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10 pages, 863 KiB  
Article
Femtosecond Laser Fabrication of Gradient Index Micro-Optics in Chalcogenide Glass
by Thien Le Phu, Mariel Ledesma Molinero, Catherine Boussard-Plédel, David Le Coq and Pascal Masselin
Photonics 2024, 11(11), 1076; https://doi.org/10.3390/photonics11111076 (registering DOI) - 15 Nov 2024
Viewed by 191
Abstract
Gradient refractive index (GRIN) lenses have been widely used for many applications. However, the traditional manufacturing methods of GRIN lenses are very time-consuming and only suitable for macro-scale operations. In addition, those methods do not have the ability to produce other GRIN optical [...] Read more.
Gradient refractive index (GRIN) lenses have been widely used for many applications. However, the traditional manufacturing methods of GRIN lenses are very time-consuming and only suitable for macro-scale operations. In addition, those methods do not have the ability to produce other GRIN optical components with complex refractive index profiles like aspheric or freeform components. We report here an approach to produce GRIN micro-optical components in chalcogenide glass based on a direct laser writing technique. Using this approach, we are able to locally modulate the refractive index of the glass subtrates and create an arbitrary refractive index profile. To prove the flexibility of the method for the production of GRIN micro-optics, we fabricated GRIN micro-lenses and a micro-Fresnel axicon (Fraxicon). The optical properties of micro-lenses can be controlled by varying the writing parameters or the substrate thickness. As a result, the working distance of the micro-lenses can extend from 0 to more than 1000 μm. Also, the micro-Fraxicon exhibits the ability to convert a Gaussian beam to a Bessel-like beam which concentrates the mid-infrared light into an approximately 1200 μm long confinement zone. Full article
(This article belongs to the Special Issue Advances in Ultrafast Laser Science and Applications)
10 pages, 8608 KiB  
Article
Large Range Curvature Measurement Using FBGs in Two-Core Fiber with Protective Coating
by Ruibin Chen, Lutian Li, Qianqing Yu, Zhijun Luo, Zhenggang Lian, Chuanxin Teng, Hang Qu and Xuehao Hu
Micromachines 2024, 15(11), 1310; https://doi.org/10.3390/mi15111310 - 28 Oct 2024
Viewed by 498
Abstract
In this work, we propose a fiber Bragg grating (FBG)-based sensor for curvature measurements. Two gratings are inscribed through the protective coating in a specialty optical fiber using focused femtosecond laser pulses and point-by-point direct writing technology. One grating is inscribed on the [...] Read more.
In this work, we propose a fiber Bragg grating (FBG)-based sensor for curvature measurements. Two gratings are inscribed through the protective coating in a specialty optical fiber using focused femtosecond laser pulses and point-by-point direct writing technology. One grating is inscribed on the central core adjacent to an air channel, while the other is inscribed on the eccentric core. The bending characteristics of the two-core fiber strongly depend on the bending direction due to the asymmetry of the fiber cores. A bending sensitivity of 58 pm/m1 is achieved by the FBG in the eccentric fiber core over the curvature range of 0–50 m1. Temperature and humidity cross-sensitivity could be significantly reduced by analyzing the differences in peak shifts between the two gratings. The sensor features a large sensing range and good robustness due to the presence of its protective buffer coating, which makes it a good candidate for curvature sensing in engineering fields. Full article
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Figure 1
<p>(<b>a</b>) Microscopic image of the fiber cross section. (<b>b</b>) Microscopic image showing the FBGs PbP-inscribed by the femeosecond laser with a wavelength of 520 nm.</p>
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<p>Reflected spectrum of the two FBGs in the eccentric and central core of the specialty fiber.</p>
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<p>(<b>a</b>) Schematic of the experimental set-up for testing bending characteristics; (<b>b</b>) illustration of the fiber bending in 0° orientation; (<b>c</b>) illustration of four fiber orientations (0°, 90°, 180°, and 270°).</p>
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<p>(<b>a</b>) The reflected spectrum of the sensor with different curvatures, when the specialty fiber is in the 0° orientation. (<b>b</b>) The resonant wavelength dependence on the curvatures for the 0°, 90°,180° and 270° fiber orientations.</p>
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<p>(<b>a</b>) Characterization of the thermal stability of the sensor and the difference in spectral shifts of the two FBGs due to temperature variations; (<b>b</b>) Characterization of the humidity stability of the sensor and the difference in spectral shift of the two FBGs due to humidity variations.</p>
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<p>(<b>a</b>) Reflection spectra of the fiber sensor as the curvature increased from 0 to ~210 m<sup>−1</sup>, (<b>b</b>) spectral shifts of the FBGs in the central core and the eccentric core, (<b>c</b>) variations in the FWHM and the amplitude of the reflection peak.</p>
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12 pages, 4877 KiB  
Article
Bubble Printing of Liquid Metal Colloidal Particles for Conductive Patterns
by Masaru Mukai, Tatsuya Kobayashi, Mitsuki Sato, Juri Asada, Kazuhide Ueno, Taichi Furukawa and Shoji Maruo
Nanomaterials 2024, 14(20), 1665; https://doi.org/10.3390/nano14201665 - 17 Oct 2024
Viewed by 1342
Abstract
Bubble printing is a patterning method in which particles are accumulated by the convection of bubbles generated by laser focusing. It is attracting attention as a method that enables the high-speed, high-precision patterning of various micro/nanoparticles. Although the bubble printing method is used [...] Read more.
Bubble printing is a patterning method in which particles are accumulated by the convection of bubbles generated by laser focusing. It is attracting attention as a method that enables the high-speed, high-precision patterning of various micro/nanoparticles. Although the bubble printing method is used for metallic particles and organic particles, most reports have focused on the patterning of solid particles and not on the patterning of liquid particles. In this study, liquid metal wiring patterns were fabricated using a bubble printing method in which eutectic gallium‒indium alloy (EGaIn) colloidal particles (≈diameter 0.7 µm) were fixed on a glass substrate by generating microbubbles through heat generation by focusing a femtosecond laser beam on the EGaIn colloidal particles. The wiring was then made conductive by replacing gallium oxide, which served as a resistance layer on the surface of the EGaIn colloidal particles, with silver via galvanic replacement. Fine continuous lines of liquid metal colloids with a line width of 3.4 µm were drawn by reducing the laser power. Liquid metal wiring with a conductivity of ≈1.5 × 105 S/m was formed on a glass substrate. It was confirmed that the conductivity remained consistent even when the glass substrate was bent to a curvature of 0.02 m−1. Full article
(This article belongs to the Special Issue Laser-Based Nano Fabrication and Nano Lithography: Second Edition)
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<p>Working principle and optical system of bubble printing. (<b>a</b>) Working principle, (<b>b</b>) Schematic of the bubble printing system.</p>
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<p>EDX mapping analysis of EGaIn colloidal particles. (<b>a</b>) SEM image, (<b>b</b>) gallium mapping image, and (<b>c</b>) indium mapping image.</p>
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<p>Picture of (<b>a</b>) fabrication process in progress using the EGaIn colloidal particles, (<b>b</b>) SEM image and (<b>b</b>) EDX gallium mapping image of fabricated line and (<b>c</b>) EDX gallium mapping image of fabricated line.</p>
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<p>Examples of 2D pattern fabrication using EGaIn colloidal particles: (<b>a</b>) YNU, (<b>b</b>) dumbbell pattern and (<b>c</b>) high magnification SEM image of aggregated EGaIn colloidal particles.</p>
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<p>Illustration of the improved conductivity of a fabricated line using galvanic displacement.</p>
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<p>Photographs of the fabricated line after galvanic replacement at different concentrations of AgNO<sub>3</sub>: (<b>a</b>) 0.5 M and (<b>b</b>) 12.7 M. Immersion time: 24 h.</p>
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<p>Confirmation that the fabricated line functions as wiring from the lighting of the SMD LED. Immersed in 12.7 M AgNO<sub>3</sub> for 24 h.</p>
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<p>Dependence of the resistance on the curvature of the flexible wiring fabricated by the bubble printing of EGaIn colloidal particles and galvanic replacement. Immersed in 12.7 M AgNO<sub>3</sub> for 5 min.</p>
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<p>Relationship between the laser power and fabricating line width. The inset shows lines fabricated at 15 mW.</p>
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36 pages, 3550 KiB  
Review
Advanced Laser Techniques for the Development of Nature-Inspired Biomimetic Surfaces Applied in the Medical Field
by Anita Ioana Visan and Gianina Florentina Popescu-Pelin
Coatings 2024, 14(10), 1290; https://doi.org/10.3390/coatings14101290 - 9 Oct 2024
Viewed by 847
Abstract
This review focuses on the innovative use of laser techniques in developing and functionalizing biomimetic surfaces, emphasizing their potential applications in the medical and biological fields. Drawing inspiration from the remarkable properties of various natural systems, such as the water-repellent lotus leaf, the [...] Read more.
