Automated collection and categorisation of STM images and STS spectra with and without machine learning

• Dylan Stewart Barker and
• Adam Sweetman

Beilstein J. Nanotechnol. 2025, 16, 1367–1379, doi:10.3762/bjnano.16.99

• results [4][5][6][7]. STS measurements are the result of an integration over the available density of states (DOS) in both the tip and the sample, with the current measured therefore being proportional to the convolution of two. To isolate the DOS of the sample, it is crucial that the tip has a nominally

• for 30 min, measuring a drain current of ≈7.0 μA, before annealing at 500 °C for 30 min and then placed into the scan head for imaging. Platinum–iridium STM tips were used throughout this work and were prepared by standard STM methods (voltage pulses, controlled contacts with the sample) until good

• the tip–sample distance constant throughout the spectroscopy measurement. The voltage is then swept through a range of values whilst measuring the current, which is obtained as a function of the varying voltage, I(V). This curve can then be differentiated with respect to the voltage to obtain the

Enhancing the therapeutical potential of metalloantibiotics using nano-based delivery systems

• Alejandro Llamedo,
• Marina Cano,
• Raquel G. Soengas and
• Francisco J. García-Alonso

Beilstein J. Nanotechnol. 2025, 16, 1350–1366, doi:10.3762/bjnano.16.98

• targets, discuss current advancements in encapsulation methods, and examine the efficacy of encapsulated metalloantibiotics. Finally, we consider the challenges and future directions for the integration of metalloantibiotic-loaded carriers in the fight against antibiotic-resistant infections. Keywords

• in discovering new active antimicrobial compounds, as the current pipeline is incapable of addressing the urgency of this issue [8]. This concern has also been echoed in recent analyses evaluating AMR trends and antibiotic development strategies [9]. Most of the antibiotics currently in clinical

Ferroptosis induction by engineered liposomes for enhanced tumor therapy

• Alireza Ghasempour,
• Mohammad Amin Tokallou,
• Mohammad Reza Naderi Allaf,
• Mohsen Moradi,
• Hamideh Dehghan,
• Mahsa Sedighi,
• Mohammad-Ali Shahbazi and
• Fahimeh Lavi Arab

Beilstein J. Nanotechnol. 2025, 16, 1325–1349, doi:10.3762/bjnano.16.97

• to high disability and mortality, and the exact mechanisms are still unclear. Current chemotherapy faces challenges, including non-specificity, toxicity to healthy cells, the development of stem-like cells, and the progression of multidrug resistance [1]. Drug resistance is a major obstacle in cancer

Deep-learning recognition and tracking of individual nanotubes in low-contrast microscopy videos

• Vladimir Pimonov,
• Said Tahir and
• Vincent Jourdain

Beilstein J. Nanotechnol. 2025, 16, 1316–1324, doi:10.3762/bjnano.16.96

• the performance comparable to the current state-of-the-art models [28]. Expanding the dataset to include more diverse video quality and nanotube localization can lead to more stable models [29]. Moreover, replacing computationally demanding models like Mask-RCNN with smaller models could enhance

Wavelength-dependent correlation of LIPSS periodicity and laser penetration depth in stainless steel

• Nitin Chaudhary,
• Chavan Akash Naik,
• Shilpa Mangalassery,
• Jai Prakash Gautam and
• Sri Ram Gopal Naraharisetty

Beilstein J. Nanotechnol. 2025, 16, 1302–1315, doi:10.3762/bjnano.16.95

• wavelength remains not fully understood, despite numerous studies on this topic. The most puzzling aspect of our current results is the decrease in the periodicity of LIPSS after irradiation with wavelengths beyond 2000 nm. Further experiments and theoretical studies are necessary to develop a precise model

• by the scanning range of the instruments, offering a facile method for industrial applications. Our findings revealed that the periodicity of LIPSS increased with the laser wavelength up to 2000 nm, followed by a decrease at 2200 and 2400 nm. Current theories and mechanisms could not explain this

