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

• light scattering (DLS) is commonly used to determine liposome size and size distribution. Transmission electron microscopy (TEM) and atomic force microscopy (AFM) can be used to image liposome morphology and determine lamellarity. Zeta potential measurements assess the surface charge of liposomes, which

• liposomes is preserved [110]. The surface charge of liposomes, often expressed as zeta potential, is an important parameter that influences their stability and interaction with biological systems. Electrophoretic light scattering is often used to measure the zeta potential of liposomes [110][125]. Cryo-TEM

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

• density coherently oscillates, coupled to both media. Usually, LIPSS formation is a multipulse phenomenon, as pulse after pulse create a different roughness on the surface or feedback mechanism to form certain SPP modes. The interference of incoming light with scattering from the SPP modes can lead to the

• absorption in the metal and scattering in other directions, which depend on the properties of the metal [43]. The penetration depth of SPPs into the metal measures how far the electric field of the SPP decays exponentially inside the metal. Ash and colleagues reported the impact of wavelength and beam width

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

• . Larger grains typically result in fewer grain boundaries, reducing phonon scattering and enhancing vibrational coherence. Raman spectra also provide insights into the influence of fabrication conditions on surface chemistry. The relative intensities of the peaks suggest that higher deposition currents

• spectrum, (b) bandgap energies of BiVO4(146), BiVO4(224), BiVO4(226), BiVO4(324), and BiVO4(326) photoanodes. Minor fluctuations above 500 nm are due to light scattering from porous films. Raman spectrum of BiVO4(146), BiVO4(224), BiVO4(226), BiVO4(324), and BiVO4(326) photoanodes. (a) LSV curves, (b) ABPE

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

• , maintaining consistent zeta potential and droplet size parameters over a 180-day storage period at 25 ± 2 °C. Dynamic light scattering analysis revealed a mean nanodroplet size (by intensity) of 173.6 ± 0.70 nm (Figure 2A). The nanoemulsion, composed of 0.28 parts of Span 80® and 0.72 parts of Tween 80

• the smallest droplet size was selected as the (HLBr) to emulsify bocaiúva oil [63]. Droplet size and zeta potential Droplet size and polydispersity index (PDI) were measured by dynamic light scattering (DLS) with a Zetasizer Nano-ZS instrument (Malvern, UK). Zeta potential was determined by

• electrophoretic light scattering with a Zetasizer Nano-ZS instrument (Malvern, UK). AANE was diluted with Milli-Q water (1:25, v/v). All measurements were performed in triplicate, and results were presented as the mean ± standard deviation [42]. Shelf stability The selected AANE was transferred to an amber vial

Investigation of the solubility of protoporphyrin IX in aqueous and hydroalcoholic solvent systems

• Michelly de Sá Matsuoka,
• Giovanna Carla Cadini Ruiz,
• Marcos Luciano Bruschi and
• Jéssica Bassi da Silva

Beilstein J. Nanotechnol. 2025, 16, 1209–1215, doi:10.3762/bjnano.16.89

• , complementary methods may be performed together, such as dynamic light scattering [26] and turbidimetry [27]. Furthermore, TEM analysis can provide a more accurate understanding of the incorporation of PpIX into the micellar systems, overcoming the limitations associated with spectrophotometric estimations

• . These limitations include potential overestimation of solubility due to light scattering by aggregates, turbidity-related interference, and the inability to distinguish between molecularly dissolved and aggregated species [28]. Therefore, TEM micrographs of PpIX samples in different media containing

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

• , controls), while the other corresponded to nanocomposites containing rotenoids (CS/TPP rot and CS/TPP–β-CD rot). Size, polydispersity, and zeta potential The average size (in nm) and PDI of the nanoparticles were measured using dynamic light scattering (DLS) on the Litesizer DLS 500 instrument (Anton Paar

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

• . Using forward light scattering experiments, Çetiner et al. reported that the time required for PA to reach an equilibrium state after osmolyte release when exposed to drastic osmotic downshocks was about 150 ms [14]. In our experiments, PA was tested in different conditions after the solution was

