Multifunctional anionic nanoemulsion with linseed oil and lecithin: a preliminary approach for dry eye disease

• Niédja Fittipaldi Vasconcelos,
• Almerinda Agrelli,
• Rayane Cristine Santos da Silva,
• Carina Lucena Mendes-Marques,
• Isabel Renata de Souza Arruda,
• Priscilla Stela Santana de Oliveira,
• Mércia Liane de Oliveira and
• Giovanna Machado

Beilstein J. Nanotechnol. 2025, 16, 1711–1733, doi:10.3762/bjnano.16.120

• and density The viscosity and density of LO were measured using an SVM 3000/G2 kinematic viscometer (Anton Paar, USA). The measurements were performed at two temperatures: 25 °C (by ASTM D7042-21 standard) and 75 °C, with each measurement repeated in triplicate to determine the mean ± standard

Beyond the bilayer: multilayered hygroscopic actuation in pine cone scales

• Kim Ulrich,
• Max David Mylo,
• Tom Masselter,
• Fabian Scheckenbach,
• Sophia Fischerbauer,
• Martin Nopens,
• Silja Flenner,
• Imke Greving,
• Linnea Hesse and
• Thomas Speck

Beilstein J. Nanotechnol. 2025, 16, 1695–1710, doi:10.3762/bjnano.16.119

• , the brown tissue, and the sclerenchyma fibers of a Pinus wallichiana pine cone scale. However, as their water uptake measurements consisted of only one measurement per tissue, being limited to the range of 30–80% RH, and their equilibrium criterion being one hour of exposure instead of a mass change

• cones. From each spiral, five scales were prepared for measurement, starting with the first basal scale whose adaxial epidermis was not blocked by another scale. For each experiment, one set of ten scales from one cone was then mounted in two rows of five in a sample holder inside a climate chamber (CTC

• due to an intra-tissue gradient. In contrast, the longitudinal shrinkage measured in the abaxial and adaxial sides of the sclereid layer was more uniform, with about 0.7 percentage points higher values for the adaxial side, likely being within the measurement noise. The brown tissue exhibited lower

Ambient pressure XPS at MAX IV

• Mattia Scardamaglia,
• Ulrike Küst,
• Alexander Klyushin,
• Rosemary Jones,
• Jan Knudsen,
• Robert Temperton,
• Andrey Shavorskiy and
• Esko Kokkonen

Beilstein J. Nanotechnol. 2025, 16, 1677–1694, doi:10.3762/bjnano.16.118

• every measurement. Thus, scanning of the retardation voltage becomes possible, that is, the analyzer transmission is accounted for. Since event averaging over many gas pulses is done in the analyzer, the measurement can be run very fast. A significant difference in the direct analysis can immediately be

• different measurement schemes are presented below. The data are taken from two experiments performed at the SLE of the HIPPIE beamline, while exposing a catalyst to gas pulses. Ammonia oxidation (microsecond time-resolution, pump–probe mode): This experiment used 150 µs wide 170 V voltage pulses with a

• component (2) oscillates in antiphase with the other two (1,3); when 2 increases, 1 and 3 decrease and vice versa. Thus, even though the oscillating signal picked up during the measurement is small in comparison to the time average of the spectra, Fourier analysis can reveal the periodic spectroscopic

Laser processing in liquids: insights into nanocolloid generation and thin film integration for energy, photonic, and sensing applications

• Akshana Parameswaran Sreekala,
• Pooja Raveendran Nair,
• Jithin Kundalam Kadavath,
• Bindu Krishnan,
• David Avellaneda Avellaneda,
• M. R. Anantharaman and
• Sadasivan Shaji

Beilstein J. Nanotechnol. 2025, 16, 1428–1498, doi:10.3762/bjnano.16.104

• , which were clusters of many individual In2O3 NPs. A discrepancy was observed between the grain size measurements from XRD and AFM. This discrepancy arises because AFM directly visualizes the grains but does not account for structural defects, while XRD measurement determines the size of the defect-free

• corresponding in situ resistance measurement as a function of temperature during heat treatment of the Ag layer is presented in Figure 11d. In conclusion, drop-casting, due to its simplicity, involves merely dropping a colloidal solution onto a substrate, offering limited control over the deposition process

Photochemical synthesis of silver nanoprisms via green LED irradiation and evaluation of SERS activity

• Tuan Anh Mai-Ngoc,
• Nhi Kieu Vo,
• Cong Danh Nguyen,
• Thi Kim Xuan Nguyen and
• Thanh Sinh Do

