In search of cytotoxic selectivity on cancer cells with biogenically synthesized Ag/AgCl nanoparticles

• Mitzi J. Ramírez-Hernández,
• Mario Valera-Zaragoza,
• Omar Viñas-Bravo,
• Ariana A. Huerta-Heredia,
• Miguel A. Peña-Rico,
• Erick A. Juarez-Arellano,
• David Paniagua-Vega,
• Eduardo Ramírez-Vargas and
• Saúl Sánchez-Valdes

Beilstein J. Nanotechnol. 2022, 13, 1505–1519, doi:10.3762/bjnano.13.124

• tested on mononuclear cells. Ag/AgCl nanoparticles with spherical and triangular morphology were obtained. The size of the nanoparticles (10–70 nm) and the size distribution depended on the reaction temperature. A dose close to 20 µg/mL of Ag/AgCl nanoparticles considerably decreased the cell viability

• ) is broader than that of the reactions at 60 and 80 °C. This behavior may be related to a larger size distribution of the nanoparticles. Hence, the uniformity of the nanoparticles is higher at 60 and 80 °C. This result is consistent with Nayak et al. [37], who reported an optimal temperature of 80 °C

• reaction temperature. If the size of the nanoparticles is considered, as the reaction temperature increases, the nanoparticles become larger or the size distribution becomes broader. At room temperature and at 60 °C, the nanoparticles are less than 50 nm in size, but at 80 °C the nanoparticles reach a size

Facile preparation of Au- and BODIPY-grafted lipid nanoparticles for synergized photothermal therapy

• Yuran Wang,
• Xudong Li,
• Haijun Chen and
• Yu Gao

Beilstein J. Nanotechnol. 2022, 13, 1432–1444, doi:10.3762/bjnano.13.118

• characterization of AB-LNPs. (a) Size distribution of Au-LNPs and AB-LNPs. Digital photo of AB-LNPs showing distinct Tyndall effects. (b) UV–vis spectra of BDP and AB-LNPs. (c) TEM image of AB-LNPs. Photothermal properties of AB-LNPs. (a) Photothermal heating curves for AB-LNPs at different BDP concentrations with

Orally administered docetaxel-loaded chitosan-decorated cationic PLGA nanoparticles for intestinal tumors: formulation, comprehensive in vitro characterization, and release kinetics

• Sedat Ünal,
• Osman Doğan and
• Yeşim Aktaş

Beilstein J. Nanotechnol. 2022, 13, 1393–1407, doi:10.3762/bjnano.13.115

• capillary cell. Particle size measurements were made at an angle of 173°, while zeta potential measurements were made at an angle of 12.8°. All formulations were measured at 25°C in triplicate. The particle size distribution was expressed as mean diameter (nm) ± standard deviation (SD) and PDI. The zeta

LED-light-activated photocatalytic performance of metal-free carbon-modified hexagonal boron nitride towards degradation of methylene blue and phenol

• Nirmalendu S. Mishra and
• Pichiah Saravanan

Beilstein J. Nanotechnol. 2022, 13, 1380–1392, doi:10.3762/bjnano.13.114

• g−1. The BJH adsorption pore size distribution indicated the dominance of mesopores (2 nm < d < 50 nm) with an average pore size of 4.42 nm. The N2 adsorption–desorption isotherm demonstrated a H4 type hysteresis curve indicating narrow slit-like pores in the as-synthesized sample. In comparison

• , the HBN nanopowder had a BET surface area of 19.14 m2 g−1 with a pore volume of 0.0385 cm3 g−1. The BJH adsorption pore size distribution indicated an average pore size of 3.63 nm with dominance of mesopores (1.54 nm < d < 60 nm). The BJH adsorption pore size distribution along with the BET adsorption

Supramolecular assembly of pentamidine and polymeric cyclodextrin bimetallic core–shell nanoarchitectures

• Alexandru-Milentie Hada,
• Nina Burduja,
• Marco Abbate,
• Claudio Stagno,
• Guy Caljon,
• Louis Maes,
• Nicola Micale,
• Massimiliano Cordaro,
• Angela Scala,
• Antonino Mazzaglia and
• Anna Piperno

Beilstein J. Nanotechnol. 2022, 13, 1361–1369, doi:10.3762/bjnano.13.112

• ) in ultrapure aqueous solution, Pent solution in ethanol (green line, 52.5 µg/mL) d = 0.2 cm. (C) Size distribution (or DH) of nanoGS (red line) and nanoGSP (purple line) in a molar ratio of CD/Pent 1:1 in ultrapure water at 25 °C. Informative changes evidenced in the range of 3.2–4.2 ppm and 60.04