Enhancing the photoelectrochemical performance of BiOI-derived BiVO₄ films by controlled-intensity current electrodeposition

• Huu Phuc Dang,
• Khanh Quang Nguyen,
• Nguyen Thi Mai Tho and
• Tran Le

Beilstein J. Nanotechnol. 2025, 16, 1289–1301, doi:10.3762/bjnano.16.94

• Abstract This study investigates the fabrication of BiVO4 photoanodes using a controlled-intensity current electrodeposition method to improve their photoelectrochemical (PEC) performance. The impact of varying the deposition current density and VO(acac)2 concentration was systematically analyzed to

• , representing a significant enhancement compared to the other samples. The surface hole injection efficiency was measured to be 47%, whereas the incident photon-to-current efficiency reached a peak of 18.1% at 420 nm. The applied bias photon-to-current efficiency of BiVO4(326) was also superior to that of the

• samples fabricated with lower current density, highlighting the benefits of the optimized electrodeposition conditions for the former. Keywords: BiOI; BiVO4; electrodeposition; photoelectrochemical water splitting; Introduction In the context of the increasing global energy demand, the development of

Better together: biomimetic nanomedicines for high performance tumor therapy

• Imran Shair Mohammad,
• Gizem Kursunluoglu,
• Anup Kumar Patel,
• Hafiz Muhammad Ishaq,
• Cansu Umran Tunc,
• Dilek Kanarya,
• Mubashar Rehman,
• Omer Aydin and
• Yin Lifang

Beilstein J. Nanotechnol. 2025, 16, 1246–1276, doi:10.3762/bjnano.16.92

• integrating nature-inspired architectures, these smart, multifunctional biomimetic nanoparticles offer a promising path to overcome current therapeutic challenges and revolutionize precision oncology. Review 1 Types of biomimetic nanoparticles 1.1 Cell membrane-camouflaged nanoparticles Cell membranes have

Functional bio-packaging enhanced with nanocellulose from rice straw and cinnamon essential oil Pickering emulsion for fruit preservation

• Tuyen B. Ly,
• Duong D. T. Nguyen,
• Hieu D. Nguyen,
• Yen T. H. Nguyen,
• Bup T. A. Bui,
• Kien A. Le and
• Phung K. Le

Beilstein J. Nanotechnol. 2025, 16, 1234–1245, doi:10.3762/bjnano.16.91

• cosmetic industries. The current major gaps in research regarding these biopackaging materials are their low mechanical strength and the introduction of functional additives to enhance their range of applications. In this paper, a biopackaging material is formulated using polyvinyl alcohol with glycerol as

Hydrogels and nanogels: effectiveness in dermal applications

• Jéssica da Cruz Ludwig,
• Diana Fortkamp Grigoletto,
• Daniele Fernanda Renzi,
• Wolf-Rainer Abraham,
• Daniel de Paula and
• Najeh Maissar Khalil

Beilstein J. Nanotechnol. 2025, 16, 1216–1233, doi:10.3762/bjnano.16.90

• most helpful strategy to minimize possible side effects related to systemic drug administration. This is because, with current technologies, it is possible to perform cutaneous drug release both in a controlled and site-specific manner. The permeability of drugs through the skin depends on the

Transfer function of an asymmetric superconducting Gauss neuron

• Fedor A. Razorenov,
• Aleksander S. Ionin,
• Nikita S. Shuravin,
• Liubov N. Karelina,
• Mikhail S. Sidel’nikov,
• Sergey V. Egorov and
• Vitaly V. Bol’ginov

Beilstein J. Nanotechnol. 2025, 16, 1160–1170, doi:10.3762/bjnano.16.85

• third (output) arm. The latter consists of an inductive element Lout, which generates a magnetic flux Φout = LoutIout when a current Iout flows through it (currents in the input arms are denoted as IA,B in Figure 1). The input signal of the neuron is the magnetic flux Φin, created using a control line

• (it can also be called critical current asymmetry or Josephson inductance asymmetry). Another possible violation involves asymmetry in the input arm inductances with LA ≠ LB. This asymmetry may be referred to as “inductive” or “geometric” as it arises from differences in the shape of the input arms

