Performance optimization of a microwave-coupled plasma-based ultralow-energy ECR ion source for silicon nanostructuring

• Joy Mukherjee,
• Safiul Alam Mollick,
• Tanmoy Basu and
• Tapobrata Som

Beilstein J. Nanotechnol. 2025, 16, 484–494, doi:10.3762/bjnano.16.37

• treatments such as nanopatterning, sputter etching, and controlled defect formation [6][7]. Particularly, ultralow-energy ion beams are exceptionally valuable for the precise modification of 2D layers [8] and ion-induced nanopatterning of semiconductor surfaces [9]. Over the past few decades, ion-induced

Impact of adsorbate–substrate interaction on nanostructured thin films growth during low-pressure condensation

• Alina V. Dvornichenko,
• Vasyl O. Kharchenko and
• Dmitrii O. Kharchenko

Beilstein J. Nanotechnol. 2025, 16, 473–483, doi:10.3762/bjnano.16.36

• , even for monoatomic layers [34]. The patterns may serve as templates for the later evolution of film textures. Relevant examples of such systems are Al or Cu layers deposited on Si substrates, or SiO2 and TiN layers deposited on Ti or Al substrates [31]. In this article, we perform a computational

• structures. In the general case, the reaction–diffusion equation for the field x1(r,t) has the form The reaction term R(x1,x2) is responsible for adsorption, desorption, and diffusion of adatoms between neighbor layers. The adsorbate flow J is defined through the free energy ℱ of the adsorbed layer Here, D0

• − x1)(1 − x2), where the adsorption rate ka = ωpexp(−Ea/kBT) is defined through the adsorption energy Ea, the frequency factor ω, and the pressure of the gaseous phase p; kB is the Boltzmann constant; T is the temperature. They require free sites on both first (1 − x1) and second (1 − x2) layers. The

Graphene oxide–chloroquine conjugate induces DNA damage in A549 lung cancer cells through autophagy modulation

• Braham Dutt Arya,
• Sandeep Mittal,
• Prachi Joshi,
• Alok Kumar Pandey,
• Jaime E. Ramirez-Vick,
• Govind Gupta and
• Surinder P. Singh

Beilstein J. Nanotechnol. 2025, 16, 316–332, doi:10.3762/bjnano.16.24

• mL of H2SO4 (98%) which intercalates between graphitic layers. Finely powdered KMnO4 (1.5 g) was slowly added (time span ≈30 min) to the reaction mixture under continuous stirring at 4 °C in an ice bath (0–5 °C). The reaction mixture was kept under vigorous stirring for 12 h at room temperature

• which could suggest the formation of nearly mono- or few layers of GO nanosheets. These spectroscopic and morphological results were in good agreement with our previous observations [25]. Quantitative estimation of Chl binding onto GO nanosheets The amount of Chl bound onto GO sheets was estimated in

Enhancing mechanical properties of chitosan/PVA electrospun nanofibers: a comprehensive review

• Nur Areisman Mohd Salleh,
• Amalina Muhammad Afifi,
• Fathiah Mohamed Zuki and
• Hanna Sofia SalehHudin

Beilstein J. Nanotechnol. 2025, 16, 286–307, doi:10.3762/bjnano.16.22

• release time of substances by exploiting the surface properties and interactions between hydrophobic and hydrophilic layers [86]. This sequential method of producing composite fibers is generally easier than the other methods as the different materials are electrospun separately, eliminating concerns

• layers. Rafieian et al. [109] incorporated PVA nanofibers onto chitosan/aloe vera films to improve the mechanical, physical, and biological properties of the films for wound dressing applications. Kim et al. [159] compared the mechanical properties of pure PVA, blended chitosan/PVA, and PVA core–chitosan

Emerging strategies in the sustainable removal of antibiotics using semiconductor-based photocatalysts

• Yunus Ahmed,
• Keya Rani Dutta,
• Parul Akhtar,
• Md. Arif Hossen,
• Md. Jahangir Alam,
• Obaid A. Alharbi,
• Hamad AlMohamadi and
• Abdul Wahab Mohammad

Beilstein J. Nanotechnol. 2025, 16, 264–285, doi:10.3762/bjnano.16.21

• tungstate (Bi2WO6) is also an n-type semiconductor that belongs to the Aurivillius phases. The material exhibits two distinct crystallographic phases, namely monoclinic and orthorhombic. Orthorhombic Bi2WO6 has alternating layers of (Bi2O2)2+ and WO6 octahedrons. It comprises perovskite layers and has a

