Venom-loaded cationic-functionalized poly(lactic acid) nanoparticles for serum production against Tityus serrulatus scorpion

• Philippe de Castro Mesquita,
• Karla Samara Rocha Soares,
• Manoela Torres-Rêgo,
• Emanuell dos Santos-Silva,
• Mariana Farias Alves-Silva,
• Alianda Maira Cornélio,
• Matheus de Freitas Fernandes-Pedrosa and
• Arnóbio Antônio da Silva-Júnior

Beilstein J. Nanotechnol. 2025, 16, 1633–1643, doi:10.3762/bjnano.16.115

• release studies showed that all samples exhibited a slight initial burst effect, releasing 30–60% of the total protein mass, followed by the subsequent slow release phase. After 144 h, the Tityus serrulatus venom-loaded PLA nanoparticles have released about 88% and 50% of the initial loaded protein for

• serrulatus venom delivery In a manner similar to [14], PLA NPs) were prepared by nanoprecipitation, up to a 30:70 (%) ratio of organic and aqueous phase (OP:AP). The organic phase was set up with 6 mL of acetone solution containing PLA (0.1% w/v) and PEI (0.1% w/v) to 14 mL of the aqueous phase containing

Nanotechnology-based approaches for the removal of microplastics from wastewater: a comprehensive review

• Nayanathara O Sanjeev,
• Manjunath Singanodi Vallabha and
• Rebekah Rubidha Lisha Rabi

Beilstein J. Nanotechnol. 2025, 16, 1607–1632, doi:10.3762/bjnano.16.114

• pollutants adsorbed on its surface. In Fenton and Fenton-like processes, hydroxyl (•OH) radicals are formed when hydrogen peroxide reacts with a metallic active phase, such as Fe2+, facilitating the oxidation and breakdown of contaminants [58]. Table 2 depicts the advantages and limitations of various

Few-photon microwave fields for superconducting transmon-based qudit control

• Irina A. Solovykh,
• Andrey V. Pashchenko,
• Natalya A. Maleeva,
• Nikolay V. Klenov,
• Olga V. Tikhonova and
• Igor I. Soloviev

Beilstein J. Nanotechnol. 2025, 16, 1580–1591, doi:10.3762/bjnano.16.112

• ) and the phase on the JJ/(interferometer) are quantized as follows: where charge energy EC = e2/2CB and Josephson energy EJ = (Φ0Ic)/2π are used (Ic is the critical current flowing through the Josephson junction). The Hamiltonian for the transmon part of our system can be written in the following form

• obtained in Equation 5 indicates that the nonlinearity of the transmon is similar to the type of Kerr phase modulation , with . Thus, the Hamiltonian in Equation 4 can be rewritten as follows: Note that, for such a system, the operator is found to be independent on time (being an integral of motion). This

• means that this nonlinearity itself leads only to phase modulation without changing the excitation statistics. In our case, the dynamics of the excitations of a Josephson nanosystem (transmon) under the action of a nonclassical electromagnetic field is studied. The interaction of the photonic and

Photocatalytic degradation of ofloxacin in water assisted by TiO₂ nanowires on carbon cloth: contributions of H₂O₂ addition and substrate absorbability

• Iram Hussain,
• Lisha Zhang,
• Zhizhen Ye and
• Jin-Ming Wu

Beilstein J. Nanotechnol. 2025, 16, 1567–1579, doi:10.3762/bjnano.16.111

• -first-order kinetic model, as determined by Equation 3: The concentration of OFL was assessed using high-performance liquid chromatography with a C18 column maintained at 30 °C. The UV–vis detector was calibrated to a wavelength of 292 nm. The mobile phase consisted of a 15:85 ratio of methanol to 0.8

• seen for the CC/HTNW, which corresponds to hydrogen titanate H2Ti5O11·3H2O (JCPDS card no. 44-0130). The TiO2 nanowires are predominantly in the anatase phase, as indicated by characteristic anatase peaks, such as the (101), (004), (200), and (105) reflections at 2θ = 25.3°, 37.8°, 48.0°, and 54.0

• °, respectively (JCPDS card no. 21-1272). The Raman spectra in Figure 2b are in accordance with the XRD analysis in phase composition. The CC/NW-450 °C spectrum displays prominent peaks at 146, 195, 287, 395, 516, and 637 cm−1, corresponding to the Eg, A1g, B1g, B1g, (A1g + B1g), and Eg modes of the anatase phase