• subtracting Equation 2–Equation 3. The symmetric case assumes LA = LB = L and IcA = IcB = Ic. The next step is to adopt dimensionless units: the magnetic flux is normalized by Φ0/2π, the current is normalized by the critical current Ic, and the inductance is normalized by the Josephson inductance LJ = Φ0/2πIc

Towards a quantitative theory for transmission X-ray microscopy

• James G. McNally,
• Christoph Pratsch,
• Stephan Werner,
• Stefan Rehbein,
• Andrew Gibbs,
• Jihao Wang,
• Thomas Lunkenbein,
• Peter Guttmann and
• Gerd Schneider

Beilstein J. Nanotechnol. 2025, 16, 1113–1128, doi:10.3762/bjnano.16.82

• Transmission X-ray microscopes (TXMs) are now increasingly used for quantitative analysis of samples, most notably in the spectral analysis of materials. Validating such measurements requires quantitatively accurate models for these microscopes, but current TXM models have only been tested qualitatively. Here

• . In the current study, we continue this effort toward further development of 3D models for TXMs. First, we introduce Mie theory as an alternate approach for light propagation through the sample. Mie theory provides an exact solution to Maxwell’s equations but limited to spheres of known refractive

• then propagated through a beamline about 26 m in length [24], which consists of several mirrors and a plane-grating monochromator that yields highly monochromatic light (E/ΔE ≈ 10000 for the energy of 510 eV used in the current study). This monochromator source is then re-focused and demagnified onto

Influence of ion beam current on the structural, optical, and mechanical properties of TiO₂ coatings: ion beam-assisted vs conventional electron beam evaporation

• Agata Obstarczyk and
• Urszula Wawrzaszek

Beilstein J. Nanotechnol. 2025, 16, 1097–1112, doi:10.3762/bjnano.16.81

• occurred for all coatings. In particular, an increase in ion beam current led to a reduction in crystallite size by approximately 30% compared to coatings prepared by conventional EBE process. The average anatase crystallite size for annealed films was in the range of 30.8 to 43.5 nm. A detailed SEM

• deposition with different values of ion beam current. Additionally, post-process annealing at 800 °C was applied to the fabricated samples in order to study its influence on the coatings’ properties. The literature lacks extensive studies of titanium dioxide thin films deposited by electron beam evaporation

• Energy) DC current (Iibg) and voltage were equal to 3 and 4 A and 80 and 90 V, respectively (samples denoted as S0A, S3A and S4A). Each process lasted 60 min, and the thicknesses of the prepared films, measured with an optical profilometer (Talysurf CCI Lite), were 350, 300, and 200 nm for samples S0A

Piezoelectricity of hexagonal boron nitrides improves bone tissue generation as tested on osteoblasts

• Sevin Adiguzel,
• Nilay Cicek,
• Zehra Cobandede,
• Feray B. Misirlioglu,
• Hulya Yilmaz and
• Mustafa Culha

Beilstein J. Nanotechnol. 2025, 16, 1068–1081, doi:10.3762/bjnano.16.78

• BaTiO3 alone. This difference can be attributed to the polarization of hBNs, which generates an electric current and initiates an interfacial redox reaction that generates ROS [60]. As a result, the ROS% levels in the cells treated with hBNs+US and BaTiO3+US were very close. Following the application of

Soft materials nanoarchitectonics: liquid crystals, polymers, gels, biomaterials, and others

• Katsuhiko Ariga

Beilstein J. Nanotechnol. 2025, 16, 1025–1067, doi:10.3762/bjnano.16.77

• for diabetic bone defects, and bactericidal materials. As can be seen from these examples, soft materials nanoarchitectonics offers a wide range of material designs, specific functions, and potential applications. In addition, this review examines the current state and future of soft materials

• had a smectic crystal phase that had a tilted chromophore (the part that gives the molecule its color) at 45° from the layer normal. This tilted chromophore caused a macroscopic polarization (a change in the electric field) when a direct current (DC) bias was applied during cooling from a high

