Applied Physics Reviews

Applied Physics Reviews

Published by AIP Publishing

Online ISSN: 1931-9401

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Overview of single-photon sources (SPSs): concepts, mechanisms, and characteristics. (a) SPSs emit discrete photon signals under external pump excitation. Mechanisms include: (b) linear photons from spontaneous emission (SE) and (d) nonlinear photons from spontaneous parametric downconversion (SPDC). SE benefits from (c) cavity-enhanced emission rates (Purcell effect) and improved purity (antibunching), while SPDC utilizes (e) Heralding. (f) Key figures of merit (FoMs): brightness, indistinguishability, and purity.
3D FoM map across various single-photon sources (SPSs). (a) At cryogenic temperature.47,56–73 (b) At room temperature.73–90 Additional representative works featuring only one or two FoMs are presented in Appendix (Tables I–III).
Brightness enhancement of color centers based SPSs at room temperature. (a) Single NV center coupled to a plasmonic nanopatch. Reproduced with permission from Bogdanov et al., Nano Lett. 18, 4837–4844 (2018). Copyright 2018 the American Chemical Society.⁸⁶ (b) SiV centers coupled with a plasmonic nanodisk array. Reproduced with permission from Boyce et al., Nano Lett. 24, 3575–3580 (2024). Copyright 2024 Authors, licensed under a Creative Commons Attribution (CC BY NC ND 4.0) license.⁹⁴ (c) Single NV center placed on a photonic crystal nanobeam cavity. Reproduced with permission from Fehler et al., ACS Nano 13, 6891–6898 (2019). Copyright 2019 the American Chemical Society.⁹⁵ (d) NV centers in diamond parabolic reflectors. Reproduced with permission from Wan et al., Nano Lett. 18, 2787–2793 (2018). Copyright 2018 the American Chemical Society.⁸⁸ (e) Single GeV center enhanced by a plasmonic waveguide. Reproduced with permission from Siampour et al., Light 7, 61 (2018). Copyright 2018 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.⁹⁶ (f) Single GeV center embedded in a plasmonic circular grating. Reproduced with permission from Kumar et al., J. Chem. Phys. 154, 044303 (2021). Copyright 2021 AIP Publishing.⁹⁷
Brightness and indistinguishability enhancement of semiconductor (or perovskite) QDs-based SPSs at cryogenic (or room) temperature. (a) QDs coupled to a DBR microcavity to enhance the brightness of polarized photons at 4 K. Reproduced with permission from Ding et al., arXiv:2311.08347 (2023). Copyright 2023 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.¹⁰⁹ (b) Quantum computing platform based on the SPS enhanced by phonon-assisted excitation with the DBR microcavity, working at 5 K. Reproduced with permission from Maring et al., Nat. Photonics 18, 603 609 (2024). Copyright 2024 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.² (c) Bright polarized photon pair emission in a circular grating at 3.2 K. Reproduced with permission from Liu et al., Nat. Nanotechnol. 14, 586–593 (2019).⁶⁰ Copyright 2019 Springer Nature. (d) Bright polarized photon emission at the telecom C-band using an elliptical Bragg grating at 4 K. Reproduced with permission from Ge et al., Nano Lett. 24, 1746–1752 (2024). Copyright 2024 the American Chemical Society.¹¹⁰ (e) A gold nanorod connecting a colloidal QD and optical nanofiber to reduce emission time at room temperature. Reproduced with permission from Sugawara et al., Phys. Rev. Res. 4, 043146 (2022). Copyright 2022 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.¹¹¹ (f) Speeding up the emission time of a colloidal QD using a silver nanobowtie at room temperature. Reproduced with permission from Gupta et al., Nat. Commun. 12, 1310 (2021). Copyright 2021 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.¹¹² (g) Spectral linewidth of a perovskite QD confined by a DBR microcavity to enhance indistinguishability at room temperature. Reproduced with permission Farrow et al., Nano Lett. 23, 10667–10673 (2023). Copyright 2023 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.¹¹³ (h) Brightness of a perovskite QD improved by a circular Bragg grating at 3.8 K. Reproduced with permission Jun et al., ACS Nano, 18, 1396–1403 (2023). Copyright 2023 Authors, licensed under a Creative Commons Attribution (CC BY NC ND 4.0) license.¹¹⁴
Performance enhancement of 2D materials and CNTs-based SPSs at three FoMs. (a) Defect and strain engineering in WSe2 via electron beam irradiation and a nanopillar array to enhance purity. Reproduced with permission from Parto et al., Nat. Commun. 12, 3585 (2021). Copyright 2021 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.¹⁵² (b) Strain engineering determining the emission site in electric-driven WSe2. Reproduced with permission from So et al., Sci. Adv. 7, eabj3176 (2021). Copyright 2021 Authors, licensed under a Creative Commons Attribution (CC BY NC 4.0) license.¹⁵³ (c) Monolayer WSe2 coupled to gold nanocube-on-mirror, obtaining the highest indistinguishability currently recorded. Reproduced with permission from Guo et al., Nat. Nanotechnol. 13, 1137–1142 (2018). Copyright 2018 Springer Nature.⁶⁹ (d) Monolayer WSe2 coupled to gold nanogap array, achieving the near unity extraction efficiency by electric-driven gating. Reproduced with permission from Cai et al., Nat. Photonics 1–6 (2024). Copyright 2024 Springer Nature.¹⁵⁴ (e) High brightness achieved by a monolayer WSe2 with a DBR microcavity. Reproduced with permission from Drawer et al., Nano Lett. 23, 8683–8689 (2023). Copyright 2023 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.⁷⁰ (f) Brightness enhancement by coupling an hBN to a microring resonator at room temperature. Reproduced with permission from Parto et al., Nano Lett. 22, 9748–9756 (2022). Copyright 2022 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.⁷⁸ (g) Brightness enhancement by coupling an hBN to a plasmonic nanodimer at room temperature. Reproduced with permission from Nguyen et al., Nanoscale 10, 2267–2274 (2018). Copyright 2018 The Royal Society of Chemistry.⁷⁷ (h) High purity and indistinguishability achieved by a CNT coupled to a nanocube on a mirror. Reproduced with permission from Nano Letters 19, 9037–9044 (2019).⁷³ Copyright 2019 the American Chemical Society. (i) The measured indistinguishability of a CNT with a DBR microcavity at room temperature. Reproduced with permission from Husel et al., Nat. Commun. 15, 3989 (2024). Copyright 2024 Authors, licensed under a Creative Commons Attribution (CC BY 4.0) license.⁷⁵