This review focuses on the innovative use of laser techniques in developing and functionalizing biomimetic surfaces, emphasizing their potential applications in the medical and biological fields. Drawing inspiration from the remarkable properties of various natural systems, such as the water-repellent lotus leaf, the adhesive gecko foot, the strong yet lightweight spider silk, and the unique optical structures of insect wings, we explore the potential for replicating these features through advanced laser surface modifications. Depending on the nature and architecture of the surface, particular techniques have been designed and developed. We present an in-depth analysis of various methodologies, including laser ablation/evaporation techniques, such as Pulsed Laser Deposition and Matrix-Assisted Pulsed Laser Evaporation, and approaches for laser surface structuring, including two-photon lithography, direct laser interference patterning, laser-induced periodic surface structures, direct laser writing, laser-induced forward transfer, and femtosecond laser ablation of metals in organic solvents. Additionally, specific applications are highlighted with the aim of synthesizing this knowledge and outlining future directions for research that further explore the intersection of laser techniques and biomimetic surfaces, paving the way for advancements in biomedical applications. Full article
(This article belongs to the Special Issue Biomimetic Approaches in Coatings Synthesis)
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<p>Surface functionalization by laser techniques to mimic natural systems [<a href="#B4-coatings-14-01290" class="html-bibr">4</a>,<a href="#B5-coatings-14-01290" class="html-bibr">5</a>,<a href="#B6-coatings-14-01290" class="html-bibr">6</a>,<a href="#B7-coatings-14-01290" class="html-bibr">7</a>,<a href="#B8-coatings-14-01290" class="html-bibr">8</a>,<a href="#B9-coatings-14-01290" class="html-bibr">9</a>].</p>
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<p>Overview of laser systems with their wavelength range [<a href="#B40-coatings-14-01290" class="html-bibr">40</a>,<a href="#B41-coatings-14-01290" class="html-bibr">41</a>,<a href="#B42-coatings-14-01290" class="html-bibr">42</a>,<a href="#B43-coatings-14-01290" class="html-bibr">43</a>].</p>
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<p>Laser Ablation (<b>a</b>) and evaporation (<b>b</b>) processes.</p>
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<p>An example of laser surface structuring and some SEM images of as-obtained structures [<a href="#B106-coatings-14-01290" class="html-bibr">106</a>,<a href="#B107-coatings-14-01290" class="html-bibr">107</a>,<a href="#B108-coatings-14-01290" class="html-bibr">108</a>,<a href="#B109-coatings-14-01290" class="html-bibr">109</a>].</p>
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<p>Applications of selected nature-inspired surfaces for medical purposes, showcasing their unique properties [<a href="#B195-coatings-14-01290" class="html-bibr">195</a>,<a href="#B196-coatings-14-01290" class="html-bibr">196</a>,<a href="#B197-coatings-14-01290" class="html-bibr">197</a>,<a href="#B198-coatings-14-01290" class="html-bibr">198</a>].</p>
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14 pages, 4146 KiB  
Article
Acridone Derivatives for Near-UV Radical Polymerization: One-Component Type II vs. Multicomponent Behaviors
by Adel Noon, Francesco Calogero, Andrea Gualandi, Hiba Hammoud, Tayssir Hamieh, Joumana Toufaily, Fabrice Morlet-Savary, Michael Schmitt, Pier Giorgio Cozzi and Jacques Lalevée
Molecules 2024, 29(19), 4715; https://doi.org/10.3390/molecules29194715 - 5 Oct 2024
Viewed by 775
Abstract
In this work, two novel acridone-based photoinitiators were designed and synthesized for the free radical polymerization of acrylates with a light-emitting diode emitting at 405 nm. These acridone derivatives were employed as mono-component Type II photoinitiators and as multicomponent photoinitiating systems in the [...] Read more.
In this work, two novel acridone-based photoinitiators were designed and synthesized for the free radical polymerization of acrylates with a light-emitting diode emitting at 405 nm. These acridone derivatives were employed as mono-component Type II photoinitiators and as multicomponent photoinitiating systems in the presence of an iodonium salt or an amine synergist (EDB) in which they achieved excellent polymerization initiating abilities and high final conversions of the acrylate group. Photoinitiation mechanisms through which reactive species are produced were investigated employing different complementary techniques including steady-state photolysis, steady-state fluorescence, cyclic voltammetry, UV–visible absorption spectroscopy, and electron spin resonance spectroscopy. Finally, these molecules were also used in the direct laser writing process for the fabrication of 3D objects. Full article
(This article belongs to the Special Issue Synthesis and Application of Photoactive Compounds)
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Graphical abstract

Graphical abstract
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<p>UV–visible absorption properties of compounds Bn-Acr and DPM-Acr in acetonitrile.</p>
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<p>Photopolymerization profiles of TA (acrylate function conversion vs. irradiation time) in laminate (thickness = 25 μm) upon exposure to an LED (λ = 405 nm) in the presence of PIs (1% <span class="html-italic">w</span>/<span class="html-italic">w</span>), PIs/Iod (1%/1% <span class="html-italic">w</span>/<span class="html-italic">w</span>), PIs/EDB (1%/1% <span class="html-italic">w</span>/<span class="html-italic">w</span>), Iod alone (1% <span class="html-italic">w</span>/<span class="html-italic">w</span>), and EDB alone (1% <span class="html-italic">w</span>/<span class="html-italic">w</span>). The irradiation starts at t = 10 s.</p>
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<p>Photolysis of (<b>A</b>) Bn-Acr with Iod (10<sup>−2</sup> M) and (<b>B</b>) DPM-Acr with Iod (10<sup>−2</sup> M) in acetonitrile using LED at λ = 385 nm.</p>
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<p>Fluorescence quenching study of Bn-Acr (<b>A</b>) and DPM-Acr (<b>B</b>) by Iod in acetonitrile; fluorescence quenching study of Bn-Acr (<b>C</b>) and DPM-Acr (<b>D</b>) by EDB in acetonitrile.</p>
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<p>ESR spectra for Bn-Acr recorded in the presence of PBN and tert-butylbenzene with an LED@405nm: (<b>A</b>) before and after irradiation; (<b>B</b>) experimental and simulated spectra observed after irradiation (at t = 180 s).</p>
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<p>ESR spectra for Bn-Acr/Iod recorded in the presence of PBN and tert-butylbenzene with an LED@405nm: (<b>A</b>) before and after irradiation; (<b>B</b>) experimental and simulated spectra observed after irradiation (at t = 60 s).</p>
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<p>Three-dimensional patterns for compound DPM-Acr with Iod (0.1%/1% <span class="html-italic">w</span>/<span class="html-italic">w</span>) in TA were produced after exposure to a laser diode at 405 nm and were analyzed by numerical microscopy.</p>
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<p>Chemical structures and abbreviations of acridone derivatives: previously studied (A-2DPA, A-2PTz) in [<a href="#B26-molecules-29-04715" class="html-bibr">26</a>], and the newly investigated ones in this work (Bn-Acr and DPM-Acr).</p>
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<p>Synthesis of the target PIs.</p>
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<p>The proposed photochemical mechanism for acridone-based PIs as one-component Type II PIs.</p>
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<p>Chemical structures and abbreviations of the benchmark monomer TA, and the additives (Iod) and (EDB).</p>
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13 pages, 3754 KiB  
Article
Size Effects of Copper(I) Oxide Nanospheres on Their Morphology on Copper Thin Films under Near-Infrared Femtosecond Laser Irradiation
by Mizue Mizoshiri, Thuan Duc Tran and Kien Vu Trung Nguyen
Nanomaterials 2024, 14(19), 1584; https://doi.org/10.3390/nano14191584 - 30 Sep 2024
Viewed by 666
Abstract
The femtosecond laser direct writing of metals has gained significant attention for micro/nanostructuring. Copper (I) oxide nanospheres (NSs), a promising material for multi-photon metallization, can be reduced to copper (Cu) and sintered through near-infrared femtosecond laser pulse irradiation. In this study, we investigated [...] Read more.