Recent trends in Bi-based nanomaterials: challenges, fabrication, enhancement techniques, and environmental applications

• Vishal Dutta,
• Ankush Chauhan,
• Ritesh Verma,
• C. Gopalkrishnan and
• Van-Huy Nguyen

Beilstein J. Nanotechnol. 2022, 13, 1316–1336, doi:10.3762/bjnano.13.109

• approaches affect the topological size and size distribution of semiconductor photocatalysts, substantially influencing adsorption characteristics and photocatalytic efficacy. As well as affecting the environment, synthesis size, and cost, the fabrication method also affects manufacturing safety

Enhanced electronic transport properties of Te roll-like nanostructures

• E. R. Viana,
• N. Cifuentes and
• J. C. González

Beilstein J. Nanotechnol. 2022, 13, 1284–1291, doi:10.3762/bjnano.13.106

• nanostructures, which shows that the prepared samples are composed of large-scale roll-like one-dimensional nanostructures, comparable to the shape of cinnamon sticks. Most nanostructures exhibit one flat end and a tip at the other end. The size distribution of the nanostructures is shown in the inset of Figure

Studies of probe tip materials by atomic force microscopy: a review

• Ke Xu and
• Yuzhe Liu

Beilstein J. Nanotechnol. 2022, 13, 1256–1267, doi:10.3762/bjnano.13.104

• broad particle size distribution, which was observed to be in the range of 2–80 μm. The polydispersity due to evaporation in the spark helps to select particles of suitable diameter size. The evaporation of sparks is a universal process that can be applied to basically all metals suitable as electrodes

Recent advances in green carbon dots (2015–2022): synthesis, metal ion sensing, and biological applications

• Aisha Kanwal,
• Naheed Bibi,
• Sajjad Hyder,
• Arif Muhammad,
• Hao Ren,
• Jiangtao Liu and
• Zhongli Lei

Beilstein J. Nanotechnol. 2022, 13, 1068–1107, doi:10.3762/bjnano.13.93

• have a good QY up to 48.5% and emit strong blue fluorescence [122]. Soni et al. synthesized CDs, co-doped with nitrogen and sulfur, from palm shell powder as a natural precursor with trifilic acid. The obtained CDs had a graphite-like structure, a narrow size distribution, and showed intense green

• though they have the same chemical surface groups and particle size distribution, they both have varying levels of surface oxidation. The emission wavelength moved from 518 to 543 nm as the degree of surface oxidation increased, which gives an indication about the reduction of band gap between LUMO and

Electrocatalytic oxygen reduction activity of AgCoCu oxides on reduced graphene oxide in alkaline media

• Iyyappan Madakannu,
• Indrajit Patil,
• Bhalchandra Kakade and
• Kasibhatta Kumara Ramanatha Datta

Beilstein J. Nanotechnol. 2022, 13, 1020–1029, doi:10.3762/bjnano.13.89

• size distribution of the particles (100–800 nm, Figure 5a and Figure S9, Supporting Information File 1). It is important to mention that we do not see the particles outside the rGO nanosheets, despite their large sizes and the sonication during sample preparation. This is because of the functional

Solar-light-driven LaFe_xNi_1−xO₃ perovskite oxides for photocatalytic Fenton-like reaction to degrade organic pollutants

• Chao-Wei Huang,
• Shu-Yu Hsu,
• Jun-Han Lin,
• Yun Jhou,
• Wei-Yu Chen,
• Kun-Yi Andrew Lin,
• Yu-Tang Lin and
• Van-Huy Nguyen

Beilstein J. Nanotechnol. 2022, 13, 882–895, doi:10.3762/bjnano.13.79

• the literature [48][49]. The pore size distribution of the samples was shown in Figure S2. The distribution between 2 and 50 nm indicated that the prepared perovskite oxides were mesoporous. The summary of the specific surface area, pore size, and pore volume for all the samples with different Fe/Ni

• kinetic analysis of LaFexNi1−xO3 perovskite oxides prepared at pH 0 and pH 7. Supporting Information Figure S1: The nitrogen adsorption and desorption curves of the samples with different Fe/Ni synthesis ratios at pH 0. Figure S2: Pore size distribution of the samples with different Fe/Ni synthesis