• varying compositions. In other words, chemical energy and catalysis can be used to reversibly move functional liquid crystals at the microscale. The chemical fuels’ energy density is significantly higher than that of current batteries, by at least two orders of magnitude, making chemically powered liquid

Time-resolved probing of laser-induced nanostructuring processes in liquids

• Maximilian Spellauge,
• David Redka,
• Mianzhen Mo,
• Changyong Song,
• Heinz Paul Huber and
• Anton Plech

Beilstein J. Nanotechnol. 2025, 16, 968–1002, doi:10.3762/bjnano.16.74

Shape, membrane morphology, and morphodynamic response of metabolically active human mitochondria revealed by scanning ion conductance microscopy

• Eric Lieberwirth,
• Anja Schaeper,
• Regina Lange,
• Ingo Barke,
• Simone Baltrusch and
• Sylvia Speller

Beilstein J. Nanotechnol. 2025, 16, 951–967, doi:10.3762/bjnano.16.73

• nanopipette with a sub-micrometer aperture, which is brought near the sample surface via piezo actuators in an electrolyte bath. A voltage applied between two Ag/AgCl electrodes, one in the pipette and the other in the bath, generates an ion current. If the pipette approaches the sample, the ionic current

• drops sharply due to reduction of ion cross section. This decrease triggers the feedback system to stop the approach at a predefined setpoint current, effectively determining the z-position of the sample at that location. By scanning the sample pixel-by-pixel in hopping mode, a three-dimensional

• cation layer on their surfaces, which is responsible for ionic conductivity in physiological media (Figure 8b). Microtubules align along direct current electric field lines and can be vibrationally excited at megahertz frequencies by electric dipole antennas [46]. Other relevant properties include

Synthesis of biowaste-derived carbon-dot-mediated silver nanoparticles and the evaluation of electrochemical properties for supercapacitor electrodes

• Navya Kumari Tenkayala,
• Chandan Kumar Maity,
• Md Moniruzzaman and
• Subramani Devaraju

Beilstein J. Nanotechnol. 2025, 16, 933–943, doi:10.3762/bjnano.16.71

• /kg at 1.5 A/g. Even at a high current density of 4 A/g, the ASC device reached a specific capacitance of 175 F/g, reinforcing its capability. The method described here provides a straightforward green approach towards biowaste-derived CD-mediated synthesis of AgNPs to produce efficient supercapacitor

• graph that as the scan rates are increased, the current densities rise owing to the quicker diffusion kinetics on the electrode surface [37]. A lower scan rate means that the entire voltammogram takes longer to complete than a high scan rate. At low scan rates, diffusion layers extend further from the

• electrode surface, resulting in reduced electrode flux compared to that of higher scan rates. This occurs because current densities are influenced by the rate of scanning [37]. The higher current density at 200 mV/s suggests that, at this specific scan rate, the ion transport rate and the reactions for the

Structural and magnetic properties of microwave-synthesized reduced graphene oxide/VO₂/Fe₂O₃ nanocomposite

• Sumanta Sahoo,
• Ankur Sood and
• Sung Soo Han

Beilstein J. Nanotechnol. 2025, 16, 921–932, doi:10.3762/bjnano.16.70

• gained considerable research attention. In this context, the current work demonstrates a facile rGO-supported solid-state MW synthetic route for fabricating a ternary nanocomposite of VO2, Fe2O3, and rGO. Here, the MW irradiation for 90 s was found to be suitable for the reduction and exfoliation of

• applications. Inspired by previous research findings, the current article aims to produce a ternary NC based on rGO, VO2, and Fe2O3 using ultrafast MW irradiation. The applied MW irradiation of only 90 s was found to be beneficial for reducing as well as exfoliating graphite oxide to form rGO. At the same time

• conducted inside the MW oven at room temperature. Furthermore, most of the reported works are based on synthesizing Fe2O3 from Fe-based aqueous salt in liquid phases. In contrast, the current work demonstrates the formation of Fe2O3 from a Fe-based organometallic compound, ferrocene. Herein, the graphite

