Han Gardeniers’s research while affiliated with University of Twente and other places

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Publications (291)


Yb3+-Mediated Luminescence Enhancement in Er3+-Doped 3D-Printed ZrO2 Microarchitectures
  • Article
  • Full-text available

June 2025

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28 Reads

Applied Materials Today

Cristian Rosero-Arias

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Lanthanide-doped ZrO2 ceramics are promising materials for optics due to their high refractive index and tunable luminescent properties. In this study, we investigated the impact of Yb3+ and Er3+ dopant concentrations on the emission behavior of lanthanide-doped 3D ZrO2 microarchitectures fabricated using two-photon lithography. Thermal treatments have been carried out at 600 C and 750 C to promote the stabilization of the ZrO2 tetragonal phase (t-ZrO2) and at 1000 C to induce phase transition in ZrO2 to the monoclinic (m-ZrO2) phase in the 3D microarchitectures. Scanning transmission electron microscopy confirmed the crystallinity changes across the thermal treatments. Photoluminescence (PL) and cathodoluminescence (CL) measurements confirm emission bands of Yb3+ and Er3+ single dopants and Yb3+:Er3+ co-dopants. Variations in Yb3+ content reveal that the PL emission of Er3+ increases (e.g., 4 S 3/2 → 4 I 15/2), which is attributed to the interplay between the dopant concentrations, defect structures and the ZrO2 host. The results highlight the importance of ZrO2 microarchitectures' crystallinity and co-doping relationship, which enable the promotion of Er3+ emissions. We expect our research will find applications in 3D optical systems.

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Schematic depiction of the feature size resolution range of TPL, PµSL, µ‐SLS, and DIW, along with illustration devices like Kinoform X‐ray lenses,[⁶³] woodpile photonic crystals,[67,68] stacked microlenses,[28,69] and micromirror components[70,71] inspired by 3D‐printed architectures found in the literature, accordingly.
Overview of the photoresin developments for pre‐GLACEs. Schematic labels: carbon atoms (grey spheres), oxygen atoms (red spheres), metal or metalloid ions (yellow spheres), nitrogen atoms (blue spheres), hydrogen atoms (white spheres), surface‐protected nanoparticles (green spheres), and functional group R (pink spheres) –, e.g., H, CH3, C2H5. Substitute R with R’ –, e.g., acrylates or di‐epoxy compounds for monomers.
Schematic representation of the thermal conversion leading to a miniaturized GLACE replica, representing the a) printing step of a pre‐GLACE microarchitecture via TPL, b) as‐printed pre‐GLACE 3D microarchitecture showing the cross‐linked chemical nature with inorganic bonded additives, and c) miniaturized GLACE conversion after thermal/annealing exposure, highlighting the inorganic chemical network exemplified as a binary metal oxide. Exemplary d) crystal phase transitions of ZrO2 in bulk and TPL‐printed microarchitectures, and e) phase diagram of bulk YSZ, highlighting (in red dashed‐line) equiv. stabilization for tetragonal zirconia at 4 mol% Y2O3 and low‐temperature phase stabilization for cubic zirconia at 10 mol% Y2O3 in TPL‐printed microarchitectures.[¹⁴⁰]
Schematic depiction of a) perfect lattice, b) atomic vacancies, c) atomic interstitials, d) substitutional and interstitial dopant atoms, e) band gap schematics, and f) 3D multi‐material arrangement including p‐ and n‐type semiconductor in thermal equilibrium including a description of possible defects encountered in such a configuration and the existence of surface states (Dit). The vacuum energy (E0), conduction band energy (EC), valence band energy (EV), and Fermi energy level (EF) are indicated. An insulating cladding layer is also included.
a) Multi‐material composition printing sketch. After printing and development, the precursor for glass/ceramic is annealed. b) Depending on the information needed and the spatial resolution at which the GLACE requires interrogation, a suitable characterization method can be selected to evaluate the chemical composition and crystallinity in space and time for single and multi‐material GLACEs. The abbreviations of the included characterization techniques are as follows. Vibrational spectroscopy methods (green): DORS, diagonally offset Raman spectroscopy; IRM, infrared microscopy; CRM, confocal Raman microscopy; CARS, coherent anti‐Stokes Raman spectroscopy; SRS, stimulated Raman scattering microscopy. Electronic spectroscopy methods (red): CFM, confocal fluorescence microscopy; 2PFM, two‐photon fluorescence microscopy; CLM, chemiluminescence microscopy; STORM, stochastic optical reconstruction microscopy. X‐ray spectroscopy methods (blue): μ‐XAFS, microbeam X‐ray absorption fine structure spectroscopy; XRM, X‐ray microscopy; XMT, and X‐ray microtomography. X‐ray diffraction methods (black): TEDDI, tomographic energy‐dispersive diffraction imaging; XRD‐CT, X‐ray diffraction‐computed tomography. Miscellaneous (orange): CL (or PL, photoluminescence), cathodoluminescence.[133,156,172,209]