Beilstein J. Nanotechnol. 2025, 16, 1417–1427, doi:10.3762/bjnano.16.103

• nm. Samples were diluted tenfold with deionized water prior to measurement. To determine the morphology, particle size of the synthesized nanostructures, the samples were analyzed using field-emission scanning electron microscopy (FESEM, Hitachi S-4800, Japan) and transmission electron microscopy

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

• learning; spectroscopy; scanning tunnelling microscopy (STM); scanning tunnelling spectroscopy (STS); Introduction Scanning tunnelling spectroscopy (STS) extends the capability of scanning tunnelling microscopy (STM) beyond topographic imaging, allowing for the direct measurement of the electronic

• 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

• measurement. The identification of each molecular configuration was determined using the CC method with two separate reference images as shown in Figure 1d,e. For the final distinctions on the Au(111) surface, the CCR thresholds used for the SnUp and SnDown molecules were 0.983 and 0.980, respectively. Using

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

Acrocomia aculeata oil-loaded nanoemulsion: development, anti-inflammatory properties, and cytotoxicity evaluation

• Verónica Bautista-Robles,
• Hady Keita,
• Edgar Julián Paredes Gamero,
• Layna Tayná Brito Leite,
• Jessica de Araújo Isaías Muller,
• Mônica Cristina Toffoli Kadri,
• Ariadna Lafourcade Prada and
• Jesús Rafael Rodríguez Amado

Beilstein J. Nanotechnol. 2025, 16, 1277–1288, doi:10.3762/bjnano.16.93

• evaluated, from 10 to 70 °C, at the same time intervals mentioned above. Measurements were performed with the Zetasizer instrument (Malvern, UK). The nanoemulsion was equilibrated at temperatures of 10, 20, 30 40, 40, 50, 60, and 70 °C for 5 min prior to measurement [42]. Hemolytic activity Hemolytic

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

• diffraction (XRD) was performed using an Aeris Minerals Edition from PANalytical (UK) with Co radiation at 40 kV. Biopackaging samples were clipped on a 16 mm holder and the measurement was performed using a 1/8° diffraction slit. Mechanical strength was determined at room temperature using a Testometric X350

• materials (BP, rBP, and rCBP) was observed using a scanning electron microscope (SEM), model Primas E (US). The samples were coated with Pt for 30 s prior to measurement. Bioactive properties UV absorption. Transparency and UV absorption of the films were determined using UV–vis spectroscopy in the

Chitosan nanocomposite containing rotenoids: an alternative bioinsecticidal approach for the management of Aedes aegypti

• Maria A. A. Bertonceli,
• Vitor D. C. Cristo,
• Ivo J. Vieira,
• Francisco J. A. Lemos,
• Arnoldo R. Façanha,
• Raimundo Braz-Filho,
• Gustavo V. T. Batista,
• Luis G. M. Basso,
• Sérgio H. Seabra,
• Thalya S. R. Nogueira,
• Felipe F. Moreira,
• Arícia L. E. M. Assis,
• Antônia E. A. Oliveira and
• Kátia V. S. Fernandes

Beilstein J. Nanotechnol. 2025, 16, 1197–1208, doi:10.3762/bjnano.16.88

• of 1 cm−1 and an accumulation of 35 scans per spectrum. A compressive force of 15 N was applied to the samples during measurement to ensure proper contact with the ATR crystal surface. Quantification of rotenoids by high-performance liquid chromatography The quantification of rotenoids was performed

Mechanical stability of individual bacterial cells under different osmotic pressure conditions: a nanoindentation study of Pseudomonas aeruginosa

• Lizeth García-Torres,
• Idania De Alba Montero,
• Eleazar Samuel Kolosovas-Machuca,
• Facundo Ruiz,
• Sumati Bhatia,
• Jose Luis Cuellar Camacho and
• Jaime Ruiz-García

Beilstein J. Nanotechnol. 2025, 16, 1171–1183, doi:10.3762/bjnano.16.86

• N/m, and tip radius of 20–60 nm as provided by the manufacturer (Bruker), to study the morphological features of bacteria under different tested conditions. The deflection set point was adjusted during the measurement to optimize imaging conditions. Nanoindentations were performed using a maximum

• single measurement was taken along the length of each bacteria, while three measurements were performed and averaged to take its width. This is presented below in Figure 2A and Figure 2B. All obtained images, FV maps, and force–distance curves were analyzed with the NanoScope analysis software 1.7 from

Crystalline and amorphous structure selectivity of ignoble high-entropy alloy nanoparticles during laser ablation in organic liquids is set by pulse duration

• Robert Stuckert,
• Felix Pohl,
• Oleg Prymak,
• Ulrich Schürmann,
• Christoph Rehbock,
• Lorenz Kienle and
• Stephan Barcikowski