Radiosensitizing properties of dual-functionalized carbon nanostructures loaded with temozolomide

• Radmila Milenkovska,
• Nikola Geskovski,
• Dushko Shalabalija,
• Ljubica Mihailova,
• Petre Makreski,
• Dushko Lukarski,
• Igor Stojkovski,
• Maja Simonoska Crcarevska and
• Kristina Mladenovska

Beilstein J. Nanotechnol. 2025, 16, 229–251, doi:10.3762/bjnano.16.18

• of the CNTs; the bands from the Raman modes that result from the vibration of all carbon atoms in the CNTs; and the 2D band occurring between 2600 and 2800 cm−1, which is sensitive to the number of graphene layers and their arrangement. The intensity ratio between the D and the G band was analyzed

• the successful introduction of functional groups on their surfaces, that is, chemical modification of their outer layers [62]. The spectra of covalently functionalized MWCNTs-G with PEG6000 follow this behavior and are also accompanied by a broadening of the G band. The broadening and its intensity

Recent advances in photothermal nanomaterials for ophthalmic applications

• Jiayuan Zhuang,
• Linhui Jia,
• Chenghao Li,
• Rui Yang,
• Jiapeng Wang,
• Wen-an Wang,
• Heng Zhou and
• Xiangxia Luo

Beilstein J. Nanotechnol. 2025, 16, 195–215, doi:10.3762/bjnano.16.16

• effectively absorb NIR radiation and convert it into heat, thus activating the hydrogel to generate sol–gel transformation, and achieving on-demand drug release. Drugs such as timolol maleate and levofloxacin were encapsulated within separate layers of the hydrogel, facilitating a sustained, stepwise release

• -specific hypotony, or high IOP resulting from tissue fibrosis [138][139][140][141]. To address this, photothermal shape memory polymers (SMPs) have been employed to program and control the inner diameter of the drainage tubes (Figure 5b) [133]. These SMP silica gel drainage tubes consist of three layers

A review of metal-organic frameworks and polymers in mixed matrix membranes for CO₂ capture

• Charlotte Skjold Qvist Christensen,
• Nicholas Hansen,
• Mahboubeh Motadayen,
• Nina Lock,
• Martin Lahn Henriksen and
• Jonathan Quinson

Beilstein J. Nanotechnol. 2025, 16, 155–186, doi:10.3762/bjnano.16.14

• precursor slurry undergoes phase separation under altered solvent, composition, or temperature conditions to form a porous support phase and a dense MMM phase [80][87][92][94]. Finally, fabrication of thin selective MMM layers on top of porous substrates can be accomplished via spin coating [95]. Defects

• layers are formed, decreasing the mass transfer resistance and increasing the gas permeation flux. Sutrisna et al. [98] fabricated a novel HFMMM consisting of an inner polyvinylidenfluorid (PVDF) porous support dip-coated with a highly permeable poly(1-trimethylsilyl-1-propyne) (PTMSP) gutter layer, a

• Pebax® 1657-based selective layer containing UiO-66, and a top pure Pebax® 1657 protective layer, illustrated in Figure 5. The thickness of the Pebax® layers reached 1.0–1.5 μm, and the tensile strength of the MOF-loaded membrane was comparable to that of the composite membrane with a pure Pebax® layer

Clays enhanced with niobium: potential in wastewater treatment and reuse as pigment with antibacterial activity

• Silvia Jaerger,
• Patricia Appelt,
• Mario Antônio Alves da Cunha,
• Fabián Ccahuana Ayma,
• Ricardo Schneider,
• Carla Bittencourt and
• Fauze Jacó Anaissi

Beilstein J. Nanotechnol. 2025, 16, 141–154, doi:10.3762/bjnano.16.13

• stretching and bending of Si–O present in the clay layers [7]. The spectra for Nb2O5 and NbOPO4 and the bentonite modified with niobium before and after adsorption/photocatalysis present an intense band in the region of 630 cm−1 related to the stretching of the Nb–O bond. The A-BEPh, A-BEPhP, A-BEOx, and A

TiO₂ immobilized on 2D mordenite: effect of hydrolysis conditions on structural, textural, and optical characteristics of the nanocomposites

• Marina G. Shelyapina,
• Rosario Isidro Yocupicio-Gaxiola,
• Gleb A. Valkovsky and
• Vitalii Petranovskii