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From Single to Multi‐Material 3D Printing of Glass‐Ceramics for Micro‐Optics

February 2025

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177 Reads

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2 Citations

Feynman's statement, “There is plenty of room at the bottom”, underscores vast potential at the atomic scale, envisioning microscopic machines. Today, this vision extends into 3D space, where thousands of atoms and molecules are volumetrically patterned to create light‐driven technologies. To fully harness their potential, 3D designs must incorporate high‐refractive‐index elements with exceptional mechanical and chemical resilience. The frontier, however, lies in creating spatially patterned micro‐optical architectures in glass and ceramic materials of dissimilar compositions. This multi‐material capability enables novel ways of shaping light, leveraging the interaction between diverse interfaced chemical compositions to push optical boundaries. Specifically, it encompasses both multi‐material integration within the same architectures and the use of different materials for distinct architectural features in an optical system. Integrating fluid handling systems with two‐photon lithography (TPL) provides a promising approach for rapidly prototyping such complex components. This review examines single and multi‐material TPL processes, discussing photoresin customization, essential physico‐chemical conditions, and the need for cross‐scale characterization to assess optical quality. It reflects on challenges in characterizing multi‐scale architectures and outlines advancements in TPL for both single and spatially patterned multi‐material structures. The roadmap provides a bridge between research and industry, emphasizing collaboration and contributions to advancing micro‐optics.


Figure 11. (a) Before the pumping starts, liquid movement patterns form inside the channel around each pillar, which increases with an increase in amplitude. The flow velocity in the channel with triangular pillars is higher than that with circular pillars. (b) After the pumping effect starts, the pumping velocity increases with time. This increase is more significant in the channel with triangular pillars.
Enhanced Acoustic Mixing in Silicon-Based Chips with Sharp-Edged Micro-Structures

October 2024

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62 Reads

Micro

The small dimensions of microfluidic channels allow for fast diffusive or passive mixing, which is beneficial for time-sensitive applications such as chemical reactions, biological assays, and the transport of to-be-detected species to sensors. In microfluidics, the need for fast mixing within milliseconds arises primarily because these devices are often used in fields where rapid and efficient mixing significantly impacts the performance and outcome of the processes. Active mixing with acoustics in microfluidic devices involves using acoustic waves to enhance the mixing of fluids within microchannels. Using sharp corners and wall patterns in acoustofluidic devices significantly enhances the mixing by acoustic streaming around these features. The streaming patterns around the sharp edges are particularly effective for the mixing because they can produce strong lateral flows that rapidly homogenize liquids. This work presents extensive characterizations of the effect of sharp-edged structures on acoustic mixing in bulk acoustic wave (BAW) mode in a silicon microdevice. The effect of side wall patterns in different angles and shapes, their positions, the type of piezoelectric transducer, and its amplitude and frequency have been studied. Following the patterning of the channel walls, a mixing time of 25 times faster was reached, compared to channels with smooth side walls exhibiting conventional BAW behavior. The average locally determined acoustic streaming velocity inside the channel becomes 14 times faster if sharp corners of 10° are added to the wall.