Focused ion beam-induced platinum deposition with a low-temperature cesium ion source

• Thomas Henning Loeber,
• Bert Laegel,
• Meltem Sezen,
• Feray Bakan Misirlioglu,
• Edgar J. D. Vredenbregt and
• Yang Li

Beilstein J. Nanotechnol. 2025, 16, 910–920, doi:10.3762/bjnano.16.69

• currents. Deposition rate, material composition, and electrical resistivity were examined and compared with layers deposited at comparable settings with a standard gallium (Ga) FIB. The deposition rate is found to depend linearly on the current density. The rate is comparable for Cs+ and Ga+ under similar

• exact order, however, of which mechanism contributes how much to the deposition, for example, for cesium (Cs) ions, is beyond the scope of this paper since FIBID is rather complex and depends on a variety of parameters. Besides beam parameters such as acceleration voltage, beam current, ion dose, dwell

• , ion currents from 16 to 285 pA were used, so the current densities were between 0.9 and 14.2 pA·μm−2. The overall deposition time was kept constant at 2:30 min, and the ion dose was changed from 128 to 2138 pC·μm−2. The ions were accelerated with voltages of 2, 5, 8, and 16 kV, while the measured ion

Heat-induced transformation of nickel-coated polycrystalline diamond film studied in situ by XPS and NEXAFS

• Olga V. Sedelnikova,
• Yuliya V. Fedoseeva,
• Dmitriy V. Gorodetskiy,
• Yuri N. Palyanov,
• Elena V. Shlyakhova,
• Eugene A. Maksimovskiy,
• Anna A. Makarova,
• Lyubov G. Bulusheva and
• Aleksandr V. Okotrub

Beilstein J. Nanotechnol. 2025, 16, 887–898, doi:10.3762/bjnano.16.67

• and 3 nm for AEY. The TEY spectra were recorded by measuring the leakage current with a Keithley ammeter. The experimental data were normalized to the ring current and photon flux measured using a clean gold crystal. In the AEY spectra, emitted Auger electrons were measured using a PHOIBOS 150

Synchrotron X-ray photoelectron spectroscopy study of sodium adsorption on vertically arranged MoS₂ layers coated with pyrolytic carbon

• Alexander V. Okotrub,
• Anastasiya D. Fedorenko,
• Anna A. Makarova,
• Veronica S. Sulyaeva,
• Yuliya V. Fedoseeva and
• Lyubov G. Bulusheva

Beilstein J. Nanotechnol. 2025, 16, 847–859, doi:10.3762/bjnano.16.64

• deposition. Initially, a Pt layer of 21 nm was electrodeposited at 5 keV and 1 nA. After that, a thick Pt cap layer was ion-plated at 30 keV and 250 pA. Then, the FIB was operated at an ion accelerating voltage of 30 keV and ion current of 20 nA to cut the sample. Finally, the section was finely polished at

• an ion current of 250 pA to obtain a smooth surface. The image was acquired using a TESCAN AMBER (TESCAN Ltd., Brno, Czech Republic) microscope at an accelerating voltage of 5 kV in secondary electron mode. Raman spectra were recorded using a LabRAM HR Evolution spectrometer (Horiba, Kyoto, Japan

• measuring leakage current in total electron yield mode. The experimental data were normalized to the ring current and a photon flux measured using a clean gold crystal. The XPS spectra were measured at synchrotron radiation of 830 and 470 eV. After the XPS and NEXAFS measurements were completed, the samples

Facile one-step radio frequency magnetron sputtering of Ni/NiO on stainless steel for an efficient electrode for hydrogen evolution reaction

• Ha Huu Do,
• Khac Binh Nguyen,
• Phuong N. Nguyen and
• Hoai Phuong Pham

Beilstein J. Nanotechnol. 2025, 16, 837–846, doi:10.3762/bjnano.16.63

• efficiency. The evaluation of catalytic activities revealed that the optimal sample of Ni/NiO/SS-10 displayed a higher HER performance than bare SS. To produce H2 at a current density of 10 mA·cm−2, this electrode required a low overpotential of 184 mV and demonstrated remarkable durability over 12 h of