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

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

• equations for a sphere of given diameter and homogeneous refractive index n = 1 – δ + iβ [22], an approach well suited to the spherical nanoparticles examined here. Mie theory is one example of scattering theory in which the time-independent part of the final field is given by the sum of the incident and

• scattered fields: At a sufficient distance from the scattering object (in our case, the distance between the nanosphere and the zone plate), the scattered field is well approximated by a spherical wave, and can be written as: where S is the scattering amplitude, ψ the scattering angle from the sphere to a

• problem reduces to determination of the scattering amplitude S(ψ). The Mie solution S(ψ) is given by an infinite series of vector spherical harmonics that for numerical computations is truncated based on the accuracy required. Conventional Mie theory is based on plane waves parallel to the optical axis

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

• showed that the annealed film was composed of big, elongated grains with a length from 160 to 350 nm (Figure 3a). It is worth noting that the coatings had a milky color. This was probably the result of the size of grains, which could lead to a significant scattering of light. In contrast, the use of the

• high refractive index and thickness up to 400 nm are required. Although the density and the refractive index of crystalline TiO2 are higher than those of the amorphous phase, it is often preferred in optical devices due to its lower surface roughness and light scattering [65]. Nanoindentation

Fabrication of metal complex phthalocyanine and porphyrin nanoparticle aqueous colloids by pulsed laser fragmentation in liquid and their potential application to a photosensitizer for photodynamic therapy

• Taisei Himeda,
• Risako Kunitomi,
• Ryosuke Nabeya,
• Tamotsu Zako and
• Tsuyoshi Asahi

Beilstein J. Nanotechnol. 2025, 16, 1088–1096, doi:10.3762/bjnano.16.80

• within the nanoparticles. The hydrodynamic diameter of the colloidal dispersion was examined by dynamic light scattering (DLS) measurements, and the Z-average value was 96 nm (see Figure S2, Supporting Information File 1). The fabricated nanoparticles remained stably dispersed over a period of one month

• microcrystalline powder into small nanoparticles with high efficiency. The particle size was determined by dynamic light scattering measurements (Zetasizer nanoS, Malvern Instruments). In this analysis, the prepared colloids were diluted more than tenfold with ion-exchanged water. Dispersion stability Dispersion

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

• -Vis-NIR) measured optical properties across the 200–800 nm range, while dynamic light scattering (DLS, Malvern Panalytical) provided data on hydrodynamic size and zeta potential after dispersing 1 mg of material in 1 mL of deionized water and sonicating for 30 min. Finally, piezoresponse force

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

• (Figure 5) [237]. The compounds exhibited ferroelectric chiral smectic C, and ordered smectic phases. The purpose of this research was to examine how these chiral units contribute to electrical functions. A specific, non-scattering photocurrent decrease was observed in the organized smectic phase of

A calix[4]arene-based supramolecular nanoassembly targeting cancer cells and triggering the release of nitric oxide with green light

• Cristina Parisi,
• Loredana Ferreri,
• Tassia J. Martins,
• Francesca Laneri,
• Samantha Sollima,
• Antonina Azzolina,
• Antonella Cusimano,
• Nicola D’Antona,
• Grazia M. L. Consoli and
• Salvatore Sortino

Beilstein J. Nanotechnol. 2025, 16, 1003–1013, doi:10.3762/bjnano.16.75

• typical features of the ABF chromophore [55][56][57][58][59][62][63][64] with a maximum at ca. 480 nm (Figure 1A). However, dynamic light scattering (DLS) measurements evidenced that, in line with its amphiphilic character, compound 1 is not present in the monomeric form but as nanoaggregates ca. 180 nm

• equation: Dynamic light scattering measurements were performed on a ZetaSizer NanoZS90 (Malvern Instrument, UK), equipped with a 633 nm laser, at a scattering angle of 90° and at 25 °C. In a manner analogous to [70], photolysis experiments were performed by irradiating the samples in solution in a

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

• scattering; Review Introduction Laser synthesis and processing of materials with emphasis on structure formation on the nanoscale offers a multitude of pathways to desired structure-related functions [1]. In green processes, nanostructures and nanoparticles (NPs) can be produced that serve applications in