The femtosecond laser direct writing of metals has gained significant attention for micro/nanostructuring. Copper (I) oxide nanospheres (NSs), a promising material for multi-photon metallization, can be reduced to copper (Cu) and sintered through near-infrared femtosecond laser pulse irradiation. In this study, we investigated the size effect of copper (I) oxide nanospheres on their morphology when coated on Cu thin films and irradiated by near-infrared femtosecond laser pulses. Three Cu2O NS inks were prepared, consisting of small (φ100 nm), large (φ200 nm), and a mixture of φ100 nm and φ200 nm NSs. A unique phenomenon was observed at low laser pulse energy: both sizes of NSs bonded as single layers when the mixed NSs were used. At higher pulse energies, the small NSs melted readily compared to the large NSs. In comparisons between the large and mixed NSs, some large NSs remained intact, suggesting that the morphology of the NSs can be controlled by varying the concentration of different-sized NSs. Considering the simulation results indicating that the electromagnetic fields between large and small NSs are nearly identical, this differential morphology is likely attributed to the differences in the heat capacity of the NSs. Full article
(This article belongs to the Special Issue Laser-Based Nano Fabrication and Nano Lithography: Second Edition)
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Figure 1
<p>A schematic illustration of the direct writing process using femtosecond laser pulse-induced reductive sintering and/or melting of Cu<sub>2</sub>O NSs.</p>
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<p>FE-SEM images and particle size distributions of Cu<sub>2</sub>O NSs with diameters of (<b>a</b>) 100 nm and (<b>b</b>) 200 nm.</p>
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<p>Absorption coefficients of three Cu<sub>2</sub>O NS inks.</p>
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<p>FE-SEM images of line patterns fabricated on Cu thin film-coated Si at various laser pulse energies with a writing speed of 0.1 mm/s.</p>
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<p>Relationship between line width and laser pulse energy.</p>
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<p>SEM images of the typical four bonding states on the Cu thin film-coated Si substrates: (<b>a</b>) single-layered, (<b>b</b>) multi-layered, (<b>c</b>) melted NSs, and (<b>d</b>) LIPSS. Scale bar: 500 nm.</p>
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<p>(<b>a</b>) Three-dimensional overall view of Cu<sub>2</sub>O NS mixed model, (<b>b</b>) xy-plane view, and (<b>c</b>) xz-plane view for calculating electromagnetic fields.</p>
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<p>Electric field distribution for the φ200 nm/φ100 nm Cu<sub>2</sub>O NS mix model: (<b>a</b>) xz plane, (<b>b</b>) yz plane (φ200 nm NS side), (<b>c</b>) yz plane (φ100 nm NS side), and (<b>d</b>) xy plane of the contact point between the Cu<sub>2</sub>O NS and Cu thin film.</p>
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<p>(<b>a</b>) Schematic illustration of the cross-sectional model showing the <span class="html-italic">z</span>-axis penetrating the φ200 nm and φ100 nm Cu<sub>2</sub>O NSs. (<b>b</b>) Electric field intensity distribution along the <span class="html-italic">z</span>-axis, and (<b>c</b>) absorbed electric field intensity distribution along the <span class="html-italic">z</span>-axis.</p>
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11 pages, 7311 KiB  
Article
Large-Scale High-Accuracy and High-Efficiency Phase Plate Machining
by Guanhua Wang, Zhaoxiang Liu, Lvbin Song, Jianglin Guan, Wei Chen, Jian Liu, Jinming Chen, Min Wang and Ya Cheng
Nanomaterials 2024, 14(19), 1563; https://doi.org/10.3390/nano14191563 - 27 Sep 2024
Viewed by 526
Abstract
In this paper, multifunctional, multilevel phase plates of quartz substrate were efficiently prepared by using a newly developed polygon scanner-based femtosecond laser photolithography system combined with inductively coupled discharge plasma reactive-ion etching (ICP-RIE) technology. The femtosecond laser photolithography system can achieve a scanning [...] Read more.
In this paper, multifunctional, multilevel phase plates of quartz substrate were efficiently prepared by using a newly developed polygon scanner-based femtosecond laser photolithography system combined with inductively coupled discharge plasma reactive-ion etching (ICP-RIE) technology. The femtosecond laser photolithography system can achieve a scanning speed of 5 m/s and a preparation efficiency of 15 cm2/h while ensuring an overlay alignment accuracy of less than 100 nm and a writing resolution of 500 nm. The ICP-RIE technology can control the etching depth error within ±5 nm and the mask-to-mask edge error is less than 1 μm. An 8-level Fresnel lens phase plate with a focal length of 20 mm and an 8-level Fresnel axicon phase plate with a cone angle of 5° were demonstrated. The diffraction efficiency was greater than 93%, and their performance was tested for focusing and glass cutting, respectively. Combined with the high-speed femtosecond laser photolithography system’s infinite field-of-view (IFOV) processing capability, the one-time direct writing preparation of phase plate masks of different sizes was realized on a 6-inch wafer. This is expected to reduce the production cost of quartz substrate diffractive optical elements and promote their customized mass production. Full article
(This article belongs to the Section Nanofabrication and Nanomanufacturing)
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Figure 1
<p>High-precision infinite field-of-view femtosecond laser direct writing system.</p>
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<p>(<b>a</b>–<b>f</b>) correspond to the mask patterns M1, M2, and M3 in three photolithographic processes of the Fresnel lens and Fresnel axicon, respectively.</p>
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<p>A flow chart of the femtosecond laser photolithography-assisted ICP-RIE in fabricating multilevel phase plates.</p>
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<p>Phase design diagram (<b>a</b>) and SEM image (<b>b</b>) of 8-level Fresnel lens; phase diagram (<b>c</b>) and SEM image (<b>d</b>) of 8-level Fresnel axicon.</p>
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<p>The partial depth variation curve of the three times mask preparations of the 8-level Fresnel lens (<b>a</b>) and Fresnel axicon (<b>b</b>). Steps 1 to 3 correspond to the mask preparation results of M1 to M3, while black dashed lines indicate the theoretical depth for each level.</p>
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<p>Graph of the diffraction efficiency as a function of the number of phase levels. The blue and green bars are the experimental diffraction efficiency of the Fresnel axicon and the Fresnel lens, respectively. The purple bars are the theoretical diffraction efficiency.</p>
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<p>(<b>a</b>) The input collimated laser beam profile with a wavelength of 1030 nm; (<b>b</b>) focused spot profile of the Fresnel lens; (<b>c</b>) schematic diagram of Fresnel lens imaging (<b>left</b>) and the imaging patterns of the masks captured using CCD camera (<b>right</b>).</p>
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<p>(<b>a</b>) Schematic diagram of the cutting experiment; (<b>b</b>) microscope image of the glass surface after laser processing; (<b>c</b>) microscope image of the glass cutting section.</p>
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<p>Large-scale diffractive optical elements fabricated on a 6-inch quartz wafer.</p>
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11 pages, 3519 KiB  
Article
Optimization of Non-Alloyed Backside Ohmic Contacts to N-Face GaN for Fully Vertical GaN-on-Silicon-Based Power Devices
by Youssef Hamdaoui, Sofie S. T. Vandenbroucke, Sondre Michler, Katir Ziouche, Matthias M. Minjauw, Christophe Detavernier and Farid Medjdoub
Micromachines 2024, 15(9), 1157; https://doi.org/10.3390/mi15091157 - 15 Sep 2024
Viewed by 1176
Abstract
In the framework of fully vertical GaN-on-Silicon device technology development, we report on the optimization of non-alloyed ohmic contacts on the N-polar n+-doped GaN face backside layer. This evaluation is made possible by using patterned TLMs (Transmission Line Model) through direct laser writing [...] Read more.