Gelatin nanoparticles with tunable mechanical properties: effect of crosslinking time and loading

• Agnes-Valencia Weiss,
• Daniel Schorr,
• Julia K. Metz,
• Metin Yildirim,
• Saeed Ahmad Khan and
• Marc Schneider

Beilstein J. Nanotechnol. 2022, 13, 778–787, doi:10.3762/bjnano.13.68

• polydispersity index (PdI) from 0.075 to 0.115, indicating a narrow size distribution. Crosslinking for 15 min did not result in stable particles with uniform colloidal properties. The surface charge of gelatin nanoparticles is clearly pH-dependent. At a pH value of 7.5 ± 0.1, the zeta potential values ranged

• size distribution. The zeta potential of FITC-dextran-loaded particles was slightly increased in comparison to the unloaded ones, which can be due to a slightly lower crosslinking rate. Sizes, PdI, and zeta potential of all formulations are listed in Table 1. Particle imaging in the QI™-mode allowed to

• extract the height image from the force–distance curves acquired at each pixel. Particles were well distributed on substrates showing no agglomeration and a narrow size distribution. GNPs occur with a smooth surface and are spherically shaped when measured under liquid conditions. Particles crosslinked

Hierarchical Bi₂WO₆/TiO₂-nanotube composites derived from natural cellulose for visible-light photocatalytic treatment of pollutants

• Zehao Lin,
• Zhan Yang and
• Jianguo Huang

Beilstein J. Nanotechnol. 2022, 13, 745–762, doi:10.3762/bjnano.13.66

• powder (16.0 m2·g−1) [52]. This is mainly benefited from the uniform and compact dispersion of Bi2WO6 nanoparticles on the hierarchical TiO2 nanotubes without aggregation. The corresponding pore size distribution pattern analyzed by the BJH model exhibits a sharp peak at approx. 3 nm and a wide peak at

Antibacterial activity of a berberine nanoformulation

• Hue Thi Nguyen,
• Tuyet Nhung Pham,
• Anh-Tuan Le,
• Nguyen Thanh Thuy,
• Tran Quang Huy and
• Thuy Thi Thu Nguyen

Beilstein J. Nanotechnol. 2022, 13, 641–652, doi:10.3762/bjnano.13.56

• spectra demonstrated that the solubility of BBR NPs was greatly enhanced compared to that of pure BBR. Glycerol played a role as a stabilizer for BBR NPs through the formation of hydrogen bonds between glycerol and BBR NPs. The prepared BBR NPs have a narrow size distribution with an average diameter of

• explained by the formation of hydrogen bonds between the oxygen-containing groups (methoxy and furyl groups) of BBR and the –OH group of glycerol in water [38]. Morphology and size distribution of BBR NPs The SEM image (Figure 3a) shows that pure BBR forms tightly agglomerated rods with rectangular cross

• the particles, polydispersity, and the agglomeration of particles during DLS analysis [39]. The BBR NPs prepared at a concentration of 2.0 mg/mL showed a narrow size distribution by intensity (Figure 3c). The z-average diameter of BBR NPs was 530.6 nm (Supporting Information File 1). In addition, its

A new method for obtaining the magnetic shape anisotropy directly from electron tomography images

• Cristian Radu,
• Ioana D. Vlaicu and
• Andrei C. Kuncser

Beilstein J. Nanotechnol. 2022, 13, 590–598, doi:10.3762/bjnano.13.51

• , the size is reported under the assumption of a quasi-spherical shape of the constituent particles. There is a multitude of techniques dedicated to nanoparticle analysis, which are able to provide information regarding the mean size and/or size distribution within a limited domain of sizes, for example

• , ImageJ, IMOD, tomo3d, or Genfire). The proposed program was designed to work directly with electron tomograms reconstructed using Genfire [22]. Although Magn3t is technically capable to provide correct information regarding particle size distribution (with particle separation capabilities) for any 3D

Correction: Coordination-assembled myricetin nanoarchitectonics for sustainably scavenging free radicals

• Xiaoyan Ma,
• Haoning Gong,
• Kenji Ogino,
• Xuehai Yan and
• Ruirui Xing

Beilstein J. Nanotechnol. 2022, 13, 570–571, doi:10.3762/bjnano.13.48

• the radical molecule is missing. It should read "ABTS•+". Correction 2: The sentence “The change of DLS was recorded at different time points (0, 2, 4, 8, 24, 48, and 72 h), showing that the average size and size distribution did not change over time (Figure 1e,f).” should read “The change of DLS was

• recorded at different time points (0, 2, 4, 8, 24, 48, and 72 h), showing that the average size and size distribution did not change over time (Figure 2e,f)."