Top: smartphone image of thermally treated hollow 3D printed complex lattice microarchitectures with sub-millimeter features. An untreated printed structure followed by thermally treated lattices in the air until 650 °C is shown. Bright-field microscope images of lattice structure cross-section for the (a) printed and annealed lattices at (b) 200, (c) 350, (d) 400, (e) 550, and (f) 650 °C. SEM images of the (a′) printed and calcined structures at (b′) 200, (c′) 350, (d′) 400, (e′) 550, and (f′) 650 °C. The yellow arrow highlights the inside opening of the hollow 3D network. EDX-mapping of half-beam cross-section: (g) merged image, single channels from left to right are Ti, Al, Si, P, and O. Scale bars in (g) represent 100 μm
(i–iv) Schematic representation of the 3D hollow network. SEM image of the beam surface of a hollow 3D printed lattice structure. The pink arrows highlight the contrast differences between TiO2 and carbon-rich materials. Thermally treated lattices in the air at (a) 200 °C, (a′) 350 °C, (a′′) 400 °C (a′′′) 550 °C, (a′′′′) 650 °C. SEM image of the TiO2 hollow lattice loaded with (b–b′′′) 2 wt% and (c–c′′′) 0.25 wt% α-Fe2O3. Yellow arrows highlight lattice structure openings and geometrical features. EDX-mapping of half-beam cross-section containing 2 wt% α-Fe2O3: (d) merged image, single channels from left to right are Ti, Al, Si, and Fe
(a)–(c) TEM images of the synthesized α-Fe2O3. XPS core spectrum of (d) Fe 2p, (d′) O 1s, and (d′′) P 2p for the synthesized α-Fe2O3. XPS core spectrum of (e and f) Ti 2p, (e′ and f′) O 1s, and (e′′ and f′′) P 2p in (e and e′′) TiO2 precursor and (f and f′′) TiO2 3DHMs loaded with 2 wt% α-Fe2O3. (g) The first derivative reflectance spectrum for TiO2 3DHMs (black), synthesized α-Fe2O3 (grey), and TiO2 3DHMs loaded with 0.5 wt% of α-Fe2O3 (green). Valence band determination for (h) TiO2 precursor (orange) and synthesized α-Fe2O3 (grey) and (i) TiO2 3DHM (black) and TiO2 3DHM loaded with 0.5 wt% α-Fe2O3 (green)
(a) MB degradation as a function of time for 3D microarchitectures composed of TiO2 and TiO2 loaded with 2, 1, 0.5, 0.25 wt% of α-Fe2O3. (b) Photo-Fenton degradation of MB for varied 3DHMs compositions. Controls include photolysis (Pho), photolysis in the presence of H2O2 (PhOx), adsorption of MB in the dark (Ads), and a TiO2 structure shaped as tabled without cellular geometries loaded with 0.5 wt% of α-Fe2O3 (TiOFe0.5P). (c) MB degradation as a function of time for TiOFe0.5. The 3DHM has been reused (R) three times (R1, R2, and R3). (d) Photo-Fenton reusability efficiencies using TiOFe0.5
(a) ACP degradation as a function of accumulated energy (QUV) without and for multiple scavengers like butanol, AgNO3, EDTA, and benzoquinone (˙OH, e⁻, h˙, and ˙O2⁻). (b) Solar photo-Fenton degradation of ACP for TiOFe0.5 3DHMs over time. (c) Kinetic of ACP degradation at 15 kJ m⁻² using the Langmuir–Hinshelwood (L–H) kinetic model. (d) Proposed ACP degradation mechanisms during solar photo-Fenton reaction using TiOFE0.5 3DHM
Additive manufacturing of hollow connected networks for solar photo-Fenton-like catalysis