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Single-photon generation and manipulation in quantum nanophotonics

January 2025

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504 Reads

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Wenjie Zhou

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174 reads in the past 30 days

Diffractive deep neural networks: Theories, optimization, and applications

June 2024

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1,110 Reads

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8 Citations

Optical neural networks (ONN) are experiencing a renaissance, driven by the transformative impact of artificial intelligence, as arithmetic pressures are progressively increasing the demand for optical computation. Diffractive deep neural networks (D²NN) are the important subclass of ONN, providing a novel architecture for computation with trained diffractive layers. Given that D²NN directly process light waves, they inherently parallelize multiple tasks and reduce data processing latency, positioning them as a promising technology for future optical computing applications. This paper begins with a brief review of the evolution of ONN and a concept of D²NN, followed by a detailed discussion of the theoretical foundations, model optimizations, and application scenarios of D²NN. Furthermore, by analyzing current application scenarios and technical limitations, this paper provides an evidence-based prediction of the future trajectory of D²NN and outlines a roadmap of research and development efforts to unlock its full potential.

Aims and scope


Applied Physics Reviews features significant research and reviews covering all areas of applied physics. The journal’s focus is on experimental and theoretical research alongside the application of physics to other branches of science and engineering. Review articles published in the journal provide in-depth coverage of new and emerging areas of interest to researchers interested in the physical sciences.

Recent articles


Model and evolution law of Q factors of FP-BICs. (a) Schematic of the interlayer-coupled resonator model. The realization of FP-BICs relies on the coupling between an upper resonator and its perfectly mirrored counterpart. (b) The theoretical evolution law and numerical result of Q factors of FP-BICs vs phase/frequency detuning. (c) Directional engineering of FP-BIC resonances in the vicinity of the resonant frequency by selecting suitable parameter (α, γ0). (d) The theoretical evolution law and numerical result of Q factors of FP-BICs vs nonradiative decay rate. ω0 was set to 100 1/s and γ0 to 10 1/s to calculate the scatter diagram.
Construction of a meta-platform for the demonstration of the FP-BICs. (a) Schematic diagram of the multilayer film metasurface, composed of metasurfaces and a multilayer film separated by a spacer. (b) The reflection spectra of the metasurfaces. (c) The reflection spectra of the multilayer films, with HfO2 and SiO2 thicknesses of 58 and 78.3 nm, respectively. (d) The relationship between spacer thickness and wavelength in terms of reflectance. (e) The reflection spectra of the multilayer film metasurface with various spacer thicknesses, indicated by the circles in (d). (f) The relationship between radius and wavelength concerning reflectance, with a fixed spacer thickness of 982.2 nm.
The evolution of Q factors about phase and frequency detuning. (a) Q factors of the multilayer film metasurface with a fixed metasurface radius at quasi-FP-BICs vs phase detuning. (b) Q factors of the multilayer film metasurface with a fixed spacer thickness at quasi-FP-BICs vs frequency detuning. (c) The functional relationship between the Q factor and detuning parameter α, including phase and frequency detuning. The standard deviations obtained from the fittings are 0.997 and 0.991, respectively. (d) Taming resonances governed by FP-BICs. The pentagrams correspond to the theoretical frequencies and Q factors predicted by the temporal coupled-mode theory, while circles correspond to the frequencies and Q factors of actual multilayer film metasurfaces. The structural parameters of the multilayer film metasurfaces are shown in the supplementary material, Sec. H.
Experimental validation of the evolution of quasi-FP-BICs. (a) The spectra and photograph of the multilayer film sample. The sample exhibits high reflection (∼100%) in the 422–477 nm wavelength. (b) The multilayer film metasurfaces' experimental reflection spectra and top-view SEM images. (c) Comparison of the Q factors obtained from simulations with those measured from experiments.
Manipulation of resonances governed by Fabry–Pérot bound states in the continuum
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March 2025

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16 Reads

Xiaofeng Rao

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Tao He

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Chengfeng Li

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Xinbin Cheng

Bound states in the continuum (BICs) have emerged as research hotspots in optics and photonics, offering a new paradigm for achieving extreme field localization and enhancing light–matter interactions. Here, we establish for the first time the intrinsic evolution laws of Fabry–Pérot bound states in the continuum (FP-BICs), revealing that the Q factor is inversely proportional to the square of phase/frequency detuning and to the nonradiative decay rate, enabling directional engineering of FP-BIC resonances. We propose an all-dielectric multilayer film metasurface to create an optical resonator and its perfectly mirrored counterpart, inducing FP-BICs and validating the conclusions. We experimentally demonstrated the evolution of the Q factor with frequency detuning, achieving a maximum Q factor of 610 in the visible. Our work offers novel insights into BICs, promising to inspire exotic phenomena and applications.


Pushing Q-factor limit of guided resonances by harnessing topologically protected terahertz bound states in the continuum

March 2025

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23 Reads

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Yue Wang

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Rongbo Xie

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Xiaoguang Zhao

Controlling and enhancing light–matter coupling at subwavelength scales is an essential requirement in the realm of meta-photonics. Recently, all-dielectric metasurfaces (MSs) governed by the physics of bound states in the continuum (BICs) have emerged as a standout platform for delivering high-quality (Q) factor resonances and near-field electromagnetic hotspots. However, in the terahertz (THz) domain, experimental validation of high-Q BICs resonances with strong robustness and advanced maneuverability in such all-dielectric photonic systems remains a long-standing challenge. Here, we demonstrate a simple and feasible fabrication approach to unlock the full potential of BICs-inspired resonances within the array of silicon cross elliptical resonators. Our results suggest that the designed THz-MS can support two symmetry-protected BICs with a topological charge of ±1 and several accidental BICs with a topological charge of +1 simultaneously. By introducing small perturbations to the individual resonator, the original two symmetry-protected BICs transform into quasi-BICs that bow to the inverse-square law. Astoundingly, for larger symmetry breaking, two additional BICs can be observed in the asymmetric THz-MSs surpass typical inverse-square rule, hence presenting a supererogatory degree of freedom for tailoring BICs resonances on demand. We bear out theoretical findings by transmission experiments implemented on the fabricated samples. We observe experimentally ultrasharp dual quasi-BICs resonances with a highest measured Q factor of up to 371, a level of performance that was previously unattainable with all-dielectric THz-MS on a substrate. The results mark an important step toward enriching the family of BICs and promise exciting opportunities in the field of THz optoelectronic devices and metadevices.