Beilstein J. Nanotechnol. 2025, 16, 1141–1159, doi:10.3762/bjnano.16.84

• indicates the formation of larger crystallites in SAED. As shown in the differential scanning calorimetry (DSC) measurement in Figure 4D, the crystallization of the amorphous particles is an exothermic process and begins at approximately 375 °C, which is exactly the same temperature where the rapid decrease

• particle core. The EELS measurement in Figure 6b and Figure 6c shows that both areas yield a significant amount of carbon signal. We observe that the particle shell mainly consists of amorphous and graphitic carbon (peak at 286 eV with respective σ* transition energy loss and possible peak at 294 eV

• combined techniques of sample preparation via FIB and consecutive EELS measurement strengthen our postulated carbon-diffusion-based mechanism about pulse-duration-driven stabilization of amorphous structures in ignoble HEA NPs. Conclusion Understanding the structure formation determinants of high-entropy

Deep learning for enhancement of low-resolution and noisy scanning probe microscopy images

• Samuel Gelman,
• Irit Rosenhek-Goldian,
• Nir Kampf,
• Marek Patočka,
• Maricarmen Rios,
• Marcos Penedo,
• Georg Fantner,
• Amir Beker,
• Sidney R. Cohen and
• Ido Azuri

Beilstein J. Nanotechnol. 2025, 16, 1129–1140, doi:10.3762/bjnano.16.83

• shows deep learning models to be superior for super-resolution tasks and enables significant reduction in AFM measurement time, whereby low-pixel-resolution AFM images are enhanced in both resolution and fidelity through deep learning. Keywords: atomic force microscopy; deep learning; fast scanning

• and deep learning models. This approach is widely used in the community, with the advantage that it saves time and resources. That said, low-resolution images formed in that way are not comprised of physically accessed measurement pixels, simplifying both the experimental and computational components

• images. Additionally, the application of the suggested procedure can greatly reduce AFM measurement time, enabling the introduction of a faster and more effective procedure into the AFM-based pipeline. Methods The Methods section is composed of Experimental and Computational Pipeline sections

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

• absorption of each nanosphere, since this is a commonly measured parameter in samples imaged by TXMs. An exact measurement of experimental absorption is non-trivial because the background around the nanosphere varies slowly with distance from the nanosphere center. Therefore, to achieve a robust estimate of

• , which we increased stepwise to include more and more of the tails of the intensity profile. This yielded multiple absorption estimates from a single nanosphere’s best-focus image, enabling an estimate of the mean absorption and its standard deviation. We performed an analogous measurement of absoprtion

Single-layer graphene oxide film grown on α-Al₂O₃(0001) for use as an adsorbent

• Shiro Entani,
• Mitsunori Honda,
• Masaru Takizawa and
• Makoto Kohda

Beilstein J. Nanotechnol. 2025, 16, 1082–1087, doi:10.3762/bjnano.16.79

• -yield method was employed to obtain the spectra. The amount of Cs adsorption was inspected by XPS. The energy scan for XPS was done with a VSW CLASS 100 hemispherical energy analyzer. An Al Kα (1486.6 eV) X-ray source (PSP TX400/2) was used for the excitation. In the XPS measurement, the CsCl solution

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

• applied electric field, the acquired phase signals determine the polarization direction of hBNs [49]. The direction and angle of polarization of piezoelectric hBNs were recorded by phase contrast measurement, and it was found to be 300°. This high value indicates that hBNs gave spontaneous responses as

Multifunctional properties of bio-poly(butylene succinate) reinforced with multiwalled carbon nanotubes

• Volodymyr Krasinskyi,
• Krzysztof Bajer,
• Ludmila Dulebova,
• Nickolas Polychronopoulos,
• Oksana Krasinska and
• Daniel Kaczor

Beilstein J. Nanotechnol. 2025, 16, 1014–1024, doi:10.3762/bjnano.16.76

• small standard deviations of the measurement results indicate the high homogeneity of the bio(nano)composite. Conclusion A comparison of the results obtained in this study with those reported in the literature reveals a lack of data on the effect of low concentrations (0.5 wt %) of pristine MWCNTs on

• for this purpose. Measurements were performed between smooth film surfaces (smooth to smooth) and rough film surfaces (rough to rough). The tests were carried out in accordance with PN-EN ISO 8295:2005 “Plastics – Film and Sheeting – Determination of the Coefficients of Friction” at a measurement

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

• using a single X-ray pulse, eliminating the need for specimen alignment to a specific Bragg angle. This ensures that the specimen can be completely damaged after a single-pulse measurement, as fresh specimens can be used for subsequent single-pulse exposures. The only requirement is that all specimens