October 2024

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86 Reads

A 3D-printing approach is used to fabricate green bodies/precursor microarchitectures that, upon annealing, allow the fabrication of hierarchical 3D hollow microarchitectures (3DHMs). The 3DHMs are composed mainly of TiO2 and inorganic stabilizers that enable the production of inorganic cellular units upon thermal annealing at 650 °C. Morphological inspection reveals that the 3D architecture beams comprise TiO2 nanoparticles (NPs). The inner and outer diameters of the hollow beams are ∼80 μm and ∼150 μm, retained throughout the 3D hollow network. A proof-of-concept photo-Fenton reaction is assessed. The 3DHMs are impregnated with α-Fe2O3 NPs to evaluate solar photo-Fenton degradation of organic compounds, such as MB used as control and acetaminophen, an organic pollutant. The optical, structural, and chemical environment characteristics, alongside scavenger analysis, generate insights into the proposed solar photo-Fenton degradation reaction over TiO2 3DHMs loaded with α-Fe2O3. Our work demonstrates newly hollow printed microarchitecture with interconnected networks, which can help direct catalytic reactions.


a) Metal‐organic photoresin composition. b) Two‐photon lithography (TPL) 3D printing of microarchitecture using an oil immersion objective. c) Thermal annealing: 3D‐printed pre‐ceramic microarchitecture (c.1) is treated through an annealing cycle at 600 °C (cycle 1) and shrinks into 3D ceramic microarchitecture (c.2), which exhibits no photoluminescence (PL). (c.2′) exhibits the same 3D ceramic microarchitecture (c.2), subjected to a second annealing cycle at 750 °C (cycle 2). (c.3) After cycle 2, PL‐promoted emission on the microarchitecture is observed.
Scanning electronic microscopy (SEM) images of Ln³⁺‐doped t‐ZrO2 microarchitectures. a) Undoped octet‐truss, b) Yb‐doped octet‐truss, c) undoped buckyball, and d) Yb‐doped buckyball are shown after 600 °C annealing (cycle 1). e) undoped octet‐truss, f) Yb‐doped octet‐truss, g) undoped buckyball, and h) Yb‐doped buckyball treated at 750° (cycle 2) are presented. SEM energy‐dispersive X‐ray spectroscopy (SEM–EDS) (i) merged image and single elemental map for j) Zr, k) O, and l) Yb are displayed. The scale bar represents 3 µm.
Transmission electron microscopy (TEM) images from focus ion beam (FIB) preparation of an octet‐truss annealed at 600 °C (a) and 750 °C (d). b,e) High‐magnification TEM images and c,f) corresponding fast Fourier transform (FFT) patterns.
Optical properties of octet‐truss treated at 750 °C. a) Raman spectra for t‐ZrO2 octet‐truss microarchitectures single‐doped, double‐doped, and triple‐doped with Yb (blue), Er (red), Tm (purple), YbEr (green), YbTm (yellow), YbErTm (light blue). b) Photoluminescence (PL) spectra for single Ln doping Yb (blue), Er (red), and Tm (purple). The Er (red) and Tm (purple) have been scaled to facilitate peak visualization. c) Proposed E diagram.
Photoluminescence (PL) spectra for double‐doped and triple‐doped t‐ZrO2 with octet‐truss microarchitecture treated at 750 °C: a) YbEr (green), b) YbTm (yellow), c) YbErTm (light blue). The YbErTm (light blue) has been scaled to facilitate peak visualization. d) Proposed energy transition diagram addressing ET and cross‐relaxation (CR) paths.
Temperature Promotes Photoluminescence in Lanthanide‐Doped 3D Ceramic Microarchitectures