Stimuli-responsive polypeptide nanogels for trypsin inhibition

• Petr Šálek,
• Jana Dvořáková,
• Sviatoslav Hladysh,
• Diana Oleshchuk,
• Ewa Pavlova,
• Jan Kučka and
• Vladimír Proks

Beilstein J. Nanotechnol. 2022, 13, 538–548, doi:10.3762/bjnano.13.45

• presence of SPAN 80 [24]. TEM microscopy analysis has revealed a slight narrowing of the particle size distribution with Đ = 1.43. PHEG-Tyr nanogel is composed of two families of compact hydrogel spheres with Dn = 111 and 19 nm, and Dw = 159 and 24 nm, respectively. Biocompatible zwitterionic Nα-Lys-NG was

• to the measurement at 25 °C as a result of the contribution from hydrophobic interactions and hydrogen bonds. However, it is important to note that the measurement was also affected by the broad particle size distribution of Nα-Lys-NG nanogel documented by the error bars in Figure 3a. PDI values

• mg/mL) at 25 and 37 °C using a Zetasizer Nano ZS (Malvern Instruments Ltd., Worcestershire, UK) at 633 nm and 173° detection angle. Size and size distribution were obtained from the correlation function using CONTIN analysis available in the Malvern software. The hydrodynamic diameters (DH) were

Ethosomal (−)-epigallocatechin-3-gallate as a novel approach to enhance antioxidant, anti-collagenase and anti-elastase effects

• Çiğdem Yücel,
• Gökçe Şeker Karatoprak,
• Sena Yalçıntaş and
• Tuğba Eren Böncü

Beilstein J. Nanotechnol. 2022, 13, 491–502, doi:10.3762/bjnano.13.41

• ) (Figure 2). As seen in Table 1, increasing particle size and particle size distribution were determined depending on the increasing lipid ratio and ethanol ratio. It is possible to say that ethanol gives a net negative charge to the ethosomal system and provides it with some degree of steric stabilization

Investigation of electron-induced cross-linking of self-assembled monolayers by scanning tunneling microscopy

• Patrick Stohmann,
• Sascha Koch,
• Yang Yang,
• Christopher David Kaiser,
• Julian Ehrens,
• Jürgen Schnack,
• Niklas Biere,
• Dario Anselmetti,
• Armin Gölzhäuser and
• Xianghui Zhang

Beilstein J. Nanotechnol. 2022, 13, 462–471, doi:10.3762/bjnano.13.39

• independent of each other. In addition, their size distribution was plotted as a function of the area (0.288 nm2) occupied by individual molecules in the β-phase (Figure 3e). It is evident that the size of most spots lies within 1–5 molecules, but large spots can contain up to 43 molecules. The areal number

• via random dimerization (Figure S6 in Supporting Information File 1). The size distribution of reacted molecules within a cell of 29700 nm2 is plotted in comparison to that of the dark spots determined from STM (Figure 3e). The cross-linked areas, for the same area fraction of 3% of the STM data

• and almost no voids are found in the brighter regions. This is consistent with Figure 4a, where regions with remaining molecular order appear brighter than cross-linked regions. The equivalent size distribution of the voids shows an average diameter of 0.5 ± 0.2 nm (Figure 4f, bottom panel). These

The effect of metal surface nanomorphology on the output performance of a TENG

• Yiru Wang,
• Xin Zhao,
• Yang Liu and
• Wenjun Zhou

Beilstein J. Nanotechnol. 2022, 13, 298–312, doi:10.3762/bjnano.13.25

• ). After the size screening, the proportion of each particle size was calculated. The particle size distribution plays a vital role in improving the output performance. The nanocrystals can be divided into pyramids, spheroids and strips. The shape of the metal nanocrystals determines the distribution of

• . Larger size distribution gaps lead to weaker output performance. The charge density of the metal surface is inversely proportional to the curvature radius of the metal surface, that is, the sharper the metal surface, the greater the surface charge density in the sharp part. In sample 4 (0.25 mol/L, 500 A

• obvious in experiment 15. The particle size distribution of experiment 15 is relatively concentrated, and its improvement on the output performance reaches 34%, almost twice that of experiments 4 and 5 (Figure 9). We measured the nanoparticle size and its variance and studied the relationship between the