Beilstein J. Nanotechnol. 2025, 16, 128–140, doi:10.3762/bjnano.16.12

• cetyltrimethylammonium bromide (CTAB) layers. The latter method involves the synthesis of layered 2D zeolites in the presence of CTAB and organic structure directing agents (OSDAs), followed by calcination to remove them from the resulting products [1]. The choice of the OSDA determines not only the interlamellar

• hybrid zeolite–CTAB aggregates, inorganic pillars are pre-formed in the CTAB layers, which will keep the zeolite lamellae from collapsing when burning the organic phase. The flexibility in the choice of material to form pillars creates a wide range of potential new materials for targeted applications

• . Typically, such pillars are amorphous SiO2 nanoparticles formed during the hydrolysis of tetraethoxysilane (TEOS) introduced into liquid crystalline 2D CTAB layers that fill the interlamellar space between the 2D zeolite nanosheets. Tetraethoxytitanium (TEOT) is a homolog of TEOS, and its hydrolysis

Comparison of organic and inorganic hole transport layers in double perovskite material-based solar cell

• Deepika K and
• Arjun Singh

Beilstein J. Nanotechnol. 2025, 16, 119–127, doi:10.3762/bjnano.16.11

• , that is, La2NiMnO6 (LNMO), is studied with the organic and inorganic hole transport layers (HTLs) Cu2O and PEDOT:PSS. Our study yields a significant improvement in the power conversion efficiency (PCE) of perovskite solar cells with two types of HTLs. The optimized devices achieved a maximum PCE of

• 2009 to 26.1% in 2023 [5][6]. PSCs consist of an absorber layer sandwiched between charge transport layers (CTLs), that is, the hole transport layer (HTL) and the electron transport layer (ETL). Light generates excitons, which further dissociate into electrons and holes. The electrons and holes are

• passivation, efficiencies of 20.8% for Cs0.05(FA0.90MA0.10)0.95Pb(I0.90Br0.10)3, 18.9% for MAPbI3, and 18.7% for FAPbI3 perovskite layers were observed under ambient conditions and illumination for over 900 h. Mohammed et al. [9] optimized triple-cation PSCs that maintained 83% of the efficiency after 1600 h

Characterization of ZnO nanoparticles synthesized using probiotic Lactiplantibacillus plantarum GP258

• Prashantkumar Siddappa Chakra,
• Aishwarya Banakar,
• Shriram Narayan Puranik,
• Vishwas Kaveeshwar,
• C. R. Ravikumar and
• Devaraja Gayathri

Beilstein J. Nanotechnol. 2025, 16, 78–89, doi:10.3762/bjnano.16.8

• . When ingested in sufficient quantities, they provide health advantages as they colonize the gut, and their metabolites generally show antimicrobial and health promotion activity to the host [6][7][8]. The thick peptidoglycan layers with crosslinks and the complex cell wall structures of Gram-positive

Bioinspired nanofilament coatings for scale reduction on steel

• Siad Dahir Ali,
• Mette Heidemann Rasmussen,
• Jacopo Catalano,
• Christian Husum Frederiksen and
• Tobias Weidner

Beilstein J. Nanotechnol. 2025, 16, 25–34, doi:10.3762/bjnano.16.3

• strongly to the steel surface and individual crystals coalesce to form larger, continuous scale layers. While it is unclear how, in detail, an SNF coating can affect the scale growth process, we hypothesize that the flow characteristics near the surface play an important role. While at regular solid–liquid

Orientation-dependent photonic bandgaps in gold-dust weevil scales and their titania bioreplicates

• Norma Salvadores Farran,
• Limin Wang,
• Primoz Pirih and
• Bodo D. Wilts

Beilstein J. Nanotechnol. 2025, 16, 1–10, doi:10.3762/bjnano.16.1

• template has a similar refractive index as the titania thin layers obtained with a sol–gel process, suggesting a similar porosity despite the more complicated geometry. The work further supports the use of biological photonic structures for synthesizing novel optical devices. Results Appearance and

Attempts to preserve and visualize protein corona on the surface of biological nanoparticles in blood serum using photomodification

• Julia E. Poletaeva,
• Anastasiya V. Tupitsyna,
• Alina E. Grigor’eva,
• Ilya S. Dovydenko and
• Elena I. Ryabchikova

Beilstein J. Nanotechnol. 2024, 15, 1654–1666, doi:10.3762/bjnano.15.130

• efforts of many researchers are aimed at finding approaches and methods for “managing” the composition of the protein corona, which, in particular, can provide the possibility of targeted delivery of drugs [1][2][3]. The protein corona is formed by two layers on any NP, called the hard and soft coronas