Incubating advances in integrated photonics with emerging sensing and computational capabilities

March 2025

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28 Reads

As photonic technologies grow in multidimensional aspects, integrated photonics holds a unique position and continuously presents enormous possibilities for research communities. Applications include data centers, environmental monitoring, medical diagnosis, and highly compact communication components, with further possibilities continuously growing. Herein, we review state-of-the-art integrated photonic on-chip sensors that operate in the visible to mid-infrared wavelength region on various material platforms. Among the different materials, architectures, and technologies leading the way for on-chip sensors, we discuss the optical sensing principles that are commonly applied to biochemical and gas sensing. Our focus is on passive optical waveguides, including dispersion-engineered metamaterial-based structures, which are essential for enhancing the interaction between light and analytes in chip-scale sensors. We harness a diverse array of cutting-edge sensing technologies, heralding a revolutionary on-chip sensing paradigm. Our arsenal includes refractive-index-based sensing, plasmonics, and spectroscopy, which forge an unparalleled foundation for innovation and precision. Furthermore, we include a brief discussion of recent trends and computational concepts, incorporating Artificial Intelligence & Machine Learning (AI/ML) and deep learning approaches over the past few years to improve the qualitative and quantitative analysis of sensor measurements.


Erbium-doped yttrium oxide thin films grown by chemical vapor deposition for quantum technologies

The obtention of quantum-grade rare-earth-doped oxide thin films that can be integrated with optical cavities and microwave resonators is of great interest for the development of scalable quantum devices. Among the different growth methods, chemical vapor deposition (CVD) offers high flexibility and has demonstrated the ability to produce oxide films hosting rare-earth ions with narrow linewidths. However, growing epitaxial films directly on silicon is challenging by CVD due to a native amorphous oxide layer formation at the interface. In this manuscript, we investigate the CVD growth of erbium-doped yttrium oxide (Er:Y2O3) thin films on different substrates, including silicon, sapphire, quartz, or yttria stabilized zirconia (YSZ). Alternatively, growth was also attempted on an epitaxial Y2O3 template layer on Si (111) prepared by molecular beam epitaxy (MBE) in order to circumvent the issue of the amorphous interlayer. We found that the substrate impacts the film morphology and the crystalline orientations, with different textures observed for the CVD film on the MBE-oxide/Si template (111) and epitaxial growth on YSZ (001). In terms of optical properties, Er³⁺ ions exhibit visible and IR emission features that are comparable for all samples, indicating a high-quality local crystalline environment regardless of the substrate. Our approach opens interesting prospects to integrate such films into scalable devices for optical quantum technologies.


Nonlinear optics in 2D materials: From classical to quantum

Nonlinear optics has long been a cornerstone of modern photonics, enabling a wide array of technologies, from frequency conversion to the generation of ultrafast light pulses. Recent breakthroughs in two-dimensional (2D) materials have opened a frontier in this field, offering new opportunities for both classical and quantum nonlinear optics. These atomically thin materials exhibit strong light–matter interactions and large nonlinear responses, thanks to their tunable lattice symmetries, strong resonance effects, and highly engineerable band structures. In this paper, we explore the potential that 2D materials bring to nonlinear optics, covering topics from classical nonlinear optics to nonlinearities at the few-photon level. We delve into how these materials enable possibilities, such as symmetry control, phase matching, and integration into photonic circuits. The fusion of 2D materials with nonlinear optics provides insights into the fundamental behaviors of elementary excitations—such as electrons, excitons, and photons—in low-dimensional systems and has the potential to transform the landscape of next-generation photonic and quantum technologies.


STM images taken at 80 K of the Bi2Se3 surface, θSb=0.5 coverage (a–c) of Sb at RT (500  × 500 nm², +1 V, 2 nA). (a) Prior to the annealing (b) after annealing to 473 K for 30 min; (c) after annealing to 473 K for 60 min. STM images taken at 80 K, for a Sb coverage of nearly θSb=1 at RT (d–f); (d) prior to the annealing (e) after annealing to 473 K for 45 min (f) 200  × 200 nm² image (+1 V, 5 nA), after annealing at 473 K for 60 min. The labels α,β, 2  β, 3  β, or 4  β stand for 1 BL α, 1, 2, 3, or 4 BL β, respectively. The Bi2Se3 substrate is depicted in the darkest color.
Panel (a) DFT band structure for 1, 2, and 3 BL of β-antimonene on Bi2Se3 along K¯Γ¯K¯ high symmetry direction. The characteristic electronic features are marked by colored arrows. (b) ‘Transit map’ of the antimonene growth strategy. In analogy with a transit map (e.g., metro or Tube map), the colored paths are referred to as cyan (deposition line), black (annealing line), red (mixed line) and brown ( β sheet line). ARPES data along K¯Γ¯K¯ direction. Top left panel, schematics of the different antimonene phases. The insets schematically indicate the coverage and composition of the adlayers (see the text for more details). The binding energy and wave vector scale are indicated on the first panel. The data are taken at RT with photon energy of 20 eV. Darker color corresponds to higher photoemission intensity.
(a) Thermodynamic phase diagram for α and β phases of antimonene on Bi2Se3 in the presence of the Sb flux. As deposition continues, phases of higher coverage become thermodynamically accessible (dashed arrows). (b) Formation energy per atom during the annealing stage, in the absence of the gaseous reservoir. Possible phase transformations are indicated by solid arrows. (c) Schematic depiction of the deposition and annealing mechanisms.
Core level spectra for (a)–(b) Sb4d, (c) Se3d, and (d) Bi5 d5/2 relative to the bismuth selenide substrate and to the antimonene phases. The data are taken at RT with a photon energy of 75 eV. A linear background was subtracted from the spectra. Vertical bars under the Sb 4 d5/2 spectra indicate the energy position of the calculated core level shifts. (e) The calculated work functions are represented by colored bars, with longer bars indicating higher values. (f) Band alignment between 1 BL β free-standing antimonene and Bi2Se3 substrate. Label D indicates the Dirac point of the Bi2Se3 substrate.
Mastering the growth of antimonene on Bi2Se3: Strategies and insights

March 2025

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15 Reads

Antimonene, the two-dimensional phase of antimony, appears in two distinct allotropes when epitaxially grown on Bi2Se3: the puckered asymmetric washboard ( α) and buckled honeycomb ( β) bilayer structures. As-deposited antimony films exhibit varying proportions of single α and β structures. We identify the conditions necessary for ordered, pure-phase growth of single to triple β-antimonene bilayers. Additionally, we determine their electronic structure, work function, and characteristic core-level binding energies, offering an explanation for the relatively large chemical shifts observed among the different phases. This study not only establishes a protocol for achieving a single β phase of antimonene but also provides key signatures for distinguishing between the different allotropes using standard spectroscopic and microscopic techniques.