Transient electronics for sustainability: Emerging technologies and future directions

• Jae-Young Bae,
• Myung-Kyun Choi and
• Seung-Kyun Kang

Beilstein J. Nanotechnol. 2025, 16, 1545–1556, doi:10.3762/bjnano.16.109

• rehabilitation [10][11], and orthopedic healing [12], where device functionality is required only for a defined recovery period. In such cases, transient electronic devices offer distinct advantages over conventional implants by providing essential sensing or therapeutic functions during the acute phase and

• wireless, fully bioresorbable electrical stimulator designed to promote nerve regeneration during the initial phase of neural injury treatment and subsequently undergo complete degradation [7] (Figure 1b), battery-free and bioresorbable pacemakers designed for on-demand cardiac rhythm management during the

• but also of electrical and mechanical performance. For instance, Mg-3Zn, which suffers from phase separation in bulk form, can be synthesized as a uniform alloy in thin films, offering improved corrosion resistance [61]. Moreover, bioresorbable amorphous metal (metallic glass) films have demonstrated

Influence of laser beam profile on morphology and optical properties of silicon nanoparticles formed by laser ablation in liquid

• Natalie Tarasenka,
• Vladislav Kornev,
• Alena Nevar and
• Nikolai Tarasenko

Beilstein J. Nanotechnol. 2025, 16, 1533–1544, doi:10.3762/bjnano.16.108

• Abstract In this study, silicon nanoparticles (NPs) were produced by pulsed laser ablation in a liquid, aiming to investigate the influence of a laser beam profile on the properties of the resultant NPs. Morphology, inner structure, and phase composition of the formed NPs were characterized by means of

• peak fluence in the central lobe can be calculated as [31][32]: where Ein is the incident Gaussian pulse energy (80 mJ per pulse) and ω0 is e−2 radius of the incident Gaussian beam (3 mm). Following these calculations, the fluence was calculated to be 84.9 J·cm−2. Morphology, phase composition, and

• , phase composition, and lattice parameters of the formed Si nanostructures were determined from HRTEM images by fast Fourier transformation (FFT). The morphology of the produced nanoparticles was also evaluated using scanning electron microscopy (SEM) with a SUPRA 55WDS microscope (Carl Zeiss, Germany

Dendrimer-modified carbon nanotubes for the removal and recovery of heavy metal ions from water

• Thao Quynh Ngan Tran,
• Huu Trung Nguyen,
• Subodh Kumar and
• Xuan Thang Cao

Beilstein J. Nanotechnol. 2025, 16, 1522–1532, doi:10.3762/bjnano.16.107

• patterns were recorded on a Shimadzu 6100 X-ray diffractometer in a 2θ range of 10–80°, providing insights into the crystalline structure and phase composition of the CNTs before and after modification. UV–vis spectroscopy was used to monitor adsorption of metal ions by the interaction of dendrimerized

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

• comprehensive understanding of the process flow, from the laser-induced ejection of material into the gas phase, through its processing and movement in the plume, to its eventual deposition onto a substrate. Figure 1 shows key developments in thin film synthesis and laser-based processing from 1909 to 2025

• traditional LAL, including milder reaction conditions, greater flexibility in size and phase control, and significantly higher productivity, making it more suitable for industrial-scale applications [42]. Additionally, selective pulsed heating in PLIL is distinct from conventional heating as it is both

• surrounding solvent, owing to the efficient light absorption capability of the NPs and their limited thermal transfer to the solvent. [35][63][72][73][74]. LIL also leads to phase transitions and morphological changes (Figure 7a–d) depending on the laser fluence and irradiation time [42]. Schematic

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

• , violet, green, and blue. This makes AgNPrs highly suitable for optical sensing applications [2]. The formation mechanism of AgNPrs in solution typically proceeds through three stages, namely, nucleation, seeding, and crystallization, with the crystallization phase being the slowest and rate-determining

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

• efficiency (EE). These techniques can be categorized into conventional approaches such as thin film hydration, reverse phase evaporation, solvent injection, detergent removal, and newer innovations. Also, modern techniques are further developments or adaptations of conventional approaches. These methods

