SWIR photodetectors (PDs), demonstrating exceptional specific detectivity of 1.08 × 10¹² Jones at 1460 nm. This achievement draws great potential of the proposed synthetic method for advancing infrared optoelectronic devices.


Volumetric, Microfluidic Plasmonic RT‐PCR

Decentralized molecular detection of pathogens remains an important goal for public health. Although polymerase chain reaction (PCR) remains the gold‐standard molecular detection method, thermocycling using Peltier heaters presents challenges in decentralized settings. Recent work has demonstrated plasmonic PCR, where nanomaterials on a surface or nanoparticles in solution heat upon stimulation by light, as a promising method for rapid thermocycling. Heating of a solution via nanoparticles suspended in solution has been demonstrated in PCR tubes, but not on microfluidic chips. We developed a volumetric, microfluidic plasmonic reverse transcription (RT)‐PCR method. A microfluidic chip is fabricated with an integrated thermocouple to measure internal temperature, feeding into a proportional‐integral‐derivative (PID) algorithm that modulates an infrared LED for closed‐loop control. Gold nanorods are dispersed in solution with RT‐PCR reagents. We created an instrument for plasmonic RT‐PCR using an infrared LED for heating, fan for cooling, and fluorometer for end‐point fluorescence detection. Rapid thermocycling and amplification of SARS‐CoV‐2 within 16 min (5 min for RT, 45 cycles in 11 min) is achieved. This paper demonstrates volumetric, plasmonic PCR in a microfluidic chip, using an integrated thermocouple for closed‐loop control. This work points to the promise of using microfluidics and nanomaterials to achieve rapid, compact detection of pathogens in decentralized settings.


Spectral characterization, aggregation‐caused quenching (ACQ) effect, and polarity‐sensitive property of fluorescence (FL) probes. The chemical structures and normalized absorption/FL emission spectra of a) P2, b) DiR, c) IR‐FE, and d) PN‐PEG2/PN‐C8/PN‐C18. FL intensity of e) P2, f) DiR, g) IR‐FE, and h) PN‐PEG2, PN‐C8, and PN‐C18 in THF/water binary systems as a function of the water content. The relationship between the integrated FL emission intensity of i) P2, j) DiR, k) IR‐FE, l) and PN‐PEG2/PN‐C8/PN‐C18 and solvent polarity observed in various solvents (carbon tetrachloride (CCl4), toluene, DCM, acetone, n‐butanol (n‐BuOH), acetic acid (AcOH), ethanol (EtOH), methanol (MeOH)). ET(30) represents the polarity parameter of various solvents. FL emission spectra of m) P2, n) DiR, o) IR‐FE, and p) PN‐PEG2/PN‐C8/PN‐C18 observed in different oil phases such as monoglyceride, glyceryl distearate, triglyceride, glyceryl behenate, ethyl oleate, fish oil, soybean oil, peanut oil, triglyceride, and olive oil.
Fluorescence (FL) labeling of lipid nanocarriers using various probes and their discriminative capacities. a) Schematic of preparation of fluorescently labeled nanoemulsions (NE) and solid lipid nanoparticles (SLN). b) Size distribution profiles of PN‐C18‐NE and PN‐C18‐SLN. Normalized FL intensity of PN‐C18‐NE and PN‐C18‐SLN in different simulated gastric or intestinal fluids such as c) water, d) SGF, e) FaSSGF, and f) FaSSIF. FL images and FL intensity of NE, SLN, and mixed micelles (MM) for g) P2, h) DiR, i) IR‐FE, and j) PN‐C18. Normalized FL intensity of NE, SLN, and MM for k) P2, l) DiR, m) IR‐FE, n) PN‐PEG2/PN‐C8/PN‐C18.
Correlation analysis between fluorescence (FL) and lipolysis dynamics of lipid nanocarriers in in vitro lipolysis model. a) Schematic of the in vitro lipolysis and in vitro imaging processes. b) FL images of PN‐C18‐NE200 in the fasted‐ or fed‐condition medium at different times. Normalized FL intensity and total NaOH consumption versus time for c) DiR‐NE200, d) P2‐NE200, and e) PN‐C18‐NE200 in the fasted condition. f) Linear regression of normalized FL intensity as a function of total NaOH consumption for DiR‐NE200, P2‐NE200, and PN‐C18‐NE200 in the fasted condition. Normalized FL intensity and total NaOH consumption versus time for g) DiR‐NE200, h) P2‐NE200, and i) PN‐C18‐NE200 in the fed‐condition. j) Linear regression of normalized FL intensity as a function of residual NaOH consumption for DiR‐NE200, P2‐NE200, and PN‐C18‐NE200 in the fed condition. k) Normalized FL intensity or l) total NaOH consumption versus time for DiR‐SLN200, P2‐SLN200, and PN‐C18‐SLN200 in the fasted condition. m) Normalized FL intensity versus time for DiR‐SLN800, P2‐SLN800, and PN‐C18‐SLN800 in the fasted condition. n,o) Linear regression of normalized FL intensity as a function of residual NaOH consumption of PN‐C18‐SLN200 and PN‐C18‐SLN800 in the n) fasted‐state and o) fed‐state. Bars are presented as mean ± SD (n = 3). The smaller the p‐value, the more significant the correlation results. p < 0.05 for the correlation indicates statistical significance. One‐way ANOVA was used to evaluate the statistical significance.
Anti‐scattering capability and in vivo tracking of various fluorescently labeled lipid nanocarriers. a) Schematic of tissue phantom study to elucidate the scattering and penetration effects. Fluorescence (FL) images b) of probe‐filled capillaries at different penetration depths and c) representative full‐width‐at‐half‐maximum (FWHM) values for different probes at 0, 1, 2, 3, 4, and 5 mm depths. One‐way ANOVA, **** P < 0.0001. Bars are presented as mean ± SD (n = 3). d) Schematic of nanoemulsions (NE) translocation in vivo. e) Images of in vivo lipolysis in ICR mice after gavage administration of DiR‐NE200, P2‐NE200, and PN‐C18‐NE200. Normalized FL intensity for different regions of interest following treatment with f) DiR‐NE200, g) P2‐NE200, and h) PN‐C18‐NE200. Bars are presented as mean ± SD (n = 3).
Tracking In Vivo Lipolysis of Lipid Nanocarriers Using NIR‐II Polarity‐Sensitive Fluorescent Probes