Signal enhancement and noise suppression technologies in Raman spectroscopic gas sensing

Raman spectroscopy, which enables simultaneous detection of multi-gas components, is considered a valuable tool for gas analysis. However, the weak Raman scattering effect limits its application in the field of high-sensitivity gas detection. In this article, we summarize the principles and characteristics of existing techniques for improving the detection of Raman spectra, from both the perspectives of signal enhancement and noise suppression. Regarding signal enhancement techniques, the main methods include multi-pass cavity enhancement, resonant cavity enhancement, and hollow-core fiber enhancement. As for noise suppression methods, the primary approaches include spatial filtering, shifted excitation Raman difference spectroscopy, polarized Raman spectroscopy, and internal standard correction. Finally, we present and outlook on how to further enhance the sensitivity of Raman spectroscopy based on existing techniques, which can lay the foundation for the future development of robust and easy-to-use gas analysis instruments.


Biomechanical and mechanobiological design for bioprinting functional microvasculature

Functional microvasculature is essential for in vitro tissue constructs, ensuring efficient transport of oxygen, nutrients, and waste and supporting vital paracrine signaling for tissue stability. Recent advancements in both direct and indirect 3D bioprinting offer promising solutions to construct complex vascular networks by allowing precise control over cell and extracellular matrix placement. The process from shape printing of microvasculature to function formation involves dynamic shift of bioink mechanical properties, mechanical microenvironments, and mechanobiology of endothelial and supporting cells. This review explores how biomechanical and mechanobiological principles are integrated into the bioprinting process to develop functional microvascular networks. Before printing, a top-level design approach based on these principles focuses on the interactions among biomaterials, cell behaviors, and mechanical environments to guide microvascular network fabrication. During printing, biomechanical design of bioinks for different bioprinting techniques, along with optimized biomechanical factors of bioprinting process, ensures accurate microvascular structure reproduction while maintaining cell viability. After printing, the emphasis is on creating a suitable mechanical environment to modulate the mechanobiology of multiple steps of neovascularization, including initiation, morphogenesis, lumen formation, stabilization, and maturation of functional microvasculature. Finally, we discuss future developments based on biomechanical and mechanobiological design to drive the bioprinting of functionalized microvascular networks.


Smart biomaterials in healthcare: Breakthroughs in tissue engineering, immunomodulation, patient-specific therapies, and biosensor applications

March 2025

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62 Reads

Smart biomaterials have significantly impacted human healthcare by advancing the development of medical devices designed to function within human tissue, mimicking the behavior of natural tissues. While the intelligence of biomaterials has evolved from inert to active over the past few decades, smart biomaterials take this a step further by making their surfaces or bulk respond based on interactions with surrounding tissues, imparting outcomes similar to natural tissue functions. This interaction with the surrounding tissue helps in creating stimuli-responsive biomaterials, which can be useful in tissue engineering, regenerative medicine, autonomous drug delivery, orthopedics, and much more. Traditionally, material engineering focused on refining the static properties of biomaterials to accommodate them within the body without evoking an immune response, which was a major obstacle to their unrestricted operation. This review highlights and explains various engineering approaches currently under research for developing stimuli-responsive biomaterials that tune their outcomes based on responses to bodily factors like temperature, pH, and ion concentration or external factors like magnetism, light, and conductivity. Applications in soft and hard tissue engineering, 4D printing, and scaffold design are also discussed. The advanced application of microfluidics, like organ-on-a-chip models, extensively benefits from the intrinsic smart properties of biomaterials, which are also discussed below. The review further elaborates on how smart biomaterial engineering could revolutionize biosensor applications, thereby improving patient care quality. We delineate the limitations and key challenges associated with biomaterials, providing insights into the path forward and outlining future directions for developing next-generation biomaterials that will facilitate clinical translation.


Preparation of 2D β-Ga2O3 flakes and polarization photodetector. (a) Liquid metal gallium dripped onto the (100) surface of β-Ga2O3 substrate at 65 °C. (b) Gallium droplets curing into solid sheet after being rapidly cooled down to 5 °C, and a PDMS tape pressed on the surface of the sheet. (c) Residual gallium washed away by ultrasonic treatment in 50 °C ethanol and the β-Ga2O3 flakes well preserved on Si/SiO2 substrate. (d) Photograph, optical microscopy and atomic force microscopy images of exfoliated 2D β-Ga2O3 flakes (scale bar: 2 mm, 100 μm and 2 μm). (e) 2D β-Ga2O3 polarization UV photodetector with interdigital Au electrodes prepared via EBL and TE.
Characterization of 2D anisotropic β-Ga2O3 nanoflakes. (a) Atomic distribution scenario and lattice parameters of monoclinic β-Ga2O3 unit cell. (b) Cross-sectional HR-TEM image and the SAED pattern of the exfoliated β-Ga2O3 flakes. (c) Atomic ratio of Ga:O (∼40.12:59.88) in β-Ga2O3 flakes analyzed by x-ray photoelectron spectroscopy. (d) Typical Raman spectrum of β-Ga2O3 flakes. (e) The ARPRS of Ag(3) mode with a fourfold symmetry at cross-polarized configurations. (f) Polarization-dependent optical transmission spectra of 2D β-Ga2O3 flakes.
Polarization-sensitive solar-blind detector with high anisotropy ratio. (a) Schematic representation of energy band diagram of 2D β-Ga2O3 flake along the (100) direction under bias. The arrows represent the transition selection rule from the valence band maximum (VBM) to conduction band minimum (CBM). (b) Wavelength-dependent responsivity of 2D β-Ga2O3 detector with a response-peak at 265 nm. (c) I-P curve with good linear behavior (α ≈ 0.97 and LDR = 114) under 265 nm illumination and 2 V bias. (d) Time-resolved current with fast response speed (100/78 μs for rise/decay time). (e) Dark current and polarization-dependent photocurrent with a high anisotropy ratio (∼2.8). (f) Variation of responsivity with continuously changing polarization angle adjusted by rotating the half-wave plate at 4 V bias, demonstrating a good periodicity.
Polarimeter based on amorphous Ga2O3 film and twistedly stacked 2D β-Ga2O3 flakes. (a) Schematic structure of Ga2O3 polarimeter consisting of three stacked ultrathin photodetectors. (b) Exceptional linear photoresponse behavior of amorphous Ga2O3 film on incident power density in Channel I. (c) Photocurrent in Channel I, Channel II, and Channel III under irradiation of linearly polarized light (power density: 200 mW/cm², wavelength: 265 nm) and 2 V bias. (d) 2D parameter space of the polarized photocurrent (III and IIII) collected from Channel II and Channel III under different irradiation power densities (50, 100, and 200 mW/cm²) and varying polarization angles (0–180°) of incident UV light.
Well-defined UV polarization imaging in one step. (a) System configuration of single-pixel polarization imaging system based on four twistedly-stacked 2D β-Ga2O3 photodetectors for one-step polarization imaging. The imaging target (2D mask) is a school badge (size: 10 × 10 mm²). The calculation of DoLP involves four polarized photocurrent values ( I0°, I45°, I90°, and I135°) and the first three components of the Stokes vector (S0, S1, and S2). (b) Direct photocurrent imaging of school badge from the first-layer β-Ga2O3 detector. (c) DoLP imaging in one step via the four-layer twistedly-stacked detection system. Such well-defined polarization imaging result is of a high resolution (150 × 150 pixels), well ahead of the photocurrent imaging in (b).
Liquid-metal-assisted exfoliation of 2D β-Ga2O3 with high anisotropy ratio for solar-blind detection and polarization imaging