In the framework of fully vertical GaN-on-Silicon device technology development, we report on the optimization of non-alloyed ohmic contacts on the N-polar n+-doped GaN face backside layer. This evaluation is made possible by using patterned TLMs (Transmission Line Model) through direct laser writing lithography after locally removing the substrate and buffer layers in order to access the n+-doped backside layer. As deposited non-alloyed metal stack on top of N-polar orientation GaN layer after buffer layers removal results in poor ohmic contact quality. To significantly reduce the related specific contact resistance, an HCl treatment is applied prior to metallization under various time and temperature conditions. A 3 min HCl treatment at 70 °C is found to be the optimum condition to achieve thermally stable high ohmic contact quality. To further understand the impact of the wet treatment, SEM (Scanning Electron Microscopy) and XPS (X-ray Photoelectron Spectroscopy) analyses were performed. XPS revealed a decrease in Ga-O concentration after applying the treatment, reflecting the higher oxidation susceptibility of the N-polar face compared to the Ga-polar face, which was used as a reference. SEM images of the treated samples show the formation of pyramids on the N-face after HCl treatment, suggesting specific wet etching planes of the GaN crystal from the N-face. The size of the pyramids is time-dependent; thus, increasing the treatment duration results in larger pyramids, which explains the degradation of ohmic contact quality after prolonged high-temperature HCl treatment. Full article
(This article belongs to the Section D1: Semiconductor Devices)
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<p>Side view diagram of the N-face (<b>a</b>) and Ga-face (<b>b</b>) GaN in the presence of oxygen atoms.</p>
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<p>Schematic overview of the studied samples to characterize the ohmic contacts on N-face GaN layer, samples B–D (<b>a</b>), and Ga-face GaN layer, sample A (<b>b</b>).</p>
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<p>Current versus etching time curves to control the etch depth.</p>
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<p>SEM and optical images of vertical GaN membranes with TLM patterns after metallization and lift-off. The rectangular membranes width are 1 mm, 3 mm, and 5 mm. The circular membrane diameters are 1 mm, 3 mm, and 5 mm.</p>
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<p>(<b>a</b>) TLM measurements of the N-face ohmic contact without treatment after various time durations between buffer etching and metal deposition. (<b>b</b>) N-face TLM measurements comparison of different HCl treatment times (0–5 min) at 70 °C.</p>
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<p>Rc versus time of treatment at 70 °C.</p>
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<p>TLM measurements of the N-face ohmic contact with HCl pretreatment before and after thermal stress for 1 h at 300 °C.</p>
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<p>(<b>a</b>) Ga3d spectra of the 5 min HCl-treated N-face sample demonstrating how the spectra are fitted. (<b>b</b>) O-Ga/Ga ratio in the Ga3d spectra as measured by XPS as a function of HCl treatment time at 70 °C for N-face (squares) and Ga-face (circles).</p>
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<p>SEM images of the HCl-treated GaN surfaces.</p>
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<p>(<b>a</b>) N-face TLM measurements for samples treated with HCl treatment at different temperatures (RT, 55 °C, and 70 °C) (<b>b</b>) Ga-face TLM measurements comparison with and without HCL treatment.</p>
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16 pages, 10385 KiB  
Article
Laser Direct Writing of Setaria Virids-Inspired Hierarchical Surface with TiO2 Coating for Anti-Sticking of Soft Tissue
by Qingxu Zhang, Yanyan Yang, Shijie Huo, Shucheng Duan, Tianao Han, Guang Liu, Kaiteng Zhang, Dengke Chen, Guang Yang and Huawei Chen
Micromachines 2024, 15(9), 1155; https://doi.org/10.3390/mi15091155 - 15 Sep 2024
Viewed by 921
Abstract
In minimally invasive surgery, the tendency for human tissue to adhere to the electrosurgical scalpel can complicate procedures and elevate the risk of medical accidents. Consequently, the development of an electrosurgical scalpel with an anti-sticking coating is critically important. Drawing inspiration from nature, [...] Read more.
In minimally invasive surgery, the tendency for human tissue to adhere to the electrosurgical scalpel can complicate procedures and elevate the risk of medical accidents. Consequently, the development of an electrosurgical scalpel with an anti-sticking coating is critically important. Drawing inspiration from nature, we identified that the leaves of Setaria Virids exhibit exceptional non-stick properties. Utilizing this natural surface texture as a model, we designed and fabricated a specialized anti-sticking surface for electrosurgical scalpels. Employing nanosecond laser direct writing ablation technology, we created a micro-nano textured surface on the high-frequency electrosurgical scalpel that mimics the structure found on Setaria Virids leaves. Subsequently, a TiO2 coating was deposited onto the ablated scalpel surface via magnetron sputtering, followed by plasma-induced hydrophobic modification and treatment with octadecyltrichlorosilane (OTS) to enhance the surface’s affinity for silicone oil, thereby constructing a self-lubricating and anti-sticking surface. The spreading behavior of deionized water, absolute ethanol, and dimethyl silicone oil on this textured surface is investigated to confirm the effectiveness of the self-lubrication mechanism. Furthermore, the sticking force and quality are compared between the anti-sticking electrosurgical scalpel and a standard high-frequency electrosurgical scalpel to demonstrate the efficacy of the nanosecond laser-ablated micro-nano texture in preventing sticking. The findings indicate that the self-lubricating anti-sticking surface fabricated using this texture exhibits superior anti-sticking properties. Full article
(This article belongs to the Special Issue Recent Advances in Micro/Nano-Fabrication)
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<p>(<b>a</b>) The morphology of Setaria Virids and the sticking state of dewdrops on the surface of Setaria Virids leaves. (<b>b</b>) The front contact angle θ<sub>A</sub> and the rear contact angle θ<sub>B</sub> of a droplet on the surface of a horizontally placed Setaria Virids leaf. (<b>c</b>) White light interference morphology characterization of micro-nano textures processed by nanosecond laser. (<b>d</b>) Ideal illustration of micro-nano textures prepared using nanosecond laser. (<b>e</b>) Scanning Electron Microscopy (SEM) characterization of the microstructure on the surface of Setaria Virids leaves. (<b>f</b>) The flow of a droplet on the surface of a Setaria Virids leaf placed at an inclination of 20°. (<b>g</b>) A mechanism illustration showing the preparation of a functionalized surface with anti-sticking properties by creating a microgroove–micropillar composite texture using a nanosecond laser, followed by Plasma modification and a self-assembled molecular layer coating.</p>
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<p>(<b>a</b>) Mechanism diagram of laser processing surface micro-nano texture. (<b>b</b>) Removal of sharp tips by water bath heating. (<b>c</b>) Microscopic observation of the processed surface micro-nano texture.</p>
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<p>(<b>a</b>) Successful OTS chemical grafting was confirmed by Raman spectroscopy. (<b>b</b>) Chemical mechanism diagram of OTS self-assembly.</p>
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<p>The white light interference morphology, longitudinal and transverse profile characterization, as well as SEM images of micro/nano texture were obtained at inclination angles β of 90°, 85°, 75°, and 60° between the oblique column and the horizontal plane. “A-A” and “B-B” denote the cross-sectional illustrations for the respective micro-nano textures, with “A-A” showcasing the horizontal profile and “B-B” the vertical profile.</p>
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<p>Self-lubricating anti-stick surface with added lubricant.</p>
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<p>Antigravity spreading of deionized water (labeled with rhodamine B as orange yellow), anhydrous ethanol (labeled with fluorescein sodium as yellow green), and dimethylsilicone oil (colorless and transparent) on the texture of oblique columns with different inclination angles. (<b>a</b>) Antigravity spreading mechanism of liquid on micro/nano texture. (<b>b</b>) Antigravity spreading of liquid on a functional surface with a slant column angle of 90°. (<b>c</b>) Antigravity spreading of liquid on a functional surface with a slant column angle of 85°. (<b>d</b>) Antigravity spreading of liquid on a functional surface with a slant column angle of 75°. (<b>e</b>) Antigravity spreading of liquid on a functional surface with a slant column angle of 60°.</p>
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<p>Unidirectional flow of the bulk on the texture of different slant column angles (90°, 85°, 75°, 60°). (<b>a</b>) Absolute ethanol (labeled with fluorescein sodium in yellow green). (<b>b</b>) Deionized water (labeled with rhodamine B in orange yellow). (<b>c</b>) 10cs dimethylsilicone oil (colorless and transparent). (<b>d</b>) Summary plot of one-way spreading data of the three liquids.</p>
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<p>Sticking force measured by digital explicit push–pull dynamometer.</p>
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<p>Sticking force and adhesion scale characteristics of high frequency electric scalpel and the inclination Angle β = 90°, 85°, 75°, and 60° between the upper oblique column of the electric scalpel and the horizontal plane. (<b>a</b>) When the operating power of the electric scalpel was 50 w, the amount of adhesion and thermal injury wound of fresh pig liver was cut with a high frequency electric scalpel (the number of electric cutting S = 1, 10, 20). (<b>b</b>) When the operating power of the electric scalpel was 50 w, the amount of adhesion and thermal injury wound of fresh pig liver was cut by the anti-stick electric scalpel with the angle of microcolumn β = 90° (the number of electric cutting S = 1, 10, 20). (<b>c</b>) When the electric scalpel working power was 50 w, the amount of adhesion and thermal injury wound of fresh pig liver was cut by the anti-stick electric scalpel with the angle of microcolumn β = 85° (the number of electric cutting S = 1, 10, 20). (<b>d</b>) When the operating power of electric scalpel was 50 w, the amount of adhesion and thermal injury wound of fresh pig liver was cut by the anti-stick electric scalpel with the angle β = 85°. The amount of adhesion and thermal injury wound of fresh pig liver was cut by the anti-stick electric scalpel with the angle of microcolumn β = 75° (the number of electric cutting S = 1, 10, 20). (<b>e</b>) When the operating power of the electric scalpel was 50 w, the amount of adhesion and thermal injury wound (electrotomy times S = 1, 10, 20) of fresh pig liver was cut with the anti-stick electrotome with micropillar angle β = 60°. (<b>f</b>) Comparison of adhesion forces between high frequency electrotome and different micropillar angle (90°, 85°, 75°, 60°).</p>
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<p>Comparison curves of adhesion amount versus adhesion force when the number of cycles are 1, 10, and 20.</p>
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35 pages, 16826 KiB  
Review
Recent Advances in Applications of Ultrafast Lasers
by Sibo Niu, Wenwen Wang, Pan Liu, Yiheng Zhang, Xiaoming Zhao, Jibo Li, Maosen Xiao, Yuzhi Wang, Jing Li and Xiaopeng Shao
Photonics 2024, 11(9), 857; https://doi.org/10.3390/photonics11090857 - 11 Sep 2024
Viewed by 1606
Abstract
Ultrafast lasers, characterized by femtosecond and picosecond pulse durations, have revolutionized material processing due to their high energy density and minimal thermal diffusion, and have played a transformative role in precision manufacturing. This review first traces the progression from early ruby lasers to [...] Read more.