• verifying proposed pathways, we describe spatially and temporally resolved optical reflectivity and short-wavelength scattering methods that are able to directly reveal structural motifs. Ultimately, it is possible to investigate single NPs with a single shot before complete destruction. With these methods

• -particle imaging” describes the processes initiated by laser-excitation of an individual NP probed by X-ray scattering up to delay times of a few tens of picoseconds. The second chapter “Structural dynamics in liquids” reports on the application of ultrafast time-resolved electron scattering to investigate

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

• nanopores in thermal and plasma-enhanced chemical vapor-deposited (PECVD) SiO2 using synchrotron-based small-angle X-ray scattering (SAXS). The nanopores were fabricated by irradiating the samples with 89 MeV, 185 MeV, and 1.6 GeV Au ions, followed by hydrofluoric acid etching. We present a new approach for

• nanopores in different materials, which is essential for optimizing membrane performance in applications that require precise pore geometry. Keywords: etched ion tracks; SiO2; small angle X-ray scattering (SAXS); swift heavy ion irradiation; track-etched nanopores; Introduction Solid-state nanopores have

• , including selectivity, throughput, and molecular capture. Small-angle X-ray scattering (SAXS) has proven to be an invaluable tool for characterizing nanopore membranes, offering nondestructive analytical capabilities that yield statistical information of more than 106 pores [6][13][29][40]. With a beam size

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

• (Figure 5a, Supporting Information File 1, Figure S5a,b). They demonstrate the main diamond peak at 1333 cm−1 corresponding to the first-order scattering of the F2g symmetry. The high intensity and small full width at half maximum (FWHM) of 4 cm−1 of this band and the absence of other Raman features

• the annealed Ni-PCD film only demonstrate the Raman peaks from sp2-carbon and the absence of the diamond peak at 1333 cm−1 (Figure 5b, Supporting Information File 1, Figure S5c-e). The probing depth of Raman scattering is estimated to be about 90 nm (Supporting Information File 1, Table S1). This

• D and 2D bands. The D band represents the disordered vibration modes of graphitic hexagonal layers, and the 2D band originates from the second-order double-resonant scattering process. In general, the quality of graphene layers can be evaluated by the ratio of the intensities of the D and G peaks

Ar⁺ implantation-induced tailoring of RF-sputtered ZnO films: structural, morphological, and optical properties

• Manu Bura,
• Divya Gupta,
• Arun Kumar and
• Sanjeev Aggarwal

Beilstein J. Nanotechnol. 2025, 16, 872–886, doi:10.3762/bjnano.16.66

• disorder-induced band can be ascribed to an increase in dpa, which leads to lattice disorder [14]. The peak corresponding to the A1 (LO) mode of implanted samples is deconvoluted as shown in Figure 6. This type of scattering from the K–M point of the Brillouin zone is symmetrically forbidden. Gupta et al

• reflectance by the following relation [41]: Here R is the diffuse reflectance of the samples; s and α correspond to scattering and absorption coefficients, respectively. The scattering coefficient does not depend on the wavelength. Thus, F(R) becomes proportional to α. It has been observed that with the rise

• . Correlations This anomalous behavior of Raman modes can be attributed to the fact that the incorporation of lattice defects and disorder by energetic ions leads to translational symmetry loss. This results in the breaking of the wave vector k = 0 selection rule required for Raman scattering from different

Insights into the electronic and atomic structures of cerium oxide-based ultrathin films and nanostructures using high-brilliance light sources

• Paola Luches and
• Federico Boscherini

Beilstein J. Nanotechnol. 2025, 16, 860–871, doi:10.3762/bjnano.16.65

• shown as dashed lines. Reprinted from [49] with permission of the Royal Society of Chemistry (“Electronic properties of epitaxial cerium oxide films during controlled reduction and oxidation studied by resonant inelastic X-ray scattering” by G. Gasperi et al., Phys. Chem. Chem. Phys. vol. 18, issue 30