Solar-blind UV polarization detection and imaging can reflect more detailed optical information, which is vital for developing next-generation deep UV optoelectronic devices. β-Ga2O3 with ultra-wide bandgap is an ideal candidate for solar-blind UV detection application. However, the bulky nature of Ga2O3 limits its application in miniaturized, integrated and multifunctional devices, and polarization imaging based on Ga2O3 photodetector has not yet been realized. Here, we report a convenient method to prepare 2D β-Ga2O3 flakes via liquid-metal-assisted exfoliation. Benefiting from high crystallinity and polarization-sensitive absorption of prepared ultrathin β-Ga2O3 flake in monoclinic structure, the β-Ga2O3 photodetector exhibits an ultra-fast response speed (100/78 μs for rise/decay time) and a prominent anisotropy ratio (∼2.8) of polarization photoresponse under 265 nm illumination. An unambiguous detection of linearly polarized light has also been realized by the double symmetry-breaking of twisted β-Ga2O3 photodetectors. Moreover, a four-layer twistedly stacked detection system further enables a one-step and well-defined polarization imaging with high resolution (150 × 150 pixels) to acquire spatial polarization information. This work presents a novel strategy for preparing ultrathin 2D gallium oxides and demonstrates a promising route to realize well-defined solar-blind polarization imaging in a simple manner.


Current trends in material research for nuclear batteries: Harnessing metal perovskite halides and other chalcogenides for greater compactness and efficiency

Nuclear energy emerges as a promising and environmentally friendly solution to counter the escalating levels of greenhouse gases resulting from excessive fossil fuel usage. Essential to harnessing this energy are nuclear batteries, devices designed to generate electric power by capturing the energy emitted during nuclear decay, including α or β particles and γ radiation. The allure of nuclear batteries lies in their potential for extended lifespan, high energy density, and adaptability in harsh environments where refueling or battery replacement may not be feasible. In this review, we narrow our focus to nuclear batteries utilizing non-thermal converters such as α- or β-voltaics, as well as those employing scintillation intermediates. Recent advancements in state-of-the-art direct radiation detectors and scintillators based on metal perovskite halides (MPHs) and chalcogenides (MCs) are compared to traditional detectors based on silicon and III-V materials, and scintillators based on inorganic lanthanide crystals. Notable achievements in MPH and MC detectors and scintillators, such as nano-Gy sensitivity, 100 photons/keV light yield, and radiation hardness, are highlighted. Additionally, limitations including energy conversion efficiency, power density, and shelf-life due to radiation damage in detectors and scintillators are discussed. Leveraging novel MPH and MC materials has the potential to propel nuclear batteries from their current size and power limitations to miniaturization, heightened efficiency, and increased power density. Furthermore, exploring niche applications for nuclear batteries beyond wireless sensors, low-power electronics, oil well monitoring, and medical fields presents enticing opportunities for future research and development.


Ionic conduction and interfacial stability in Na1+xZr2SixP3−xO12 solid electrolytes: Past, present, and future perspectives

While the development of new solid electrolytes (SEs) is crucial for advancing energy storage technologies, revisiting existing materials with significantly improved knowledge of their physical properties and synthesis control offers significant opportunities for breakthroughs. Na1+xZr2SixP3−xO12 (NaSICON) SEs have recently regained attention for applications in both solid-state and aqueous redox flow batteries due to their improved electrochemical and mechanical properties, along with their inherent electrochemical stability, air robustness, and low manufacturing cost. Recent improvements in NaSICON have primarily targeted macroscopic property enhancements and synthesis techniques. To enable further breakthroughs in the performance of NaSICON SEs, future efforts should focus on understanding how modified synthesis conditions influence atomic and microscopic-scale features, such as conduction channels, electronic structures, phase distributions, and grain boundaries. These features ultimately control ion conductivity, mechanical properties, and electrochemical stability of NaSICON and its interfaces. Here, we review the current understanding of the structure-chemistry-property relationships of NaSICON SEs, focusing on atomic and microscopic levels. First, we introduce the proposed ionic conduction mechanisms in NaSICON crystallites. Then, we explore experimental investigations at phase and grain boundaries to assess ionic conduction and interfacial stability. We also examine strategies to address interfacial challenges such as high resistance and chemical reactions between SEs and electrodes, highlighting the difficulties in analyzing interfaces at the nano/atomic scale. Finally, we provide an outlook on advancing microscopy and spectroscopy techniques to enhance insights into NaSICON SEs ionic conduction and interfacial stability, supporting the development of improved long-duration energy storage devices.