• . Other characterization techniques include nuclear magnetic resonance (NMR) spectroscopy to study membrane fluidity and phase transitions, fluorescence spectroscopy for investigating drug–liposome interactions, and capillary electrophoresis to analyze liposome–drug interactions and drug release [110][121

• and 31P NMR are used to evaluate the lamellarity of liposomes, which refers to the number of bilayers of lipids in the vesicles [122]. 31P NMR provides information on membrane fluidity and phase transitions, while cryo-TEM allows for direct observation of the number of lipid bilayers [110]. X-ray

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

• and carrier gas. Oxygen and water sensors monitored gas-phase contaminants at the outlet line. In situ microscopy Nanotube growth was imaged in situ using a custom-built optical setup for homodyne polarization microscopy. A supercontinuum source (Fianium SC-400-4, 2 ps pulses, 40 MHz, spectral range

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

• ), corresponding to Bi3+ in the monoclinic phase of BiVO4 [36][37]. The V 2p region (Figure 7d) exhibits peaks at 516.2 eV (V 2p3/2) and 524.1 eV (V 2p1/2), indicating the presence of V5+ species associated with the VO43− tetrahedra [38][39]. The Bi 4f and V 2p spectra remained unchanged after testing, confirming

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

• ]. Moreover, the surfactants exhibit temperature-responsive behavior, reorganizing at higher temperatures to stabilize finer dispersions. The concurrent decline in oil phase viscosity with increasing temperature also improves emulsification efficiency by promoting shear-induced droplet breakup, particularly

• under mechanical agitation [48]. Nevertheless, while these conditions favor the formation of smaller nanodroplets, temperatures above 60 °C may compromise emulsion stability, potentially triggering phase separation or degradation of labile components. This highlights the necessity for stringent

• nanoemulsion After confirmation of the nonhemolytic effect of the nanoemulsion, the anti-inflammatory effect was evaluated. In inflammatory processes, therapeutic interventions aim primarily to attenuate the productive phase of inflammation, particularly by inhibiting leukocyte infiltration at the injury site

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

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

• visibly lower. This may be related to the disruption of the crystalline structure of PVA after encapsulation of essential oil. For rBP and rCBP, which also contains NC, a small rise in the XRD signal can be seen at around 18°, which may be from the (110) plane of the Iβ cellulose crystalline phase [32

• mobility [43]. When CEO content exceeds 8%, WVP slightly increases to 5.27 × 10−12 g·m−1·s−1·Pa−1, likely due to structural heterogeneity and phase separation within the polymer matrix [45]. These findings suggest that an optimal PE-CEO concentration exists to balance water resistance and mechanical

• (cinnamaldehyde and eugenol) [33][52]. The release of CEO from the films was studied over time (Figure 5a). The release pattern had two phases, namely, a fast initial release of 42% within the first 100 min, followed by a slower phase up to 300 min. The fast release happened because some CEO was near the surface

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

• become attractive due to their high biocompatibility and long circulating time in the blood, as well as low cytotoxicity [73]. They can be prepared by various methods, including phase inversion [73], copolymerization [110][111], and double chemical cross-linking reaction [51]. Cellulose derivatives, such

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

• lag time parameter in the model reflects the initial phase of micelle formation and the subsequent accommodation of PpIX into the micellar core, which precedes the diffusion-driven dissolution process [23]. Among the systems evaluated, water + P407 and EtOH77 + P407 exhibited the highest correlation

• ), indicated a Fickian diffusion mechanism occuring after the initial phase of micelle formation and subsequent accommodation of PpIX within the micellar core of the P407-based systems. These results reinforce the structural stability and controlled-release potential of the micellar formulations, particularly

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

• the literature that larvicidal bioassays are effective tests for identifying new insecticides against this vector mosquito, as the larval stage is the longest and most vulnerable immature phase of the insect. In addition, this species is synanthropic, which means that it is adapted to live close to

• chromatographic conditions. An NST C18 column (250 mm × 4.6 mm; 5 μm) was used as the stationary phase, while the mobile phase consisted of solution A (50% MeOH) and solution B (100% MeOH) as eluents. For each concentration, two HPLC runs were performed, and the average peak areas obtained were used to construct

Electronic and optical properties of chloropicrin adsorbed ZnS nanotubes: first principle analysis