Ultrafast lasers, characterized by femtosecond and picosecond pulse durations, have revolutionized material processing due to their high energy density and minimal thermal diffusion, and have played a transformative role in precision manufacturing. This review first traces the progression from early ruby lasers to modern titanium–sapphire lasers, highlighting breakthroughs like Kerr-lens mode-locking and chirped pulse amplification. It also examines the interaction mechanisms between ultrafast pulses and various materials, including metals, dielectrics, and semiconductors. Applications of ultrafast lasers in microstructure processing techniques are detailed, such as drilling, cutting, surface ablation, and nano welding, demonstrating the versatility and precision of the technology. Additionally, it covers femtosecond laser direct writing for optical waveguides and the significant advancements in imaging and precision measurement. This review concludes by discussing potential future advancements and industrial applications of ultrafast lasers. Full article
(This article belongs to the Special Issue New Perspectives in Ultrafast Intense Laser Science and Technology)
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<p>A diagram of the short history of ultrafast lasers and manufacturing processing. (The yellow border indicates the short history of ultrafast lasers, and the purple border indicates the short history of manufacturing processing).</p>
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<p>The applications of ultrafast lasers. Reprinted with permission from [<a href="#B57-photonics-11-00857" class="html-bibr">57</a>,<a href="#B58-photonics-11-00857" class="html-bibr">58</a>,<a href="#B59-photonics-11-00857" class="html-bibr">59</a>,<a href="#B60-photonics-11-00857" class="html-bibr">60</a>,<a href="#B61-photonics-11-00857" class="html-bibr">61</a>,<a href="#B62-photonics-11-00857" class="html-bibr">62</a>]. Copyright (2017) AIP publishing, Copyright (2017) DE GRUYTER, Copyright (2020) Annual Reviews, Copyright (2022) Springer, Copyright (2016) Wiley Online Library, and Copyright (2020) Optica Publishing Group.</p>
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<p>Morphology of micropores drilled by laser with different pulse widths. Reprinted with permission from [<a href="#B72-photonics-11-00857" class="html-bibr">72</a>]. Copyright (1996) Springer-Verlag 1996. (<b>a</b>) Nanosecond-pulse laser. (<b>b</b>) Picosecond-pulse laser. (<b>c</b>) Femtosecond-pulse laser.</p>
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<p>Four categories of laser drilling strategies. (<b>a</b>) Single pulse. (<b>b</b>) Percussion. (<b>c</b>) Trepanning. (<b>d</b>) Helical drilling.</p>
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<p>(<b>a</b>,<b>b</b>) are SEM images of ball end mill before and after cutting. Reprinted with permission from [<a href="#B83-photonics-11-00857" class="html-bibr">83</a>]. Copyright (2016) Elsevier B.V. (<b>c</b>) 600 μm thickness X−ray diamond lens. Reprinted with permission from [<a href="#B85-photonics-11-00857" class="html-bibr">85</a>]. Copyright (2016) Springer Nature.</p>
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<p>Hierarchical hydrophilic/hydrophobic/bumpy Janus film. Reprinted with permission from [<a href="#B88-photonics-11-00857" class="html-bibr">88</a>]. Copyright (2021) ACS Publications.</p>
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<p>(<b>a</b>,<b>b</b>) are the welding of Ag-Ag homogeneous metal nanowires. Reprinted with permission from [<a href="#B98-photonics-11-00857" class="html-bibr">98</a>]. Copyright (2016) IOP Publishing. (<b>c</b>,<b>d</b>) are the welding of ZnO-ZnO homogeneous semiconductor nanowires. Reprinted with permission from [<a href="#B99-photonics-11-00857" class="html-bibr">99</a>]. Copyright (2019) AIP Publishing. (<b>e</b>) is the welding of Ag-TiO<sub>2</sub> heterogeneous nanowires. Reprinted with permission from [<a href="#B100-photonics-11-00857" class="html-bibr">100</a>]. Copyright (2016) AIP Publishing. (<b>f</b>) is the welding of Au nanowires and TiO<sub>2</sub> sinkers. Reprinted with permission from [<a href="#B61-photonics-11-00857" class="html-bibr">61</a>]. Copyright (2016) WILEY.</p>
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<p>(<b>a</b>) Two−dimensional waveguide. Reprinted with permission from [<a href="#B102-photonics-11-00857" class="html-bibr">102</a>]. Copyright (2005) Optica Publishing Group. (<b>b</b>) Three-dimensional waveguide. Reprinted with permission from [<a href="#B103-photonics-11-00857" class="html-bibr">103</a>]. Copyright (2005) IOP Publishing. (<b>c</b>) Photonic wires for optical interconnection. Reprinted with permission from [<a href="#B104-photonics-11-00857" class="html-bibr">104</a>]. Copyright (2012) Optica Publishing Group.</p>
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<p>Cross-section of four types of FsLDW waveguide. (<b>a</b>) Directly written waveguides. (<b>b</b>) Stress-induced waveguides. (<b>c</b>) Depressed cladding waveguides. (<b>d</b>) Ablated ridge waveguides.</p>
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<p>(<b>a</b>) 1 × 2 couplers. (<b>b</b>) 2 × 2 couplers. (<b>c</b>) 3 × 3 couplers. Reprinted with permission from [<a href="#B111-photonics-11-00857" class="html-bibr">111</a>]. Copyright (2020) MDPI.</p>
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<p>(<b>a</b>,<b>b</b>) are schematics of cladding splitters in Ti: Sapphire substrate with a femtosecond laser. Reprinted with permission from [<a href="#B117-photonics-11-00857" class="html-bibr">117</a>]. Copyright (2018) Elsevier B.V. (<b>c</b>,<b>d</b>) are schematics and results of 1 × 3 waveguide beam splitters in lithium niobate crystals. Reprinted with permission from [<a href="#B120-photonics-11-00857" class="html-bibr">120</a>]. Copyright (2016) Optica Publishing Group.</p>
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<p>(<b>a</b>) Two−aperture geometrical layout of an interferometer system. Reprinted with permission from [<a href="#B126-photonics-11-00857" class="html-bibr">126</a>]. Copyright (2010) IEEE. (<b>b</b>) Model of the SPIDER payload integrated with a Surrey spacecraft bus. Reprinted with permission from [<a href="#B129-photonics-11-00857" class="html-bibr">129</a>]. Copyright (2013) Maui Economic Development Board, Inc., Kihei, HI, USA. All Rights Reserved. (<b>c</b>) Layer-by-layer concept of SPIDER [<a href="#B127-photonics-11-00857" class="html-bibr">127</a>,<a href="#B128-photonics-11-00857" class="html-bibr">128</a>]. (<b>d</b>) Head-to-tail baseline pairing method. (<b>e</b>) Schematic functional diagram. Reprinted with permission from [<a href="#B128-photonics-11-00857" class="html-bibr">128</a>]. Copyright (2023) Optica Publishing Group.</p>
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<p>(<b>a</b>) Wide−FOV SPIDER mosaic image. Reprinted with permission from [<a href="#B129-photonics-11-00857" class="html-bibr">129</a>]. Copyright (2013) Maui Economic Development Board, Inc. All Rights Reserved. (<b>b</b>) Schematic of the 2D image optical bed and simulated image. Reprinted with permission from [<a href="#B130-photonics-11-00857" class="html-bibr">130</a>]. Copyright (2017) Advanced Maui Optical and Space Surveillance Technologies Conference (AMOS). (<b>c</b>) USAF bar chart test target and the train scene target used for SPIDER imaging and its corresponding reconstructed image. Reprinted with permission from [<a href="#B131-photonics-11-00857" class="html-bibr">131</a>]. Copyright (2018) Optical Society of America.</p>
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<p>(<b>a</b>) The system structure, the novel arrangement of a lenslet array, and the images acquired through different approaches. Reprinted with permission from [<a href="#B132-photonics-11-00857" class="html-bibr">132</a>]. Copyright (2021) Optical Society of America. (<b>b</b>) A schematic diagram of the lenslet arrangement, uv−spatial spectrum coverage, and simulation results by different approaches. Reprinted with permission from [<a href="#B128-photonics-11-00857" class="html-bibr">128</a>]. Copyright (2023) Optical Society of America.</p>