Physics-informed learning in artificial electromagnetic materials

The advent of artificial intelligence—deep neural networks (DNNs) in particular—has transformed traditional research methods across many disciplines. DNNs are data driven systems that use large quantities of data to learn patterns that are fundamental to a process. In the realm of artificial electromagnetic materials (AEMs), a common goal is to discover the connection between the AEM's geometry and material properties to predict the resulting scattered electromagnetic fields. To achieve this goal, DNNs usually utilize computational electromagnetic simulations to act as ground truth data for the training process, and numerous successful results have been shown. Although DNNs have many demonstrated successes, they are limited by their requirement for large quantities of data and their lack of interpretability. The latter results because DNNs are black-box models, and therefore, it is unknown how or why they work. A promising approach which may help to mitigate the aforementioned limitations is to use physics to guide the development and operation of DNNs. Indeed, this physics-informed learning (PHIL) approach has seen rapid development in the last few years with some success in addressing limitations of conventional DNNs. We overview the field of PHIL and discuss the benefits of incorporating knowledge into the deep learning process and introduce a taxonomy that enables us to categorize various types of approaches. We also summarize deep learning principles which are critical to PHIL understanding and the Appendix covers some of the physics of AEMs. A few specific PHIL works are highlighted and serve as examples of various approaches. Finally, we provide an outlook detailing where the field is currently and what we can expect in the future.


Multi-material additive manufacturing of energy storage and conversion devices: Recent progress and future prospects

The ever-increasing energy demand has highlighted the need for sustainable, low-carbon, and multi-functional energy solutions. Recently, multi-material additive manufacturing (MMAM) has become an emerging processing approach to prototype energy storage and conversion devices by enabling the fabrication of complex systems in a single, streamlined process while offering design freedom to customize end-product properties at precise, user-defined patterns and geometries. Moreover, it provides opportunities to fine-tune interfaces and material compositions at the microscale, opening new avenues for next-generation energy storage and conversion devices. As MMAM is still in its early stages, a comprehensive understanding of the interplay between material chemistry, processing methods, and device design is fundamental to fully realize its potential for developing high-performance energy materials. This review proposes a framework to bridge the gaps between the fundamental principles of processing physics and the practical implementation of various MMAM techniques in fabricating advanced energy storage and conversion devices, highlighting research challenges and future opportunities.


Defect-induced magnetic symmetry breaking in oxide materials

March 2025

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68 Reads

Magnetic properties of crystalline solids are fundamental to a wide range of applications, capturing the attention of a vast scientific community. Thus, engineering magnetic order in materials such as ferromagnetism and antiferromagnetism holds great scientific and technological interest. Defects such as vacancies, interstitials, and dopants induce local perturbations within the crystal lattice. These perturbations locally disturb the entire symmetry of crystals, resulting in symmetry breaking. Oxides, in particular, exhibit intriguing properties when subjected to defects, which can lead to significant modifications in their structural, electronic, and magnetic properties. Such defects in non-magnetic oxides can induce magnetic symmetry breaking, leading to the formation of emergent magnetic domains and orderings. In this review, we focus on the recent progress in magnetic breaking symmetries in materials via defect engineering and present our perspectives on how these may lead to new understanding and applications.


Magnetic characterization at room temperature and thickness-dependent FMR shift at superconducting states. (a) Frequency-dependent resonant field and the Kittel fit for the sample Nb(100 nm)/NiFe(30 nm)/Nb(100 nm) measured at 300 K. (b) Frequency-dependent FMR linewidth and the linear fit for the sample Nb(100 nm)/NiFe(30 nm)/Nb(100 nm) measured at 300 K. (c) Area magnetization as a function of the thickness of NiFe for the sample Nb(100 nm)/NiFe(t nm)/Nb(100 nm) measured at 300 K. (d) Temperature-dependent resonant field for the sample Nb(100 nm)/NiFe(t nm)/Nb(100 nm) measured at 9 GHz.
Interface effect on the shift of resonant fields at superconducting states. (a)–(e) Temperature-dependent shift values and shift ratios for the plain sample Nb(100 nm)/NiFe(30 nm)/Nb(100 nm), Pt-inserted sample, PMA-inserted sample, Gd-inserted sample, and Nb-shorted sample, respectively. The resonant field at 15 K (denoted as μ0H015 K) serves as the reference to calculate the shift value. The shift ratio is defined as the shift value divided by μ0H015 K. (f) Comparison of the shift ratios for different sample structures.
Comparison of the FMR shift between experiments and theoretical calculations. (a) Schematic of the S/F/S heterostructure for theoretical calculations. (b)–(e) Comparison for the sample Nb(100 nm)/NiFe(t nm)/Nb(100 nm) with t = 5, 10, 20, and 30 nm, respectively. (f) Fitted London penetration depth according to the theories as a function of the thickness of NiFe.
Proposal for devices leveraging ultrastrong magnon–Cooper pair couplings. (a) Negligible FMR shift for the sample Nb(100 nm)/Pt(10 nm)/NiFe(30 nm)/Pt(10 nm)/NbN(100 nm) with asymmetric structures. (b) Electrical field-induced distortions of the superconducting phase, e.g., breaking of Cooper pairs into quasiparticles. (c) Gate voltage (Vg)-controlled device to modulate FMR where the resonant field/frequency shifts with Vg on. (d) Vg-controlled device to modulate spin wave transmission with the wavelength tuned upon Vg on.
Efficient shift of ferromagnetic resonance by superconductor gating

The proximity effect has long been recognized as the primary driver of static transport behavior in superconductor/ferromagnetic heterostructures, yet the understanding of magnetic dynamics in this context remains limited. Here, we demonstrate a significant shift of ferromagnetic resonance spectra in ferromagnetic films placed between two superconductor gating layers. Through deliberate modifications of the interface structure using various insertion layers, we have determined that the superconducting proximity effect has a minimal impact on the modulation of ferromagnetic resonance characteristics. Instead, our findings strongly support very recent theoretical predictions that emphasize the phenomenon of ultrastrong coupling between Kittel magnons and Cooper pairs arising from the superconducting magnetoelectric effect. We propose that this ultrastrong coupling not only provides a precise method for determining superconducting parameters like the London penetration depth but also lays the foundation for the manipulation of spin waves through superconductors in future magnonic circuits.