September 2024

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83 Reads

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2 Citations

Two‐photon lithography (TPL) is a powerful technique for creating 3D microarchitectures. Applied to high‐refractive‐index materials like ZrO2, it promises advanced optics. This is the case of ZrO2 host matrixes in combination with luminescent dopants. However, due to the nonideal crystallinity attained to the TPL pre‐ceramic replica from a custom‐made photoresin, the emission of lanthanide (Ln) dopants in ZrO2 microarchitectures can be suboptimal. However, crystallinity exacerbated by annealing can promote Ln‐emission, thereby enabling the integration of ceramic micro‐optic into a low‐temperature process. This work presents a photoresin containing a metal‐organic monomer tailored for TPL, enabling the fabrication of Ln‐doped tetragonal ZrO2 (t‐ZrO2) microarchitectures. The emission properties of Ln‐doped microarchitectures with trivalent Ln ions (Ln³⁺), i.e., Yb³⁺ (2.5 mol%), Er³⁺ (0.35 mol%), and Tm³⁺ (0.35 mol%) are studied. The results demonstrate that Ln emission is absent when annealing the microarchitectures at 600 °C. Annealing at 750 °C activates Ln³⁺ emissions, including ²F5/2–²F7/2 (infrared), ⁴S3/2–⁴I15/2 (green), and ³H4–³F6 (near‐infrared) transitions corresponding to Yb, Er, and Tm species. Transmission electron microscopy (TEM) confirms that t‐ZrO2 crystallinity becomes more prominent at 750 °C, demonstrating the promotion of Ln emissions upon thermal treatment and underscoring the role of crystalline in TPL micro‐optical ceramics.


Figure 1. The acoustofluidic setup schematic, including the microchip and PZT transducer, is fixed in a PMMA holder.
Figure 2. The sharp corners are etched alongside the silicon microfluidic channel.
Figure 3. Resulting streaming velocity for a range of PZT devices and applied frequencies.
Figure 9. Z-stacking of particle movements in the channel with triangular pillars. The top-left image shows all the frames since the start of streaming and pumping on top of one another.
Figure 10. a) Z-stacking of particle movements in the channel with circular pillars. The top-left image is all the frames since the start of streaming and pumping on top of each other. b) A cross-section of an etched feature showing the scallop formation that causes circulation in the circular pillars (number 1 in the figure is 0.80 µ m and number 2 is 3.33 µ m).
Enhanced Acoustic Mixing in Silicon-Based Chips with Sharp-Edged Micro-Structures

September 2024

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27 Reads

The small dimensions of microfluidic channels allow for fast diffusive or passive mixing, which is beneficial for time-sensitive applications such as chemical reactions, biological assays, and the transport of to-be-detected species to sensors. In microfluidics, the need for fast mixing within milliseconds arises primarily because these devices are often used in fields where rapid and efficient mixing significantly impacts the performance and outcome of the processes. Active mixing with acoustics in microfluidic devices involves using acoustic waves to enhance the mixing of fluids within microchannels. Using sharp corners and wall patterns in acoustofluidic devices significantly enhances mixing by acoustic streaming around these features. The streaming patterns around sharp edges are particularly effective for mixing because they can produce strong lateral flows that rapidly homogenize liquids. This work presents extensive characterizations of the effect of sharp-edged structures on acoustic mixing in bulk acoustic wave (BAW) mode in a silicon microdevice. The effect of side wall patterns in different angles and shapes, their position, the type of piezoelectric transducer, and its amplitude and frequency have been studied. Following the patterning of the channel walls, a mixing time of 25 times faster was reached, compared to channels with smooth sidewalls exhibiting conventional BAW behavior. The average locally determined acoustic streaming velocity inside the channel becomes 14 times faster if sharp corners of 10° are added to the wall.


Fig. 1. Schematic illustrating a magnetically actuated device integrating a miniaturized fuel cell stack as an onboard power source, positioned within a static external magnetic field.
Fig. 2. Components and sizes of proton exchange membrane fuel cells (PEMFCs): (a) Schematic and experimental image of the components of a PEMFC; 1: end plate, 2: Viton gasket, 3: current collector, 4: flow field plate (FFP), 5: Teflon gaskets, 6: membrane electrode assembly (MEA), and 7: Teflon frame, (b) Relative sizes of MEAs and FFPs considered in the study.
Fig. 3. Schematic of the experimental setup. Operation of a PEMFC is characterised by a potentiostat. A PEM electrolyzer was used as the supply reactants to the PEMFC, at rates controlled by a source measurement unit.
Fig. 6. Performance characterization of PEMFCs with varying active areas. (a) I-E characteristics, and (b) the variation of output power of PEMFCs as a function of load current shown for PEMFCs of different active areas for I EL = 1 A.
Exploring PEMFCs for Powering Untethered Small-Scale Robots

