Attempts to preserve and visualize protein corona on the surface of biological nanoparticles in blood serum using photomodification

• Julia E. Poletaeva,
• Anastasiya V. Tupitsyna,
• Alina E. Grigor’eva,
• Ilya S. Dovydenko and
• Elena I. Ryabchikova

Beilstein J. Nanotechnol. 2024, 15, 1654–1666, doi:10.3762/bjnano.15.130

• these samples were spherical LPs of low electron density, having a homogeneous structure and different sizes (Figure 3a,e,f). According to [24], we identified LPs with a diameter of 10 nm and less as high-density LPs (Figure 3a,e,f), particles of 20–30 nm as low-density LPs (Figure 3a,e,f), and

• appeared homogeneous, and its high electron density made it difficult to study its fine structure. The material continued, without a visible boundary, into an appendage with polymorphic structure. The appendage showed rounded protrusions, tails, and clouds formed by structureless material of variable

• deepening. The deepening was often filled with an electron-dense substance; in this case, the EV had the appearance of a thick ring on the grids (Figure 4g–j,m–o). The analysis of the structure and identification of bio-NPs in samples obtained from photomodified sera were complicated by the changes caused

Fabrication of hafnium-based nanoparticles and nanostructures using picosecond laser ablation

• Abhishek Das,
• Mangababu Akkanaboina,
• Jagannath Rathod,
• R. Sai Prasad Goud,
• Kanaka Ravi Kumar,
• Raghu C. Reddy,
• Ratheesh Ravendran,
• Katia Vutova,
• S. V. S. Nageswara Rao and
• Venugopal Rao Soma

Beilstein J. Nanotechnol. 2024, 15, 1639–1653, doi:10.3762/bjnano.15.129

• . These Hf sponges, cut and polished to 10 mm × 10 mm × 2 mm, were used as ablation targets. The pristine target had the crystal structure of hexagonal HfO0.25, as confirmed by X-ray diffraction (XRD) data (see Figure 1a). The elemental composition (Hf: 73.68%, O: 26.32%) was determined by energy

• , we did not notice such a structure in the case of NPs fabricated in DW (Figure 4a). Shell-like structures in Figure 4b and Figure 4c are indicated with red arrows. These structures are multilayered carbon shells around the NPs. Similar formations were noticed in other studies where carbon-rich

• grow to form crystals [43][44][45]. These crystals coalesce to form a polycrystalline structure [43][46]. As the vapour rushes out as a jet, these polycrystals assemble [43][47] linearly to form nanofibres. The formation of these nanofibres seems to depend upon laser parameters such as pulse duration

Biomimetic nanocarriers: integrating natural functions for advanced therapeutic applications

• Hugo Felix Perini,
• Beatriz Sodré Matos,
• Carlo José Freire de Oliveira and
• Marcos Vinicius da Silva

Beilstein J. Nanotechnol. 2024, 15, 1619–1626, doi:10.3762/bjnano.15.127

• replicating the characteristics or functions of native cells [19]. Nanoparticle coating involves obtaining nanoparticles (Figure 1-2A), which can be organic or inorganic in structure (Figure 2A), and conjugating them with functional ligands (Figure 1-2B) or biological structures, such as cell membranes

Natural nanofibers embedded in the seed mucilage envelope: composite hydrogels with specific adhesive and frictional properties

• Agnieszka Kreitschitz and
• Stanislav N. Gorb

Beilstein J. Nanotechnol. 2024, 15, 1603–1618, doi:10.3762/bjnano.15.126

• the mucilage envelope, primarily in the context of its structure and physical properties, as well as biological functions associated with these properties. Keywords: adhesion; cellulose; friction; hydrogel; mucilage envelope; seeds; Introduction The definition of hydrogels describes them as

• its composition [14][15][16]. The nanoscale level of the spatial organisation of mucilage observed with scanning electron microscopy (SEM) reveals the complexity of the mucilage with special features, such as 3D organisation of polysaccharides in a net-like structure [7][13]. In the last years, the

• ], or to animal bodies, promoting epizoochory [31][32][33]. These distinct physical features make mucilage also an important substrate for pharmaceutical, biomedical, and food industries [11][15][19][20][21]. Here, we briefly review the basic composition and structure of mucilage, its frictional and

Liver-targeting iron oxide nanoparticles and their complexes with plant extracts for biocompatibility

• Shushanik A. Kazaryan,
• Seda A. Oganian,
• Gayane S. Vardanyan,
• Anatolie S. Sidorenko and
• Ashkhen A. Hovhannisyan

Beilstein J. Nanotechnol. 2024, 15, 1593–1602, doi:10.3762/bjnano.15.125

• adverse reactions. The toxicity of MNPs depends on various factors such as size, shape, structure, surface modification, concentration, dosage, biodistribution, bioavailability, solubility, immunogenicity, and pharmacokinetics [23][24]. Their use in some clinical applications is limited by low solubility

• hepatotoxicity and cause inflammatory reactions [31][40][41][42][43]. Askri et al. demonstrated the weakness of the antioxidant barrier against these iron nanoparticles [31]. When Fe3O4 NPs accumulate in lysosomes and release iron ions from their structure, this leads to the dysfunction of mitochondria

• . Histological analysis of morphological changes in liver tissue In the histological examination of the toxic effects of the agents in all groups, a characteristic architecture typical of the liver was observed, with preserved lobular structure and radial arrangement of hepatocytes, as well as normal blood