Elucidating in vivo lipolysis is crucial for clarifying the underlying mechanisms and in vivo fates of lipid‐based nanocarriers, which are essential oral drug delivery carriers. Current mainstream methodologies use various in vitro digestion models to predict the in vivo performance of lipid formulations; however, their accuracy is often impeded by the complicated environment of the gastrointestinal tract. Although fluorescence labeling with conventional probes partly reveals the in vivo translocation of lipid nanocarriers, it fails to elucidate the lipolysis process because of poor signal discrimination among nanocarriers, free probes, and mixed micelles (lipolysis end‐products). Here, a polarity‐sensitive probe (PN‐C18) with aggregation‐caused quenching properties for labeling lipid nanocarriers is developed and optimized. PN‐C18 successfully eliminates interference from both free probes and mixed micelles during lipolysis. In a representative in vitro lipolysis model, PN‐C18 labeling shows stronger correlation between fluorescence intensity and lipolysis progression than those of previous methods. In vivo, the translocation and lipolysis of lipid nanoparticles are clearly visualized and effectively monitored, owing to the high tissue‐penetrating capability of PN‐C18 NIR‐II photons. This study provides practical means for elucidating the in vivo fate of lipid‐based drug delivery systems and offers valuable insights and reference for further studies in this domain.


Double‐Angling‐Subspace Enabled Laser‐Induced Fluorescence Method for Determining the Types and Mass Ratio of Marine Microplastics

Currently, the laser‐induced fluorescence method faces challenges in reliably determining the types and mass ratios of marine microplastics due to overlapped fluorescence spectra of different microplastics. To address this issue, this paper proposes a double‐angling‐subspace (DAS) method to differentiate the overlapped fluorescence spectra. The key idea is to span subspaces with vectors converted by known fluorescence spectra, followed by calculating the angle between vectors and subspaces. Specifically, it is found that the angle between the vectors converted from fluorescence spectra of unknown microplastics and their projections on the subspaces, as well as the angle between these vectors and the vectors spanning the subspaces, is indicative of microplastic types. The vector of an unknown microplastic belongs to the subspace spanned by the vectors converted by the known microplastics, and the mass ratios of unknown samples can be determined by analyzing the linear correlation between the vectors of both unknown and known microplastics. The reliability of the proposed DAS method is validated with real marine microplastic samples.


Harnessing Lithiophilic Hetero‐Interfacial Chemistry for Stable Lithium Metal Batteries with Low Negative/Positive Capacity Ratios

Lithium (Li) metal batteries hold great promise for next‐generation energy storage due to their high energy density. However, their application is hindered by uncontrollable Li plating/stripping, leading to limited cycle life, especially under practical conditions with a low negative/positive (N/P) capacity ratio. Here, it is demonstrated that stable cycling of low N/P ratio Li metal batteries can be realized by harnessing hetero‐interfacial redox chemistry to regulate Li nucleation and deposition behavior. It is shown that replacing pure Li metal with intercalated Li in graphite facilitates the formation of an increasingly lithiophilic heterointerface upon discharge, which homogenizes Li deposition during subsequent charge, resulting in highly reversible Li plating/stripping with minimal active Li loss under lean Li conditions. This enables Li metal cells with a Li/graphite hybrid anode to demonstrate remarkable improvements in cycling life, even with an N/P ratio as low as 0.4, compared to those with a pure Li metal anode. This strategy provides new insights into the role of hetero‐interfacial chemistry in constructing highly reversible composite anodes for high‐energy and long‐cycling Li metal batteries.


Journal metrics


10.7 (2023)

Journal Impact Factor™


37%

Acceptance rate


17.4 (2023)

CiteScore™


19 days

Submission to first decision


$4,420 / £3,000 / €3,690

Article processing charge

Editors