September 2024

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163 Reads

Magnetically guided untethered devices are used in a variety of medical applications. These devices are typically powered by onboard battery units. Instead, a hydrogen fuel cell(FC) is a promising alternative power source for such small-scale devices as it relies on a sustainable fuel. They function as electric power sources by utilizing the redox reaction of hydrogen and oxygen, using a proton exchange membrane(PEM). Understanding the impact of reducing FC active area is crucial for deploying FCs in untethered devices and gaining insights into the challenges of downscaling the devices. This research investigates the performance of PEM FCs (PEMFCs)when their active area is reduced, and when the FC is supplied with reactants at different flow rates. PEMFCs with three active areas of electrodes, 3.5×3.5, 2.7×2.7, and 1.6×1.6 cm2were designed, fabricated, and characterised. Maximum fuel cell output powers of 0.3, 0.09, and 0.03 W (maximum power densities of 0.025, 0.012, and 0.012 W/cm2) were achieved, respectively. Mathematical modelling of the PEMFC simulated the FC response, providing insights into the activation kinetics of the fuel cell. In the context of small-scale magnetic actuation, the smallest PEMFC with an active area of 1.6×1.6 cm2 was used to power an inductor coil (rated 130 mA, 150 mH, 8 Ω).The resistive behavior of the coil was captured at a power of0.0277 W (0.0108 W/cm2).


Temperature Promotes Selectivity During Electrochemical CO2 Reduction on NiO:SnO2 Nanofibers

September 2024

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112 Reads

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2 Citations

Journal of Materials Chemistry A

Electrolyzers operate over a range of temperatures; hence, it is crucial to design electrocatalysts that do not compromise the product distribution unless temperature can promote selectivity. This work reports a synthetic approach based on electrospinning to produce NiO:SnO2 nanofibers (NFs) for selectively reducing CO2 to formate above room temperature. The NFs comprise compact but disjoined NiO and SnO2 nanocrystals identified with STEM. The results are attributed to the segregation of NiO and SnO2 confirmed with XRD. The NFs are evaluated for the CO2 reduction reaction (CO2RR) over various temperatures (25, 30, 35, and 40 °C). The highest Faradaic efficiencies to formate (FEHCOO-) are reached by NiO:SnO2 NFs containing 50% of NiO and 50% SnO2 (NiOSnO50NF), and 25% of NiO and 75% SnO2 (NiOSnO75NF), at an electroreduction temperature of 40 °C. At 40 °C, product distribution is assessed with in-situ differential electrochemical mass spectrometry (DEMS), identifying methane besides other products, like formate, hydrogen, and carbon monoxide, in the flow electrochemical cell. XPS and EELS unveiled the FEHCOO- variations due to a synergistic effect between Ni and Sn. DFT-based calculations reveal the superior thermodynamic stability and activity of Ni-containing SnO2 systems towards CO2RR over the pure oxide systems. Furthermore, computational surface Pourbaix diagrams showed that the presence of Ni as a surface dopant increases the reduction of the SnO2 surface and enables the production of formate. Our results highlight the synergy between NiO and SnO2, which can promote the electroreduction of CO2 at temperatures above room temperature.