• layered (Figure 2d3). Then, 2 mL of 10% intact FBS or NBS were applied on top of the resulting gradient and underwent UC for 18 h at 4 °C (Ultracentrifuge L8-70M, rotor SW-40, 100,000g). The layers were then separated; each was diluted with PBS to 14 mL and underwent UC again for 2 h, to clear from

Fabrication of hafnium-based nanoparticles and nanostructures using picosecond laser ablation

• Abhishek Das,
• Mangababu Akkanaboina,
• Jagannath Rathod,
• R. Sai Prasad Goud,
• Kanaka Ravi Kumar,
• Raghu C. Reddy,
• Ratheesh Ravendran,
• Katia Vutova,
• S. V. S. Nageswara Rao and
• Venugopal Rao Soma

Beilstein J. Nanotechnol. 2024, 15, 1639–1653, doi:10.3762/bjnano.15.129

• ][41][43]. The decomposed surrounding liquid has a carbon-rich environment. As the polycrystals grow, they also act as a nucleus for carbon atoms to self-assemble [27][50], forming graphite layers and, eventually, core–shell NPs of different sizes. This formation of graphite layers might prevent the

Biomimetic nanocarriers: integrating natural functions for advanced therapeutic applications

• Hugo Felix Perini,
• Beatriz Sodré Matos,
• Carlo José Freire de Oliveira and
• Marcos Vinicius da Silva

Beilstein J. Nanotechnol. 2024, 15, 1619–1626, doi:10.3762/bjnano.15.127

• cellular membranes and carriers is coextrusion through polyester or polycarbonate membranes with various pore sizes [51][52]. In this method, mechanical extrusion forces the nanocarriers into the membrane vesicles. This approach yields product uniformity and preserves membrane protein layers, though it

Natural nanofibers embedded in the seed mucilage envelope: composite hydrogels with specific adhesive and frictional properties

• Agnieszka Kreitschitz and
• Stanislav N. Gorb

Beilstein J. Nanotechnol. 2024, 15, 1603–1618, doi:10.3762/bjnano.15.126

• . Macroscopically observable mucilage is often a transparent, gel-like capsule formed around the diaspore after hydration with water (Figure 1). At the microscale mucilage exhibits, before hydration, successive layers formed by adcrustation in the mucilaginous cells of the seed/fruit coat (the outermost covering of

• of the mucilage – from pressed layers to a 3D network Substances with gel character (slime, mucus, and mucilage) are ubiquitous in nature and are produced by diverse organisms such as bacteria, plants representing diverse groups (algae, ferns, and higher plants), and animals (fishes, frogs, and

• hydration [8][22][38]. Mucilage, which is produced by the mucilaginous cells of diaspores in a form of densely packed layers, has the ability of loosening its structure after hydration into an easily accessible 3D fibrillar network [7][13][14][39] (Figure 3 and Figure 4 below). One of the key components of

Ultrablack color in velvet ant cuticle

• Vinicius Marques Lopez,
• Wencke Krings,
• Juliana Reis Machado,
• Stanislav Gorb and
• Rhainer Guillermo-Ferreira

Beilstein J. Nanotechnol. 2024, 15, 1554–1565, doi:10.3762/bjnano.15.122

• spines and setae (Figure 4). The setae display nanostructures in the form of grooves and are hollow (Figure 4D). No morphological distinction was observed between white and black setae (Figure 4A). The cuticle is composed of overlapping lamellae with connective pillars and underlying layers (Figure 5

•  5) are integral to the structures represented in Figure 6, where setae and lamellae likely enhance light absorption through multiple scattering and increased path length as light interacts with the cuticular protrusions and lamellar layers. Additionally, iterative scattering and absorption occur

Integrating high-performance computing, machine learning, data management workflows, and infrastructures for multiscale simulations and nanomaterials technologies

• Fabio Le Piane,
• Mario Vozza,
• Matteo Baldoni and
• Francesco Mercuri

Beilstein J. Nanotechnol. 2024, 15, 1498–1521, doi:10.3762/bjnano.15.119

• multiscale materials development pipeline (Figure 8). The general structure of this framework is based on a set of interfaces and different abstraction layers. General user queries, related to use cases, are translated into tasks and workflows, returning advice and support to decision making [60]. The

Polymer lipid hybrid nanoparticles for phytochemical delivery: challenges, progress, and future prospects