• Prakash Yadav,
• Boddepalli SanthiBhushan and
• Anurag Srivastava

Beilstein J. Nanotechnol. 2025, 16, 1184–1196, doi:10.3762/bjnano.16.87

• humidity sensing performance compared to that of ZnO/ZnS nanorod arrays and ZnO nanorod arrays, with enhanced response, faster recovery, good linearity, and reliable reproducibility across a wide range of relative humidity conditions at room temperature. Giri et al. [48] demonstrated that phase-selective

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

• by the internal turgor pressure [56]. As depicted in the force curves for the case of hypotonic solution, the combination of a high curvature with shorter δmax strongly indicates a higher membrane tension as a result of osmolyte release in the final equilibrium phase by the MS channels, which is

• potential cell lysis are prevented by the rapid reaction of MS channels to low osmolarities, which also decreases membrane tension. Decompression of exceeding internal pressures within PA is then reduced, and obtained values for kPA and Pt represent the equilibration phase of PA which counteracts exceeding

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

• Neuron For clarity and systematic exposition, let us first consider the case of a symmetric Gauss neuron [8][12][14]. The equations of state consist of Kirchhoff’s law in the node O (Equation 1) and two phase balance equations in the partial loops of the neuron: Here, φA,B is the phase difference across

• positive directions of currents (indicated by arrows in Figure 1) and the directions of loop traversal (counterclockwise and clockwise for the left and right loops, respectively) are chosen according to [14]. The phase balance equation for the full input loop, consisting of both input arms, is obtained by

• output signal and the mean phase φ+ according to Equation 13. The TF (Equation 12–Equation 14) is obviously periodic with respect to ϕin. Within the first period, the TF of the Gauss neuron represents a symmetric bell-shaped curve that “rests” on a horizontal line (Figure 2a). The symmetry of the TF

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

• nanomaterials, usually consisting of single-phase solid solutions made of five or more elements, forming relatively simple face-centered cubic [6][7][8] (fcc) or body-centered cubic [9][10] (bcc) crystal structures, stabilized by the configurational part of Gibbs-free energy. It is worth noting that high

• HEA NPs could also be synthesized by inert gas condensation as stated very recently by Zhou et al. [31]. However, none of these aforementioned synthesis techniques give access to colloidal HEA NPs but to structures bound to an often very specific support material or limited to gas phase conditions. An

• g/h. Both the bulk target and the NPs showed a crystalline fcc phase with a lattice parameter of 3.58 Å and a solid solution structure. Löffler et al. investigated the very same element system enriched with Mn, again made by ps-LAL in ethanol. They reported particle mean diameters below 10 nm and a

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

• units of nanometers. The values of the low-resolution images were normalized to be in the range between zero and one using min–max normalization and expanded equally across RGB color channels as part of the image preprocessing phase for the SR deep learning models. To prepare the normalized low

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

• that this model produces good qualitative agreement with our 3D measurements of 60 nm gold nanospheres, but only if both β and δ for the complex refractive index n = 1 – δ + iβ of gold are included in the model. This shows that both absorption and phase properties of the specimen influence the acquired

• the parabolic wave equation to propagate light through a sample that was defined by its 3D distribution of complex refractive indices, thereby accounting for both the absorption and phase properties of the sample. We refer to this model as the partially coherent, parabolic-wave-equation (pc-PWE) model

• when the magnitude of the complex refractive index n is close to one [27]. These two requirements ensure that light rays pass through the sphere without significant deflection or reflection, subject only to the accumulated phase change. We confirm the validity of the anomalous diffraction approximation

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

• ) coatings deposited using electron beam evaporation (EBE) and ion beam-assisted deposition (IBAD) are presented. Post-process annealing at 800 °C was also conducted to examine its impact on the properties of the prepared coatings. After annealing at 800 °C, a transition from amorphous to the anatase phase

• , brookite, anatase, or rutile [16][17][18][19][20]. The rutile phase is the most stable structure of TiO2, while anatase is a metastable phase. Recently, the anatase phase of TiO2 has been particularly used in the production of solar cells and optical coatings. According to [17][18], titanium dioxide in the

• anatase phase, compared to other phases, is particularly favorable for electrochromic applications due to its efficient ion transport and relatively open configuration of octahedral units. These two phases of titanium dioxide differ significantly in their properties in terms of electronic applications [21