Linear flip-chipped resonant-cavity green μLEDs arrays for low-crosstalk optogenetic probes with low damage

Optogenetics with high temporal and spatial resolution hold great potentials to replace the traditional drug and electrical stimulation techniques, which calls for optical probing devices with low crosstalk and organic damages. Here, we report a fabrication method of optoelectrical probes for precise modulation of neurons. A linear array of flip-chipped green resonant-cavity μLEDs (RCLED) with an emitting aperture of 50 μm is integrated on Si platform as the stimulation source. Due to the top/bottom Bragg reflectors, the RCLEDs' output light view-angle is narrowed to <90°. The emission wavelength demonstrates remarkable stability under various injection current densities. Under the 50 A/cm² driving current density, the RCLEDs' output optical density is 100 mW/mm² and maximum temperature rise is 0.5 °C, both of which exhibit great improvement compared with those of the optical probes on sapphire substrate. Using these green RCLED probes to stimulate Mac-mCherry photosensitive protein, the analgesia and inhibition effects for medium prefrontal cortex GABAergic neurons are verified. This work provides an effective approach to fabricate integrated microscale light sources for precise stimulation and modulation of neurons, which facilitate the study of complex neural functions.


Application and prospect of in situ TEM in wide bandgap semiconductor materials and devices

Wide bandgap semiconductor (WBS) materials have a wide range of applications in radio frequency and power electronics due to their many advantages such as high saturation drift velocity, breakdown voltage, and excellent thermal/chemical stability. Diamond, Ga2O3, GaN, and SiC are typical WBS materials. Reliability studies for these four materials and devices are crucial for WBS applications. Traditional means of reliability studies include, but are not limited to, x-ray diffraction, atomic force microscopy, Raman spectroscopy, and electron microscopy et al. However, most of these methods are ex situ studies after material or device failure and thus have some limitations. In situ transmission electron microscope (TEM) is a favorable technology to observe the degradation and failure process of materials and devices in real time, which may provide effective guidance in material growth, device structure design, device process optimization, and reliability improvement. In recent years, in situ TEM technology has been gradually used by researchers to study WBS materials and devices. In this review, we present a comprehensive and systematic review of in situ TEM works on diamond, Ga2O3, GaN, and SiC materials and devices, with a particular focus on the progress of the technology in the reliability study of such materials and devices. While summarizing the advantages of in situ TEM in the investigation of WBS materials and devices, the review also looks forward to the future of in situ TEM in promoting the study of WBS materials and devices.


Inorganic semiconducting nanostructures-based printed photodetectors

Optoelectronic devices, such as photodetectors (PDs), are needed in many applications including high-speed optical communications, robotics, healthcare, and biomimetic visual systems, which require detection and interaction using light. As a result, a wide variety of PDs on planar substrates have been reported using various light sensitive materials and traditional micro-/nano-fabrication technologies. In recent years, considerable efforts have been devoted to developing PDs with flexible form factors and using eco-friendly materials and approaches. These efforts have resulted in exploration of degradable materials and printed electronics as a resource-efficient route for manufacturing and to contain end-of-life issues. This paper reviews such new advances, particularly focusing on flexible PDs based on inorganic (e.g., crystalline silicon, compound semiconductors, metal oxides, etc.) semiconductor nanostructures [e.g., Nanowires (NWs), Nanoribbons (NRs), etc.]. The advantages and disadvantages of various bottom-up and top-down methods explored to realize the nanostructures and the wet (solution-processable) and dry printing and assembly methods to print the nanostructures on flexible substrates, are discussed along with their suitability for various applications. This discussion is supported by a comparative analysis of printed PDs in terms of key performance metrics such as responsivity, detectivity, ILight/IDark ratio, response speed, and external quantum efficiency. This comprehensive discussion is expected to benefit researchers and practitioners from academia and industry interested in the field of printed and flexible PDs.


Bulk nonlinear metamaterials for generation of quantum light

March 2025

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22 Reads

Quantum states of light, such as fixed photon number (Fock) states, entangled states, and squeezed states, offer important advantages with respect to classical states of light, such as coherent states and thermal states, in different areas: they enable secure communication and distribution of encryption keys, enable realization of sensors with higher sensitivity and resolution, and are considered candidates for quantum computing and simulation applications. To accommodate these applications, suitable methods for generating the quantum states are needed. Today, the quantum states are often produced by a spontaneous nonlinear process in a standard nonlinear material, followed by a series of optical elements necessary for encoding the desired state on the generated photons. In this review, we consider an alternative approach of structuring the nonlinearity of the crystal so that the desired quantum state will be generated directly at the crystal, without the need for additional elements. Our main focus here is on bulk crystals having structured second-order nonlinearity. The rising interest in these nonlinear metamaterials is fueled by advancements in the ability to efficiently simulate and design spontaneous parametric downconversion (SPDC) processes, as well as by new capabilities of structuring the nonlinearity of ferroelectric crystals, either by electric field poling or by laser-induced writing. As a result, nonlinear metamaterials were recently used to directly shape the spatial and spectral correlations of quantum light that is generated in SPDC. The paper covers the theoretical background and the design and fabrication methods of bulk nonlinear metamaterials for generating quantum light, as well as a series of demonstrations of the use of metamaterials in quantum optical applications.


Optical phonons on thermal conduction in advanced materials

The requirements for high performance, reliability, and longevity in electronic devices, such as power semiconductors and thermal sensors, make effective thermal management a formidable challenge. Thus, understanding lattice dynamics is crucial for regulating thermal conduction, as the intrinsic limit mainly depends on phonon dispersions. Conventionally, thermal conduction is regulated through heat-carrying acoustic phonon manipulation due to their high group velocities, which are widely utilized in materials such as thermal coatings and thermoelectrics. In recent years, with advancements in thermal transport, optical phonons have been of great interest for tuning thermal conduction, with a particular focus on those with special dispersive behaviors; however, the microscopic mechanisms are significantly different. This review aims to provide a comprehensive understanding of the effect of optical phonons, especially those with high weights on thermal conduction in advanced materials, as well as discuss the fundamental mechanisms, including (i) phonon bandwidth, (ii) phonon gap, (iii) avoided-crossing, (iv) phonon nesting/twinning, (v) optical-acoustic phonon bunching, and (vi) multiple optical phonons.


3D printing-based photonic waveguides, fibers, and applications

February 2025

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106 Reads

Along with the ever expanding frontiers of photonic applications as the world is fast advancing into the information era, there is a growing market for specialty photonic waveguides and fibers requiring sophisticated structures and materials that conventional manufacturing technologies meet great challenges and difficulties to accommodate. Advanced 3D printing or additive manufacturing possesses great flexibility in structure and diversity in material and is emerging as an essential alternative in developing novel specialty photonic waveguides, fibers, and devices for new photonic applications. This paper reviews 3D printing-based photonic waveguides, fibers, and their applications in terms of basic material and processing techniques, fundamental principles and mechanisms, current research and development, and remaining technical problems and challenges.