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

• a very reflective surface, the percentage reflectance was measured and is given in Supporting Information File 1, Figure S2c. Estimating the bandgap values of the films was challenging due to light scattering [8]. For homogenous and smooth deposition by EPD, it is crucial that the particles in the

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

• nanoscale amorphous grains exhibit averaged, broad X-ray scattering maxima, in contrast to the sharp diffraction maxima from a crystalline material [30][31]. The prediction of the amorphous iron-containing phase is based on XRD contrasts with the TEM images, which registered the crystalline structure of the

Serum heat inactivation diminishes ApoE-mediated uptake of D-Lin-MC3-DMA lipid nanoparticles

• Demian van Straten,
• Luuk van de Schepop,
• Rowan Frunt,
• Pieter Vader and
• Raymond M. Schiffelers

Beilstein J. Nanotechnol. 2025, 16, 740–748, doi:10.3762/bjnano.16.57

• Slide-A-Lyzer, MWCO 20,000, 0.5–3 mL, dark, 4 °C). LNP stocks were stored at 4 °C in the dark. LNP characterization The hydrodynamic diameter of LNPs was determined via dynamic light scattering (DLS). LNP stocks were diluted 1:20 in PBS and analyzed at 25 °C using a ZetaSizer Nano ZS 90 (Malvern

Efficiency of single-pulse laser fragmentation of organic nutraceutical dispersions in a circular jet flow-through reactor

• Tina Friedenauer,
• Maximilian Spellauge,
• Alexander Sommereyns,
• Verena Labenski,
• Tuba Esatbeyoglu,
• Christoph Rehbock,
• Heinz P. Huber and
• Stephan Barcikowski

Beilstein J. Nanotechnol. 2025, 16, 711–727, doi:10.3762/bjnano.16.55

• scattering needs to be carefully considered. The SEM images in Figure 3A and the number-weighted particle size distribution of the curcumin feedstock material in Figure 3C show a bimodal size distribution mainly composed of two size fractions, a smaller main fraction with a modal value of xmode 1, LP0

• , Supporting Information File 1. For curcumin, the influence of particle size on extinction, absorption, and scattering was calculated based on the Mie theory (using the program MiePlot [72]) for spherical particles in a range of 0.1 to 1000 µm at wavelengths of 532 and 1064 nm (Figure 7). For monodisperse

• particle sizes (1, 5, 10, and 40 µm) the relative ratio of absorption to scattering was calculated from Figure 7, and a clear size dependency was observed. Considering the relative values, it is noticeable that the portion of the fragmentation-relevant absorption efficiency (Figure 7, blue graph and values

High-temperature epitaxial growth of tantalum nitride thin films on MgO: structural evolution and potential for SQUID applications

• Michelle Cedillo Rosillo,
• Oscar Contreras López,
• Jesús Antonio Díaz,
• Agustín Conde Gallardo and
• Harvi A. Castillo Cuero

Beilstein J. Nanotechnol. 2025, 16, 690–699, doi:10.3762/bjnano.16.53

• interactions and a relatively unperturbed plume expansion. As the background pressure increases, the collision frequency between plume particles and background gas molecules rises. This leads to more pronounced interactions, including increased scattering, energy transfer, and chemical reactions. In the

• TaN film with the MgO substrate is critical for achieving superior superconducting properties, as high crystallinity and minimal defects reduce electron scattering, improving Tc of the film. The combination of cubic phase dominance, epitaxial growth, and precise lattice match with the MgO substrate

Colloidal few layered graphene–tannic acid preserves the biocompatibility of periodontal ligament cells

• Teissir Ben Ammar,
• Naji Kharouf,
• Dominique Vautier,
• Housseinou Ba,
• Nivedita Sudheer,
• Philippe Lavalle and
• Vincent Ball

Beilstein J. Nanotechnol. 2025, 16, 664–677, doi:10.3762/bjnano.16.51

• determination of the size distribution was attempted by means of dynamic light scattering but was unsuccessful owing to the lack of transparency of the suspensions even after strong dilution. The TEM images also reveal visible granules atop the layers (Figure 1D,E). Additional analysis of these granules (Figure