A zero-gap silicon membrane with defined pore size and porosity for alkaline electrolysis

June 2024

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55 Reads

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1 Citation

Sustainable Energy & Fuels

Porous separators are a key component in alkaline water electrolyzers and are significant sources of overpotential. In this paper, porous silicon separators were fabricated by etching precise arrays of cylindrical pores into silicon substrates through lithography. Chemical stability of the silicon-based separators is ensured through the deposition of a silicon nitride layer. Platinum or nickel were vapor-deposited directly on the faces of the separator to complete a zero-gap configuration. Separator porosity (ε) was varied by changing the pore diameter and the pore spacing. These well-controlled porous silicon zero gap electrodes (PSi-ZGEs) were used to study the trade-off between separator resistance and gas-crossover at different porosities. It was found that separator resistances comparable to commercially used Zirfon UTP 500 at much lower ε. Gas crossover remained within the explosive limits for ε ≤ 0.15 %. In the broad perspective, the current work can pave the path for the development of ionomer-free separators for alkaline water electrolysis which rely on the separator geometry to limit gas-crossover. The PSi-ZGEs achieved stable performance at 100 mA/cm2 for 24 hours without significant surface damage in the alkaline electrolyte


Citations (55)


... TPL uses focused femtosecond laser pulses, triggering localized photopolymerization within a photoresin containing inorganic salts and photoinitiator, allowing tenth-of-nanometer voxel-level control over features in intricate pre-ceramic architectures (i.e., metal-organic printed microarchitectures) [21]. The adaptability of photoresin composition in TPL is essential to achieving glass and ceramics with tailored optical properties, enabling applications in photonics, micro-optics, and functional microdevices [22]. ...

Reference:

Yb3+-Mediated Luminescence Enhancement in Er3+-Doped 3D-Printed ZrO2 Microarchitectures
From Single to Multi‐Material 3D Printing of Glass‐Ceramics for Micro‐Optics

... While traditional methods like solid-state reactions and sol-gel techniques are effective for bulk materials, they lack the precision to produce doped 3D arbitrary complex designs [14][15][16]. Recently, we reported suboptimal doping to limit Ln³⁺ emission in co-doped systems with 3D complex designs made by two-photon lithography and subsequent annealing steps [17]. In the case of Yb 3+ and Er 3+ co-dopants, Yb³⁺ can act as a sensitizer, transferring energy to Er³⁺, enabling visible emissions of value in lasers and energy transfer devices [18]. ...

Temperature Promotes Photoluminescence in Lanthanide‐Doped 3D Ceramic Microarchitectures

... Among host materials, zirconium dioxide (ZrO₂) stands out for its wide band gap (4-4.5 eV), broad transparency range (spanning from ultraviolet to mid-infrared), and low phonon energy (~470 cm⁻¹) [7]. ZrO₂ exists in multiple crystallographic phases, such as monoclinic (m-ZrO₂) and tetragonal (t-ZrO₂), with characteristic luminescence mainly originated by defects [8]. At room temperature and ambient pressure, the monoclinic phase is the most stable, while the tetragonal phase can be stabilized through doping with aliovalent ions or by reducing crystallite size below ~30 nm to lower surface energy [9]. ...

Additive Manufacturing of Zn‐Doped ZrO2 Architectures

... In contrast, for the 30 and 35 µL precursor volumes, a noticeable decline in peak intensity was observed relative to the 25 µL concentration. This suggests the onset of agglomeration phenomena affecting the Au NPs as the precursor concentration exceeded optimal levels [40]. Thus, the findings indicate that the substrate synthesized with a precursor volume of 25 µL produced the highest level of signal enhancement, establishing it as the most effective formulation for SERS applications. ...

Alternative Nano-lithographic Tools for Shell-Isolated Nanoparticle Enhanced Raman Spectroscopy Substrates

Nanoscale

... Because reductive reactions are driven at applied potential, the use of external reducing agents such as H 2 will be avoided [49]. As shown in Fig. 4, the formation of amino acids follows two possible pathways: one is the reaction of keto acids with ammonia to generate imines, which undergoes a two-electron reduction to give amino acids; the other is the initial formation of oximes, followed by a fourelectron reduction on the cathode [50][51][52]. During the electro-reduction process, hydrogen evolution reaction (HER) and the reduction of keto-to hydroxyl-group may occur and compete with the reductive amination. ...

Alanine Formation in a Zero‐Gap Flow Cell and the Role of TiO2/Ti Electrocatalysts

... The temperature within the catalytic combustion chamber is regulated using electric heating, and a first-order inertial lagging link is utilized to describe the mathematical model of the temperature environment [45][46][47], where its transfer function is: ...