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<p>Schematic of self-assembly of silver nanoparticles. Reprinted with permission from [<a href="#B138-photonics-11-00857" class="html-bibr">138</a>]. Copyright (2015) IOP Publishing.</p>
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<p>SEM images of the morphology of a microlens array. (<b>a</b>) Morphology of a square microlens array. (<b>b</b>) Morphology of a hexagon microlens array. (<b>c</b>) Enlarged view of a part of (<b>a</b>), and (<b>d</b>) enlarged view of part (<b>b</b>). Dotted boxes of the same color represent local magnification [<a href="#B140-photonics-11-00857" class="html-bibr">140</a>]. Copyright (2021) optica publishing group.</p>
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<p>(<b>a</b>) Microlens array snapshot hyperspectral system. (<b>b</b>) The original graph. (<b>c</b>) Images at wavelength from 350.67 to 770.21 nm. Reprinted with permission from [<a href="#B146-photonics-11-00857" class="html-bibr">146</a>]. Copyright (2019) Chinese Laser Press.</p>
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<p>White-light remote sensing system. (<b>a</b>) Schematic. (<b>b</b>) Vertical white-light remote sensing profile at three wavelengths. (<b>c</b>) High-resolution atmospheric absorption spectrum. Reprinted with permission from [<a href="#B149-photonics-11-00857" class="html-bibr">149</a>]. Copyright (2003) AAAS.</p>
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<p>(<b>a</b>) Result of 45 km remote sensing. Reprinted with permission from [<a href="#B151-photonics-11-00857" class="html-bibr">151</a>]. Copyright (2020) Optica Publishing Group. (<b>b</b>) Result of 201.5 km remote sensing. Reprinted with permission from [<a href="#B62-photonics-11-00857" class="html-bibr">62</a>]. Copyright (2021) Optica Publishing Group. (<b>c</b>) Result of 100 km remote sensing by a single-pixel camera. Reprinted with permission from [<a href="#B152-photonics-11-00857" class="html-bibr">152</a>]. Copyright (2020) Optica Publishing Group.</p>
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<p>High-numerical-aperture femtosecond pump–probe microscope. (<b>a</b>) Experimental setup. (<b>b</b>) The spectra of white light pulse. (<b>c</b>–<b>e</b>) are optical micrographs obtained a few seconds before and after the arrival of the pump pulse. Reprinted with permission from [<a href="#B57-photonics-11-00857" class="html-bibr">57</a>]. Copyright (2017) AIP Publishing.</p>
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<p>Spectra resulting from fs laser-induced breakdown in an air–methane flame operating with different fuel content. Reprinted with permission from [<a href="#B162-photonics-11-00857" class="html-bibr">162</a>]. Copyright (2013) Elsevier B.V.</p>
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10 pages, 3059 KiB  
Article
High-Extraction-Rate Ta2O5-Core/SiO2-Clad Photonic Waveguides on Silicon Fabricated by Photolithography-Assisted Chemo-Mechanical Etching (PLACE)
by Jian Liu, Youting Liang, Lang Gao, Chao Sun, Jianglin Guan, Zhe Wang, Zhaoxiang Liu, Zhiwei Fang, Min Wang, Haisu Zhang and Ya Cheng
Nanomaterials 2024, 14(17), 1466; https://doi.org/10.3390/nano14171466 - 9 Sep 2024
Viewed by 785
Abstract
We demonstrate high-extraction-rate Ta2O5-core/SiO2-clad photonic waveguides on silicon fabricated by the photolithography-assisted chemo-mechanical etching technique. Low-confinement waveguides of larger than 70% coupling efficiency with optical fibers and medium propagation loss around 1 dB/cm are investigated in the [...] Read more.
We demonstrate high-extraction-rate Ta2O5-core/SiO2-clad photonic waveguides on silicon fabricated by the photolithography-assisted chemo-mechanical etching technique. Low-confinement waveguides of larger than 70% coupling efficiency with optical fibers and medium propagation loss around 1 dB/cm are investigated in the experiment. Monolithic microring resonators based on Ta2O5 waveguides have shown the quality factors to be above 105 near 1550 nm. The demonstrated Ta2O5 waveguides and their fabrication method hold great promise in various cost-effective applications, such as optical interconnecting and switching. Full article
(This article belongs to the Special Issue Laser-Based Nano Fabrication and Nano Lithography: Second Edition)
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<p>Design and property of Ta<sub>2</sub>O<sub>5</sub> waveguide: (<b>a</b>) a cross-section schematic of the Ta<sub>2</sub>O<sub>5</sub> waveguide, (<b>b</b>) the simulated fundamental TE-mode profile of the Ta<sub>2</sub>O<sub>5</sub> waveguide at 1550 nm, (<b>c</b>) the effective refractive index vs waveguide width for different modes, (<b>d</b>) the effective index and group index vs wavelength for the fundamental modes.</p>
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<p>Fabrication processes of the Ta<sub>2</sub>O<sub>5</sub> waveguide: (<b>a</b>) the thickness profile of the deposited Ta<sub>2</sub>O<sub>5</sub> film, (<b>b</b>) the process flow for the Ta<sub>2</sub>O<sub>5</sub> waveguide fabrication.</p>
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<p>Microscopy characterization of the Ta<sub>2</sub>O<sub>5</sub> waveguide: (<b>a</b>) SEM image of the Ta<sub>2</sub>O<sub>5</sub> waveguide before oxide cladding deposition, (<b>b</b>) SEM image of the Ta<sub>2</sub>O<sub>5</sub> waveguide after oxide cladding deposition, (<b>c</b>,<b>d</b>) top-view optical microscope images of the Ta<sub>2</sub>O<sub>5</sub> waveguide, (<b>e</b>) top-view SEM image of the Ta<sub>2</sub>O<sub>5</sub> waveguide, (<b>f</b>) top-view AFM image of the Ta<sub>2</sub>O<sub>5</sub> waveguide. The region in the green dashed boxes is the Ta<sub>2</sub>O<sub>5</sub> core layer.</p>
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<p>Guided mode and propagation loss: (<b>a</b>) the experimental setup for waveguide mode and loss measurement, (<b>b</b>) the output mode profile of the Ta<sub>2</sub>O<sub>5</sub> waveguide, (<b>c</b>) the output mode profile of the UHNA7 fiber, (<b>d</b>) the calculated mode overlap factor and coupling loss between the Ta<sub>2</sub>O<sub>5</sub> waveguide and the UHNA7 fiber, (<b>e</b>) the measured insertion losses of the Ta<sub>2</sub>O<sub>5</sub> waveguide of variable lengths and bending radii.</p>
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<p>Microresonator characterization setup. The microscope image of the fabricated microring resonator is shown in the middle. Red lines denote a fiber connection and black lines represent an electrical connection.</p>
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<p>Microresonator Q-factor characterization. (<b>a</b>) The full transmission spectrum of the microresonator from 1545 nm to 1555 nm. (<b>b</b>) The enlarged part of the transmission spectrum showing the FSR of 0.05 nm. (<b>c</b>) The Lorentz fitting of the resonance profile around 1550.12 nm. (<b>d</b>) The Q-factors and corresponding propagation losses retrieved from microring resonators of different waveguide widths.</p>
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16 pages, 12602 KiB  
Article
Advancing 3D Spheroid Research through 3D Scaffolds Made by Two-Photon Polymerization
by Eglė Vitkūnaitė, Eglė Žymantaitė, Agata Mlynska, Dovilė Andrijec, Karolina Limanovskaja, Grzegorz Kaszynski, Daumantas Matulis, Vidmantas Šakalys and Linas Jonušauskas
Bioengineering 2024, 11(9), 902; https://doi.org/10.3390/bioengineering11090902 - 9 Sep 2024
Viewed by 1206
Abstract
Three-dimensional cancer cell cultures have been a valuable research model for developing new drug targets in the preclinical stage. However, there are still limitations to these in vitro models. Scaffold-based systems offer a promising approach to overcoming these challenges in cancer research. In [...] Read more.