Defect physics and thermal transport properties. (a) Schematic diagram of the formation of compensating defects. (b) Temperature- and (c) doping-content-dependent lattice thermal conductivity of pristine and doped TiCoSb samples. The dashed lines in (c) represent the predicted trend of thermal conductivity variation based on the substitutional defect scattering mechanism (discussed below).
Phonon softening induced by aliovalent doping. (a) Calculated phonon dispersion for TiCoSb. (b) Phonon dispersion comparison between TiCoSb and TiCo0.75Ni0.25Sb along the same path. Inset: magnified view of the “M-Γ” path showing the avoided crossing phenomenon for the Ni-doped sample. (c) Energy-dependent calculated group velocity for TiCoSb and TiCo0.75Ni0.25Sb. (d) IpCOHP values for the bonds in TiCoSb and TiCo0.25Ni0.75Sb.
Calculated impact of aliovalent doping on anharmonicity and lattice thermal conductivity. (a) Comparison among the phonon velocity determined by first-principles calculations and the corresponding values estimated from different theoretical models. (b) Mode Grüneisen parameters for TiCoSb and TiCo0.75Ni0.25Sb. (c) Comparison of Umklapp scattering phonon relaxation time between TiCoSb and TiCo0.75Ni0.25Sb at 300 K. (d) Spectral lattice thermal conductivity κlat(ω) of TiCoSb and TiCo0.75Ni0.25Sb at 300 K.
Compensating defects in the aliovalent-doped samples and their impact on thermal conductivity. (a) Neutron powder diffraction Rietveld refinement results for TiCoSb and TiCo0.8Ni0.2Sb at 300 K. (b) Fermi-level-dependent defect formation energy in TiCoSb. The green shaded area defines the bandgap. (c) Experimental and theoretical temperature-dependent lattice thermal conductivity results for TiCoSb and TiCo0.8Ni0.2Sb. (d) Temperature-dependent theoretical lattice thermal conductivity of TiCo0.8Ni0.2Sb with consideration of different scattering mechanisms. (e) Spectral lattice thermal conductivity κlat(ω) of TiCo0.8Ni0.2Sb at 300 K with consideration of different scattering mechanisms.
Anomalous thermal transport in semiconductors induced by aliovalent doping

February 2025

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51 Reads

As an effective method for thermal management technologies, doping or substitution has been extensively utilized to reduce the lattice thermal conductivity of various materials. Intensive studies have been conducted about the phonon mechanism of isoelectronic alloying since the 1950s. Very recently, the specific role of aliovalent doping was elucidated in the half-Heusler NbFeSb system. Here, we have theoretically and experimentally investigated the mechanism of reducing thermal conductivity through aliovalent doping by combining first-principles calculations and neutron diffraction studies for the case study of the TiCoSb half-Heusler system. The softening of the acoustic branches induced by aliovalent doping can effectively reduce the phonon group velocities. Moreover, the introduction of compensating defects, resulting from changes in the Fermi level, plays a vital role in decreasing the relaxation time of phonons, as demonstrated by the analysis of neutron powder diffraction. Due to these two factors, doping with adjacent elements results in a significant reduction in lattice thermal conductivity (for instance, Ni doping at the Co site in the TiCoSb half-Heusler system), especially in the low-temperature range. Our findings provide valuable insight into the phonon scattering mechanism in aliovalent-doped materials and demonstrate the role of compensating defects in heat transport, which is applicable to other doped semiconductor systems.


Engineering THz-frequency light generation, detection, and manipulation through graphene

February 2025

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74 Reads

Graphene has been one of the most investigated materials in the last decade. Its unique optoelectronic properties have indeed raised it to an ideal and revolutionary candidate for the development of entirely novel technologies across the whole electromagnetic spectrum, from the microwaves to the x-rays, even crossing domain of intense application relevance, as terahertz (THz) frequencies. Owing to its exceptionally high tensile strength, electrical conductivity, transparency, ultra-fast carrier dynamics, nonlinear optical response to intense fields, electrical tunability, and ease of integration with semiconductor materials, graphene is a key disruptor for the engineering of generation, manipulation, and detection technologies with ad hoc properties, conceived from scratch. In this review, we elucidate the fundamental properties of graphene, with an emphasis on its transport, electronic, ultrafast and nonlinear interactions, and explore its enormous technological potential of integration with a diverse array of material platforms. We start with a concise introduction to graphene physics, followed by the most remarkable technological developments of graphene-based photodetectors, modulators, and sources in the 1–10 THz frequency range. As such, this review aims to serve as a valuable resource for a broad audience, ranging from novices to experts, who are keen to explore graphene physics for conceiving and realizing microscale and nanoscale devices and systems in the far infrared. This would allow addressing the present challenging application needs in quantum science, wireless communications, ultrafast science, plasmonics, and nanophotonics.


Wireless mechanical and hybrid thrombus fragmentation of ex vivo endovascular thrombosis model in the iliac artery

February 2025

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61 Reads

This study investigates the efficacy of an untethered magnetic robot (UMR) for wireless mechanical and hybrid blood clot removal in ex vivo tissue environments. By integrating x-ray-guided wireless manipulation with UMRs, we aim to address challenges associated with precise and controlled blood clot intervention. The untethered nature and size of these robots enhance maneuverability and accessibility within complex vascular networks, potentially improving clot removal efficiency. We explore mechanical fragmentation, chemical lysis, and hybrid dissolution techniques that combine mechanical fragmentation with chemical lysis, highlighting their potential for targeted and efficient blood clot removal. Through experimental validation using an ex vivo endovascular thrombosis model within the iliac artery of a sheep, we demonstrate direct revascularization of a 13-mm-long, 1-day-old blood clot positioned inside the left common iliac artery. This was achieved by deploying a UMR into the abdominal aorta within 15 min. Additionally, both mechanical fragmentation and hybrid dissolution achieve a greater volume rate of change compared to no intervention (control) and chemical lysis alone. Mechanical fragmentation exhibits clot removal with a median of 0.87 mm³/min and a range of 2.81 mm³/min, while the hybrid approach demonstrates slower but more consistent clot removal, with a median of 0.45 mm³/min and a range of 0.23 mm³/min.


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32 days

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