Enhanced Performance of an Acoustofluidic Device by Integrating Temperature Control

... The spatial structure has a crucial impact on the function of macrophages and fibroblasts [26]. Based on the 2D co-culture, this study also used a 3D co-culture model, which can further simulate the regulation of infiltration and interaction between macrophages and CFs (Fig. 6a). ...

3D topographies promote macrophage M2d-Subset differentiation

Materials Today Bio

... 。 气泡生长可能会经历扩散控制和化学反应控制, 也可能只经历一种。 是扩散控制还是化学反应控制是由电极的活化面积决定的。 许多调控方式被用于 改善气泡的生长和脱离模式。通过表面工程,构建超亲水电极能减小电极与气泡 之间的粘附力, 能促进气泡脱离 [5] 。 纳米阵列电极表现出加速的气泡生长动力学, 具有高的时间系数、 最小的气泡分离尺寸和最短的分离时间。 磁场 [6,7] , 超声场 [8] , 压力的改变 [9,10] 也会加速气泡的演化,增强溶液中的质量传递,改善反应动力学。 然而,通过这种主动调控的方式需要消耗额外的能量,可能会增加电解水的成本 和复杂性。电解质的特性,如溶质的类型 [11] 和 pH [12,13] 会影响作用于气泡的离子 浓度 Marangoni 力从而影响气泡的脱离。氢气泡脱离模式取决于电解液中阴离子 的霍夫迈斯特序列。一些学者也通过构建活性位点诱导气泡聚并 [14,15] ,显著了提 高反应动力学,将平均电流提高了 2.4 倍。尽管有关气泡演化的许多实验有趣且 巧妙,然而由于实验的局限性,获取气泡的周围的物理场的分布的详细信息具有 较大的难度。 为了揭示电解液中的传质和流动特性, 一些研究使用有限元方法对电解水中 的气泡进行了数值模拟。Liu 等人 [16] 通过 VOF 方法模拟了气泡的演化,揭示了 气泡生长过程中的浓度分布。然而,由于气液界面通过气体体积分数区分,因此 无法准确描述气泡的边界和气泡与电解液之间的相互作用。Meulenbroek 等人 [17] 数值模拟了铂微电极上的氢气泡周围的热 Marangoni 对流和浓度 Marangoni 对 流,揭示了气泡界面顶部停滞的起源。Zhan 等人 [18] 对不同生长情况的气泡直径 进行稳态模拟,发现电解液的焦耳热主要在电极表面的微层内产生,并根据模拟 得到的多物理场参数改进了预测气泡脱离直径的力平衡模型。Raman 等人 [19] ...

Investigating mass transfer around spatially-decoupled electrolytic bubbles
  • Citing Article
  • October 2023

Chemical Engineering Journal

... The 3D ZrO₂ microarchitectures can be fabricated at the highest definition using additive manufacturing (AM), also known as 3D printing. AM methods include two-photon lithography (TPL), which provides tenths of nanometer control over micrometer-size luminescent microarchitecture features [11,19,20]. TPL uses focused femtosecond laser pulses, triggering localized photopolymerization within a photoresin containing inorganic salts and photoinitiator, allowing tenth-of-nanometer voxel-level control over features in intricate pre-ceramic architectures (i.e., metal-organic printed microarchitectures) [21]. ...

3D‐Architected Alkaline‐Earth Perovskites

... The functionality of the most active 3DHMs (i.e., TiOFe0.5) is assessed for acetaminophen (ACP), an emerging organic pollutant that has come to the forefront of environmental issues. 59, 60 We also provide insights into the photo-Fenton degradation mechanism under natural solar light. For such purpose, the inuence of radical scavengers on ACP solar photo-Fenton degradation is assessed, and the results are shown in Fig. 5a and b. ...

Acetaminophen oxidation under solar light using Fe-BiOBr as a mild Photo-Fenton catalyst

Journal of Photochemistry and Photobiology A Chemistry