Coordination-assembled myricetin nanoarchitectonics for sustainably scavenging free radicals

• Xiaoyan Ma,
• Haoning Gong,
• Kenji Ogino,
• Xuehai Yan and
• Ruirui Xing

Beilstein J. Nanotechnol. 2022, 13, 284–291, doi:10.3762/bjnano.13.23

• that the average size and size distribution did not change over time (Figure 1e,f). The results indicate that MZG nanoparticles are stable in water and culture medium. Although noncovalent interactions are relatively weak compared to covalent interactions, the metal coordination interaction is the

Systematic studies into uniform synthetic protein nanoparticles

• Nahal Habibi,
• Ava Mauser,
• Jeffery E. Raymond and
• Joerg Lahann

Beilstein J. Nanotechnol. 2022, 13, 274–283, doi:10.3762/bjnano.13.22

• function for the scattering intensity to deduce a size distribution spectrum based on signal intensity (or a calculated size distribution based on volume or number of particles). While SEM analysis can provide key insights into the “as manufactured” state, DLS provides insights into the in situ state of

• nSEM diameter (d = 59 nm) that is smaller than that of both HSA (d = 77 nm) and TF (d = 81 nm) with a narrower size distribution, as confirmed by a lower SEM PDISEM (0.16). The iSEM data indicates the same trend; TF/HSA is smaller (d = 92 nm) than TF (d = 109 nm) and HSA SPNPs (d = 116 nm) (Supporting

• process. Dynamic light scattering DLS measurements were performed on particles in their hydrated state using a Zetasizer Nano ZS (Malvern Panalytical). The solution in which the particles were suspended was DPBS. DLS was employed to measure the particle size distribution after particle collection and

Photothermal ablation of murine melanomas by Fe₃O₄ nanoparticle clusters

• Xue Wang,
• Lili Xuan and
• Ying Pan

Beilstein J. Nanotechnol. 2022, 13, 255–264, doi:10.3762/bjnano.13.20

• synthesized Fe3O4 NPCs was confirmed by the conserved DLS pattern of size distribution after five heating/cooling cycles with a NIR laser (Figure 1e). Altogether, our data confirmed the successful fabrication of superparamagnetic Fe3O4 NPCs that are spherical, uniformly sized and highly absorptive in the NIR

• morphology of the as-synthesized nanoparticle clusters was characterized with a JEOL JEM-2100 transmission electron microscopy (TEM). Dynamic light scattering (DLS) The synthesized Fe3O4 NPCs were diluted in RPMI 1640 medium to a final concentration of 0.25 mg/mL. The particle size distribution was

• quadratic fit of the correlation function. The particle size distribution was measured using the inbuilt DTS (nano) software. Samples were equilibrated for 1 min before measurement. All measurements were performed in triplicates. Hyperthermia effect of Fe3O4 nanoparticle clusters in solution The Fe3O4

Effects of drug concentration and PLGA addition on the properties of electrospun ampicillin trihydrate-loaded PLA nanofibers

• Tuğba Eren Böncü and
• Nurten Ozdemir

Beilstein J. Nanotechnol. 2022, 13, 245–254, doi:10.3762/bjnano.13.19

• composition, porosity, average size, distribution, individual nanofiber orientation, interaction between nanofibers, and arrangement and entanglement of the nanofibers [27][28][29]. When the mechanical properties of PLA nanofibers containing different amounts of drug were examined, the increase in the amount

Surfactant-free syntheses and pair distribution function analysis of osmium nanoparticles

• Mikkel Juelsholt,
• Jonathan Quinson,
• Emil T. S. Kjær,
• Baiyu Wang,
• Rebecca Pittkowski,
• Susan R. Cooper,
• Tiffany L. Kinnibrugh,
• Søren B. Simonsen,
• Luise Theil Kuhn,
• María Escudero-Escribano and
• Kirsten M. Ø. Jensen

Beilstein J. Nanotechnol. 2022, 13, 230–235, doi:10.3762/bjnano.13.17

• reaction at 85 °C in nuclear magnetic resonance (NMR) tubes (volume approx. 0.2 mL). The size analysis suggests that the NPs are (a) 1.6 ± 0.4 nm and (b) 1.7 ± 0.3 nm. The size distribution is presented in (c) from the analysis of 103 and 106 NPs, respectively. PDFs obtained from three different syntheses