Three-dimensional cancer cell cultures have been a valuable research model for developing new drug targets in the preclinical stage. However, there are still limitations to these in vitro models. Scaffold-based systems offer a promising approach to overcoming these challenges in cancer research. In this study, we show that two-photon polymerization (TPP)-assisted printing of scaffolds enhances 3D tumor cell culture formation without additional modifications. TPP is a perfect fit for this task, as it is an advanced 3D-printing technique combining a μm-level resolution with complete freedom in the design of the final structure. Additionally, it can use a wide array of materials, including biocompatible ones. We exploit these capabilities to fabricate scaffolds from two different biocompatible materials—PEGDA and OrmoClear. Cubic spheroid scaffolds with a more complex architecture were produced and tested. The biological evaluation showed that the human ovarian cancer cell lines SKOV3 and A2780 formed 3D cultures on printed scaffolds without a preference for the material. The gene expression evaluation showed that the A2780 cell line exhibited substantial changes in CDH1, CDH2, TWIST, COL1A1, and SMAD3 gene expression, while the SKOV3 cell line had slight changes in said gene expression. Our findings show how the scaffold architecture design impacts tumor cell culture 3D spheroid formation, especially for the A2780 cancer cell line. Full article
(This article belongs to the Section Nanobiotechnology and Biofabrication)
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<p>Schematic illustrating study design. First, 3D scaffolds were produced using TPP technology. Then, the structures were seeded with two different human ovarian cancer cell lines—SKOV3 and A2780. Spheroid formation on the scaffolds conformed to and allowed the determination of various peculiarities related to cell line growth on 3D scaffolds, related to the geometry’s impact, cell–material interactions, and gene expression.</p>
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<p>Schematic of laser printing setup used in this work.</p>
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<p>Three-dimensional models of basic (<b>a</b>) and spherical (<b>b</b>) scaffolds showing the main components and dimensions.</p>
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<p>(<b>a</b>) Optical image of an array of 15 basic scaffolds with 50 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m pores, which were used for the majority of the experiments. (<b>b</b>) SEM image of basic scaffolds with 80 <math display="inline"><semantics> <mi mathvariant="sans-serif">μ</mi> </semantics></math>m pores, showing good structural discrepancies and slight surface roughness for better cell adhesion.</p>
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<p>Top-down optical and SEM images of spheroid scaffolds made out of OrmoClear (<b>a</b>,<b>b</b>) and PEGDA (<b>c</b>,<b>d</b>). (<b>e</b>) An optical image of an OrmoClear spheroid scaffold from an angle. Clear and well-defined 3D pores are visible.</p>
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<p>Representative images of the ovarian cancer cell line SKOV3 3D cell culture grown in 96-well plates at different seeding densities between days 1 and 4. White arrow: ovarian cancer cells. The scale bar represents 300 μm.</p>
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<p>Representative images of the ovarian cancer cell line SKOV3 and A2780 3D cell cultures grown on different scaffolds between days 0 and 7. The scale bar represents 300 μm.</p>
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<p>Ovarian cancer cell line SKOV3 and A2780 3D cell culture gene expression represented as heat maps: (<b>a</b>) gene expression comparison between the cell lines cultured in 3D cell culture conditions. (<b>b</b>) Gene expression comparison of SKOV3 cell line when cells were cultured without and with different scaffolds made from PEGDA or OrmoClear in cubic/standard and spheroid shapes. (<b>c</b>) Gene expression comparison of the A2780 cell line when cells were cultured without and with different scaffolds made from PEGDA or OrmoClear in cubic/standard and spheroid shapes.</p>
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<p>Representative images of the ovarian cancer cell line SKOV3 and A2780 3D cell cultures grown on basic scaffolds with different pore sizes ranging from 100 to 40 µm. Images represent 3D cell culture at day 4. The scale bar represents 300 μm.</p>
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14 pages, 11748 KiB  
Article
Crack-Based Composite Flexible Sensor with Superhydrophobicity to Detect Strain and Vibration
by Yazhou Zhang, Huansheng Wu, Linpeng Liu, Yang Yang, Changchao Zhang and Ji’an Duan
Polymers 2024, 16(17), 2535; https://doi.org/10.3390/polym16172535 - 7 Sep 2024
Viewed by 706
Abstract
Vibration sensors are widely applied in the detection of faults and analysis of operational states in engineering machinery and equipment. However, commercial vibration sensors with a feature of high hardness hinder their usage in some practical applications where the measured objects have irregular [...] Read more.
Vibration sensors are widely applied in the detection of faults and analysis of operational states in engineering machinery and equipment. However, commercial vibration sensors with a feature of high hardness hinder their usage in some practical applications where the measured objects have irregular surfaces that are difficult to install. Moreover, as the operating environments of machinery become increasingly complex, there is a growing demand for sensors capable of working in wet and humid conditions. Here, we present a flexible, superhydrophobic vibration sensor with parallel microcracks. The sensor is fabricated using a femtosecond laser direct writing ablation strategy to create the parallel cracks on a PDMS film, followed by spray-coating with a conductive ink composed of MWCNTs, CB, and PDMS. The results demonstrate that the developed flexible sensor exhibits a high-frequency response of up to 2000 Hz, a high acceleration response of up to 100 m/s2, a water contact angle as high as 159.61°, and a linearity of 0.9812 between the voltage signal and acceleration. The results indicate that the sensor can be employed for underwater vibration, sound recognition, and vibration monitoring in fields such as shield cutters, holding significant potential for mechanical equipment vibration monitoring and speech-based human–machine interaction. Full article
(This article belongs to the Section Polymer Composites and Nanocomposites)
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<p>Preparation of the conductive ink and flexible vibration sensor. (<b>a</b>) Fabrication process of the conductive ink composed of PDMS, CNTs, CBs, and ethyl acetate. (<b>b</b>) Structural and conductive layer fabrication of the vibration sensor. (<b>c</b>) Schematic diagram showing the architecture of the vibration sensor. (<b>d</b>) Optical images of the vibration sensor under different mechanical loads, showing the flexibility of the sensor.</p>
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<p>The sensing mechanism and optical surface images of the sensor, as well as the hydrophobic performance. (<b>a</b>) Sensing mechanism of the sensor under vibrations. (<b>b</b>) Optical images of the sensor’s surface obtained from an ultra-depth three-dimensional microscope. (<b>c</b>) Contact angles of the sensor when different liquids (water, tea, milk, and cola) drop on the sensor’s surface. (<b>d</b>) Water contact angles of the sensor after being subjected to different vibration cycles.</p>
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<p>The response of the flexible sensor to vibrations. (<b>a</b>) Original signals from the sensor under an applied periodic vibration with a frequency of 2000 Hz. Inset: FFT analysis of the original signals, showing a dominant frequency of 2000 Hz. (<b>b</b>) Amplified view of the signal from 0.1 s to 0.105 s in (<b>a</b>). (<b>c</b>) Voltage change of the sensor over time after filtering noise from the original signal in (<b>a</b>). (<b>d</b>) Original signals from the sensor under an applied periodic vibration with a frequency of 100 Hz. Inset: FFT analysis of the original signals, showing a dominant frequency of 100 Hz. (<b>e</b>) Amplified view of the signal from 0.40 s to 0.50 s in (<b>d</b>). (<b>f</b>) Voltage change of the sensor over time after smoothing from the original signal in (<b>d</b>). (<b>g</b>) Real-time response of the sensor to vibrations with different waveforms at a frequency of 100 Hz. (<b>h</b>) Signal output of the sensor under an applied periodic vibration with a frequency of 500 Hz, recording the sensor’s responses of 15,000 cycles within a duration of 30 s. Insets: partially magnified curves for different time stages.</p>
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<p>The response of the vibration sensor to tensile strain and underwater vibration. (<b>a</b>) Sensitivity and linearity of the sensor to tensile strain. (<b>b</b>) Response/recover time of the sensor at 10% strain. (<b>c</b>) Signal output of the sensor for 1000 cycles to the tensile strain of 10%. (<b>d</b>) Electrical response of the three sensors to vibration with a frequency of 100 Hz and an acceleration of 5 m/s<sup>2</sup> in air and underwater, respectively. (<b>e</b>) Electrical response of the three sensors to vibration with a frequency of 300 Hz and an acceleration of 20 m/s<sup>2</sup> in air and underwater, respectively. (<b>f</b>) Electrical response of the three sensors to vibration with a frequency of 900 Hz and an acceleration of 100 m/s<sup>2</sup> in air and underwater, respectively. (<b>g</b>) Relative voltage changes of the sensor under vibrations at a fixed frequency of 100 Hz but different accelerations at 5, 10, 15, 20, 25, 30, 35, and 40 m/s<sup>2</sup>, respectively. (<b>h</b>) Relationship between the sensor’s voltage response and acceleration under vibrations at a fixed frequency of 100 Hz.</p>
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<p>Vibration monitoring and speech recognition performance of the developed sensor. (<b>a</b>) Optical image of the flexible sensor installed on the surface of a speaker. (<b>b</b>) Output response signals of the sensor when the speaker played a sentence twice and the spectrogram analysis for the recorded electric signals. (<b>c</b>) Voltage responses of the sensor to vibrations generated from the speaker which played four letters in turn. (<b>d</b>) Voltage responses of the vibration sensor to three utterances, including the monosyllabic word “one”, the disyllabic word “sensor”, and the polysyllabic word “sensitivity”. (<b>e</b>) Voltage responses of the commercial accelerometers to three utterances, including the monosyllabic word “one”, the disyllabic word “sensor”, and the polysyllabic word “sensitivity”.</p>
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<p>Vibration monitoring and analysis for the shield machine cutter head when fracturing a rock. (<b>a</b>) Optical image of the shield machine cutter head’s testing platform and the installation of the vibration monitoring system. (<b>b</b>) Real-time voltage signals output from the flexible vibration sensor during the rock fracturing process. (<b>c</b>) An enlarged view from (<b>b</b>) at the stage when the disc cutter contacts with the rock. (<b>d</b>) An enlarged view from (<b>b</b>) at the stage when the disc cutter begins to fracture the rock. Each peak shows the positions where the rock is cracked thoroughly. (<b>e</b>) An enlarged view from (<b>b</b>) at the stage when the disc cutter is retracted.</p>
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14 pages, 2519 KiB  
Review
Developments of Waveguide Lasers by Femtosecond Laser Direct–Writing Technology
by Yang Zhang, Boyan Yu, Zihao Zhang, Xinghao Duan and Junli Wang
Photonics 2024, 11(9), 803; https://doi.org/10.3390/photonics11090803 - 28 Aug 2024
Viewed by 1028
Abstract
Waveguide lasers have the advantages of miniature and compact structure and have broad application prospects in photonic integration and on–chip laboratories. The development of femtosecond laser direct–writing technology makes the processing of transparent materials more flexible and controllable. This paper mainly introduces a [...] Read more.