• Iqra Rahat,
• Pooja Yadav,
• Aditi Singhal,
• Mohammad Fareed,
• Jaganathan Raja Purushothaman,
• Mohammed Aslam,
• Raju Balaji,
• Sonali Patil-Shinde and
• Md. Rizwanullah

Beilstein J. Nanotechnol. 2024, 15, 1473–1497, doi:10.3762/bjnano.15.118

• , phospholipids help to form a carrier-like structure, which is an integral part of the system. In addition, the modification of lipoidal layers with a PEG chain provides flexibility to the nanocarrier. The ratio of the polymer and lipid can easily be adjusted to modulate the physicochemical characteristics of

Lithium niobate on insulator: an emerging nanophotonic crystal for optimized light control

• Midhun Murali,
• Amit Banerjee and
• Tanmoy Basu

Beilstein J. Nanotechnol. 2024, 15, 1415–1426, doi:10.3762/bjnano.15.114

• and hybrid devices with combined functionalities [16]. We focus on the DBR structure out of lithium niobate. To achieve PhC effects, one of the ways is creating alternating layers of LN and another material with a contrasting refractive index. We chose TiO2 and SiO2 as it has a considerable difference

• transferred onto a DBR structure consisting of 11 layers of SiO2/Ta2O5. The optimized design of the DBR effectively suppresses the leakage of acoustic energy [33]. Superradiance describes a collective effect where excited atoms or molecules emit light much faster than they would individually [33][34]. This

• photonic band could be tuned for specific for real applications. Methodology The reflectance of the multilayer stack was evaluated by simulating it in COMSOL Multiphysics. Lithium niobate (n = 2.21) is placed in odd layers while TiO2 (n = 2.6) is in even layers. Figure 1 shows alternating PhC layers of LN

A biomimetic approach towards a universal slippery liquid infused surface coating

• Ryan A. Faase,
• Madeleine H. Hummel,
• AnneMarie V. Hasbrook,
• Andrew P. Carpenter and
• Joe E. Baio

Beilstein J. Nanotechnol. 2024, 15, 1376–1389, doi:10.3762/bjnano.15.111

• surface coatings based on the slick surfaces of carnivorous pitcher plants (Nepenthes), termed slippery liquid-infused porous surfaces (SLIPS). This study introduces a simplified method to produce SLIPS using a polydopamine (PDA) anchor layer, inspired by mussel adhesion. SLIPS layers were formed on

• about the presence and ordering of specific chemical groups within the substrate–PDA–FDT layers was provided by SFG spectra collected from the COC–PDA–FDT sample (Figure 4). The stretching region between 1100 and 1850 cm−1 contains modes related to specific molecular groups within each layer of the

Out-of-plane polarization induces a picosecond photoresponse in rhombohedral stacked bilayer WSe₂

• Guixian Liu,
• Yufan Wang,
• Zhoujuan Xu,
• Zhouxiaosong Zeng,
• Lanyu Huang,
• Cuihuan Ge and
• Xiao Wang

Beilstein J. Nanotechnol. 2024, 15, 1362–1368, doi:10.3762/bjnano.15.109

• , bilayer WSe2 can be divided into 3-rhombohedral (3R) and 2-hexagonal (2H) phases [24][26][38]. When two layers are stacked antiparallel, bilayer WSe2 exhibits a hexagonal stacked (H-stacked) structure with inversion symmetry. In contrast, artificially stacking two layers in parallel to form a rhombohedral

•  1a). In contrast, the BA stacking order, opposite to AB, induces upward polarization (Figure S1a). The transition between AB and BA stacking orders can be accomplished through the interlayer sliding of adjacent WSe2 layers. To further investigate the OOP polarization in 3R WSe2, we prepared the

• contrast, and characterized by photoluminescence (PL) measurements at room temperature (see Supporting Information File 1, Figure S3). The relative angles between crystalline axes of the top and bottom WSe2 layers were determined by polarization-resolved SHG measurements. The zigzag directions of the two

Investigation of Hf/Ti bilayers for the development of transition-edge sensor microcalorimeters

• Victoria Y. Safonova,
• Anna V. Gordeeva,
• Anton V. Blagodatkin,
• Dmitry A. Pimanov,
• Anton A. Yablokov and
• Andrey L. Pankratov

Beilstein J. Nanotechnol. 2024, 15, 1353–1361, doi:10.3762/bjnano.15.108

• compared to the full-size films. This is because at the edges of the structure, the film thickness may differ from that at the center. Smooth edges are also necessary for good contact with subsequent layers. For this reason, special attention is paid to the development of technology for creating structures