• accompanied by toxic solvents and gases, influencing the environment and people’s health. One of the most significant current discussions in water electrolysis is finding green methods to prepare high-efficiency electrocatalysts. Thus, vacuum physical techniques have gained considerable attention in

• provides better HER efficacy than other as-synthesized catalysts. To reach a cathodic current density of 10 mA·cm−2, SS, Ni/NiO/SS-5, Ni/NiO/SS-10 Ni/NiO/SS-15, and Ni/NiO/SS-20 electrodes needed overpotentials of 431, 247, 184, 326, and 382 mV vs RHE, respectively. A smaller overpotential implies a

Synthesis and magnetic transitions of rare-earth-free Fe–Mn–Ni–Si-based compositionally complex alloys at bulk and nanoscale

• Shabbir Tahir,
• Tatiana Smoliarova,
• Carlos Doñate-Buendía,
• Michael Farle,
• Natalia Shkodich and
• Bilal Gökce

Beilstein J. Nanotechnol. 2025, 16, 823–836, doi:10.3762/bjnano.16.62

• [50]. In the current work, we aim to develop NPs of bulk rare-earth-free MnTX-based CCAs via PLAL. We start with bulk Ge-based CCA synthesized by high energy ball milling (HEBM) followed by spark plasma sintering (SPS), and an Al-based CCA obtained by powder pressing and sintering. Our goal is not

• information, indicating the coexistence of BCC and FCC phases. This differs from the work by Law et al. [25] where the alloy synthesized by arc melting resulted in a single-phase HCP structure at room temperature. The BCC phase, predominant in the current work, may not appear in alloys processed by arc

Morphology and properties of pyrite nanoparticles obtained by pulsed laser ablation in liquid and thin films for photodetection

• Akshana Parameswaran Sreekala,
• Bindu Krishnan,
• Rene Fabian Cienfuegos Pelaes,
• David Avellaneda Avellaneda,
• Josué Amílcar Aguilar-Martínez and
• Sadasivan Shaji

Beilstein J. Nanotechnol. 2025, 16, 785–805, doi:10.3762/bjnano.16.60

• Akshana Parameswaran Sreekala Bindu Krishnan Rene Fabian Cienfuegos Pelaes David Avellaneda Avellaneda Josue Amilcar Aguilar-Martinez Sadasivan Shaji Facultad de Ingeniería Mecánica y Eléctrica, Universidad Autónoma de Nuevo León, San Nicolás de los Garza, Nuevo León, 66455, México Current

• parallel to one another and immersed in 12.5 mL FeS2 nanocolloid (FIPA) kept at room temperature during EPD. A potential difference of 400 V (constant voltage, with current of approximately 2 mA) was applied after optimization of EPD conditions. The deposition was carried out for 1 h. The positive

• analysis. A dual-beam UV–vis–NIR spectrophotometer was used to analyze the optical characteristics of the nanocolloids (Jasco V770). A Keithley 6487 picoammeter/voltage source was used to record the electrical properties of the films. The current–voltage (I–V) curves for the photodiodes were measured both

Changes of structural, magnetic and spectroscopic properties of microencapsulated iron sucrose nanoparticles in saline

• Sabina Lewińska,
• Pavlo Aleshkevych,
• Roman Minikayev,
• Anna Bajorek,
• Mateusz Dulski,
• Krystian Prusik,
• Tomasz Wojciechowski and
• Anna Ślawska-Waniewska

Beilstein J. Nanotechnol. 2025, 16, 762–784, doi:10.3762/bjnano.16.59

• obtained [17][18], the investigation of AB-Fortis iron seems to be relevant. In this context, the AB-Fortis iron was selected as the main object of research (as the experimental sample) and an in-depth analysis of its physical properties, which in the current state of knowledge still remain undefined, is