Waveguide lasers have the advantages of miniature and compact structure and have broad application prospects in photonic integration and on–chip laboratories. The development of femtosecond laser direct–writing technology makes the processing of transparent materials more flexible and controllable. This paper mainly introduces a waveguide laser based on femtosecond laser direct–writing technology. Firstly, the applications of femtosecond laser direct–writing technology in an optical waveguide are introduced, including the principles of femtosecond laser direct–writing technology, common optical wave scanning methods, and types of optical waveguides. After that, we summarize the development of a waveguide continuous–wave laser, a Q–switched laser and a mode–locked laser from visible to mid–infrared wavebands and analyze some new representative work. Finally, we explain the difficulty of compensating for dispersion in pulse waveguide lasers and summarize some new ideas that have been proposed to solve the problem. Full article
(This article belongs to the Special Issue New Perspectives in Ultrafast Intense Laser Science and Technology)
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<p>Ion exchange technology diagram: (<b>a</b>) thermal ion exchange, (<b>b</b>) field-assisted ion exchange.</p>
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<p>The methods to achieve relative displacement between the laser focus and the sample: (<b>a</b>) sample fixed–laser focus moving method [<a href="#B18-photonics-11-00803" class="html-bibr">18</a>], (<b>b</b>) laser focus fixed–sample moving method [<a href="#B18-photonics-11-00803" class="html-bibr">18</a>]. Waveguide trace writing method: (<b>c</b>) longitudinal scanning method, (<b>d</b>) transverse scanning method.</p>
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<p>Optical microscope pictures of the different waveguide types fabricated in Pr:LLF: (<b>a</b>) circular cladding, (<b>b</b>) ear–like cladding, (<b>c</b>) hexagonal cladding, (<b>d</b>) stress–induced dual–line, (<b>e</b>) stress–induced dual–line with rhombic cladding, (<b>f</b>) single line [<a href="#B58-photonics-11-00803" class="html-bibr">58</a>].</p>
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<p>(<b>a</b>) Experimental setup and (<b>b</b>) output pulse characteristics of Nd:GdVO<sub>4</sub> crystal CW waveguide laser [<a href="#B48-photonics-11-00803" class="html-bibr">48</a>]. WP1 and WP2: waveplate; GTP: Glan Taylor prism; MO: microscope objective lens (20×); CL: convex lens; M1 and M2: laser cavity mirrors adhered to the two end facets of the sample; DB: dichroic beamsplitter; λ<sub>p</sub> and λ<sub>L</sub>: pump and generated laser beam; OC: output coupler.</p>
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<p>The common deposition methods of SA in waveguide lasers: (<b>a</b>) evanescent and (<b>b</b>) direct–field interaction with SA.</p>
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<p>The experimental setup for the Ti:sapphire channel waveguides soliton mode–locking [<a href="#B26-photonics-11-00803" class="html-bibr">26</a>]. DPSS laser: diode–pumped solid–state laser. The green arrow represents the propagation direction of the pump light, while the red arrow represents the propagation direction of the signal light.</p>
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<p>The experimental setup of a Yb:YAG crystal CWML waveguide laser from [<a href="#B65-photonics-11-00803" class="html-bibr">65</a>]. OPSL: optically pumped semiconductor laser; DM: dichroic beamsplitter; L, L1 and L2: lens; OC: output coupler.</p>
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9 pages, 2132 KiB  
Article
A Hermetic Package Technique for Multi-Functional Fiber Sensors through Pressure Boundary of Energy Systems Based on Glass Sealants
by Zhichun Fan, Shuda Zhong, Kehao Zhao, Qirui Wang, Yuqi Li, Guangyin Zhang, Guangqun Ma, Jieru Zhao, He Yan, Zhiyong Huang, Jyotsna Sharma and Kevin P. Chen
Photonics 2024, 11(9), 792; https://doi.org/10.3390/photonics11090792 - 25 Aug 2024
Viewed by 774
Abstract
This paper presents a hermitic fiber sensor packaging technique that enables fiber sensors to be embedded in energy systems for performing multi-parameter measurements in high-temperature and strong radiation environments. A high-temperature stable Intrinsic Fabry–Perot interferometer (IFPI) array, inscribed by a femtosecond laser direct [...] Read more.
This paper presents a hermitic fiber sensor packaging technique that enables fiber sensors to be embedded in energy systems for performing multi-parameter measurements in high-temperature and strong radiation environments. A high-temperature stable Intrinsic Fabry–Perot interferometer (IFPI) array, inscribed by a femtosecond laser direct writing scheme, is used to measure both temperature and pressure induced strain changes. To address the large disparity in thermo-expansion coefficients (TECs) between silica fibers and metal parts, glass sealants with TEC between silica optical fibers and metals were used to hermetically seal optical fiber sensors inside stainless steel metal tubes. The hermetically sealed package is validated for helium leakages between 1 MPa and 10 MPa using a helium leak detector. An IFPI sensor embedded in glass sealant was used to measure pressure. The paper demonstrates an effective technique to deploy fiber sensors to perform multi-parameter measurements in a wide range of energy systems that utilize high temperatures and strong radiation environments to achieve efficient energy production. Full article
(This article belongs to the Special Issue Quantum Enhanced Devices and Instruments for Sensing Applications)
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<p>(<b>a</b>) The fabrication of IFPI; (<b>b</b>) The 3D-diagram of IFPI with the glass package installed in the metal tube; (<b>c</b>) the Rayleigh backscattering profile of the multiplexed IFPIs; (<b>d</b>) the spectrum of the multiplexed IFPI array; and (<b>e</b>) the FFT spatial domain of the spectrum.</p>
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<p>(<b>a</b>) The experimental setup of the glass package fabrication; (<b>b</b>) the pressure test setup for IFPI with the glass package.</p>
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<p>(<b>a</b>) The meshing grid of the fiber-glass-metal structure; (<b>b</b>) the fine grid and joint of the glass package and fiber core; (<b>c</b>) the contour of numerical results after the fabrication process; (<b>d</b>) the strain distribution in the fiber core.</p>
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<p>The monitored residual strain of IFPIs during the manufacturing process and corresponding finite element modeling (FEM) results. (<b>a</b>) overall sensors’ cavity change during the embedment process; (<b>b</b>) temperature sensor 2 cavity change during the embedment process; (<b>c</b>) temperature sensor 1 cavity change during the embedment; (<b>d</b>) strain sensor cavity change during the embedment process; (<b>e</b>) residual strain demodulation of the strain sensor.</p>
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<p>The leakage rate of IFPI with a glass sealant package under (<b>a</b>) high-temperature environments and (<b>b</b>) high-pressure environments.</p>
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