• scattering, and system-specific background. With the last two components removed, the total elastic scattering signal (Figure 4D) exhibits a distribution typical of amorphous materials with two major humps situated between 1 and 4 Å−1, consistent with the X-ray scattering measurement as shown below in Figure

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

• local environment. The similarities between the nanopipette in the measurement setup and the microtubules in the cellular context are discussed as the basis for the hypothesis. Keywords: HeLa; metabolically active; mitochondria; morphodynamics; scanning ion conductance microscopy; Introduction

• . One of these effects appears to be associated to the dynamics of the mitochondria’s morphology (in the following referred to as morphodynamics, cf. [6]) and their contact with the measurement environment. Finally, we propose hypotheses to explain the observed effects. Results Viability of the

• investigated mitochondria was analysed by microscopy and oxygen consumption measurement. Figure 1 shows isolated mitochondria by nitrogen cavitation [34] and subsequently labelled by MitoTracker™ Green FM (MTG, Figure 1a) and tetramethylrhodamine ethyl ester perchlorate (TMRE, Figure 1b). TMRE accumulates only

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

• time obtained from the GCD measurement. Higher SCs are demonstrated by electrode materials with longer discharge durations. At 2 A/g, the obtained SC for PG-CDs-AgNPs was found to be 540 F/g. Figure 5c exemplifies plots of the current density as a function of SC of PG-CDs-AgNPs at multiple current

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

• indicates the position of the cross section. (b) SEM image of this cross section. Before the FIB cut for the cross section measurement was done, an additional Pt layer was deposited with FEBID for protection. (a) Resistivity of Ga+-induced Pt deposits using the same current density and acceleration voltage

Characterization of ion track-etched conical nanopores in thermal and PECVD SiO₂ using small angle X-ray scattering

• Shankar Dutt,
• Rudradeep Chakraborty,
• Christian Notthoff,
• Pablo Mota-Santiago,
• Christina Trautmann and
• Patrick Kluth

Beilstein J. Nanotechnol. 2025, 16, 899–909, doi:10.3762/bjnano.16.68

• images do not provide robust statistical information and are prone to measurement errors. Cross-sectional SEM imaging provides limited statistical reliability as the probability of cleaving directly through a nanopore’s central axis is extremely low. This sampling bias introduces significant

• uncertainties in dimensional measurements and makes it challenging to obtain robust structural information about the nanopores. Figure 2 shows a representative 2D scattering pattern obtained from conical nanopores in thermal SiO2. This image represents the simultaneous measurement of approximately 107 parallel

• as is, and the Si substrate was not removed before SAXS measurements. The sample-to-detector distances ranged between 7.2 and 7.6 m. Data collection was performed using Pilatus 1M and Pilatus 2M detectors during different measurement cycles. A silver behenate (AgBeh) standard was used to calibrate

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

• the preparation and measurement chambers. The Na/Mo ratio on the surface of the MoS2 film is 2.0 after Na deposition for 10 min, 5.5 after additional Na deposition for 20 min, and 3.0 after annealing (Figure 4c). The corresponding Na/Mo ratios in the bulk of the MoS2 film are 1.0, 2.4, and 1.5 (Figure

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

• Co Kα radiation over a 2θ range of 20–110°. The magnetic properties of the samples were measured using a Quantum Design DynaCool physical property measurement system at temperatures ranging from 5 to 390 K under external magnetic fields up to 9 T. Synthesis of CCA NPs by PLAL The CCA colloidal NPs

Supramolecular hydration structure of graphene-based hydrogels: density functional theory, green chemistry and interface application

• Hon Nhien Le,
• Duy Khanh Nguyen,
• Minh Triet Dang,
• Huyen Trinh Nguyen,
• Thi Bang Tam Dao,
• Trung Do Nguyen,
• Chi Nhan Ha Thuc and
• Van Hieu Le

Beilstein J. Nanotechnol. 2025, 16, 806–822, doi:10.3762/bjnano.16.61

• using the method reported in our previous paper [14][26]. Measurement of tensile properties was conducted using a universal tensile testing machine (Yang Yi Technology, 500-N load cell) and the ASTM D882-18 standard [14][27]. Results and Discussion Density functional theory calculations of intersheet

• GO-SG-ZH/PLA films are described in Figure 12 and summarized in Table 4. Additional data of measurement values and stress–strain curves are given in Supporting Information File 1, Table S1, Figure S4, Table S2, and Figure S5. Our previous paper presented that GO-ZnO coating on PLA film led to an

• shows SEM images of surfaces at the fracture of a GO-SG-ZH/PLA film generated by the tensile measurement. Conclusion Supramolecular graphene-based hydrogels are bioinspired structures which are biomimetic to natural hydration structures of cellular membranes, proteins, and other biomolecules. While