Facile synthesis of size-tunable L-carnosine-capped silver nanoparticles and their role in metal ion sensing and catalytic degradation of p-nitrophenol

• Akash Kumar,
• Ridhima Chadha,
• Abhishek Das,
• Nandita Maiti and
• Rayavarapu Raja Gopal

Beilstein J. Nanotechnol. 2024, 15, 1576–1592, doi:10.3762/bjnano.15.124

• structure and imparts functional attributes such as metal ion chelation and catalytic enhancement. These features make ʟ-carnosine-capped AgNPs an ideal candidate for environmental applications. It was also reported that pristine AgNPs significantly interact with ʟ-carnosine [7]. Traditional methods for

• , Netherlands) for a detailed examination of size and morphology. The crystalline structure of ʟ-car-AgNP1 was determined using X-ray diffraction (XRD, Rigaku Smartlab, Japan) within a 2θ range of 35° to 80°. Nanoparticle solutions were air-dried, and the obtained nanopowders (20 mg) were used for measurements

• -carnosine and ʟ-car-AgNPs and 100 s for ʟ-carnosine in aqueous solution. DFT calculations Theoretical insights into the FTIR and Raman measurements were obtained through molecular structure optimization of ʟ-carnosine, its anionic form, and probable ʟ-carnosine–(Ag)4 complexes. The structure optimization

Ultrablack color in velvet ant cuticle

• Vinicius Marques Lopez,
• Wencke Krings,
• Juliana Reis Machado,
• Stanislav Gorb and
• Rhainer Guillermo-Ferreira

Beilstein J. Nanotechnol. 2024, 15, 1554–1565, doi:10.3762/bjnano.15.122

• spectroscopy, we conducted a comprehensive analysis of the cuticle to elucidate its unique optical properties. SEM imaging provided a detailed surface morphology, while TEM provided insights into the internal structure. CLSM showed that the cuticle exhibits no autofluorescence. Our findings reveal a highly

• underneath the epicuticle, stacked on top of each other and interconnected by columns. This kind of structure can also be found in another wasp, the oriental hornet Vespa orientalis (Hymenoptera, Vespidae) [20][21][22], however, it does not result in ultrablack colors. The structures of T. bifurca may act as

• suggests that this layered structure contributes to the overall antireflective properties of the cuticle by increasing the effective surface area available for light absorption [20]. Although this system in V. orientalis is coupled with xanthopterins to absorb light, the similar structure in T. bifurca is

The round-robin approach applied to nanoinformatics: consensus prediction of nanomaterials zeta potential

• Dimitra-Danai Varsou,
• Arkaprava Banerjee,
• Joyita Roy,
• Kunal Roy,
• Giannis Savvas,
• Haralambos Sarimveis,
• Ewelina Wyrzykowska,
• Mateusz Balicki,
• Tomasz Puzyn,
• Georgia Melagraki,
• Iseult Lynch and
• Antreas Afantitis

Beilstein J. Nanotechnol. 2024, 15, 1536–1553, doi:10.3762/bjnano.15.121

• a broad range of computational and data-driven methodologies for the exposure, hazard, and risk assessment of NMs, such as quantitative structure–activity relationship models adapted to the specificities of NMs (nanoQSAR) and grouping/read-across models, specifically developed to accurately predict

• generally more toxic than negatively charged particles of similar composition [28][29][30]. In fact, several in silico models for the ZP have been developed based on different theoretical and experimental descriptors employing a range of approaches, that is, quantitative structure–property/feature

• orbital per metal atom of 15 metal oxide NPs. Toropov et al. [31] developed, for a set of 15 metal and metal oxide NPs, a QFPR model considering both the NPs’ molecular structure and the experimental conditions, encoded in quasi-SMILES. Furthermore, research has explored the computational assessment of

Electrochemical nanostructured CuBTC/FeBTC MOF composite sensor for enrofloxacin detection

• Thi Kim Ngan Nguyen,
• Tien Dat Doan,
• Huy Hieu Luu,
• Hoang Anh Nguyen,
• Thi Thu Ha Vu,
• Quang Hai Tran,
• Ha Tran Nguyen,
• Thanh Binh Dang,
• Thi Hai Yen Pham and
• Mai Ha Hoang

Beilstein J. Nanotechnol. 2024, 15, 1522–1535, doi:10.3762/bjnano.15.120

• mixture of CuBTC and FeBTC to modify carbon paste electrodes for the determination of enrofloxacin. The characterization and properties of the fabricated electrode, including molecular structure, morphology, and electrochemical characteristics, were thoroughly investigated using various analytical

• °, 19.10°, 20.12°, 24.07°, and 27.82°, which are associated with the crystalline structure of FeBTC (CCDC card No. 640536). The CuBTC sample exhibits reflection peaks at 2θ values of 6.77° (200), 9.65° (220), 11.73° (222), 13.57° (400), 14.76° (331), 15.24° (420), 16.6° (422), 17.56° (500), 19.16° (440

Integrating high-performance computing, machine learning, data management workflows, and infrastructures for multiscale simulations and nanomaterials technologies

• Fabio Le Piane,
• Mario Vozza,
• Matteo Baldoni and
• Francesco Mercuri

Beilstein J. Nanotechnol. 2024, 15, 1498–1521, doi:10.3762/bjnano.15.119

• materials research by extracting valuable patterns and correlations from vast amounts of experimental and computational data [6][7][8][9]. These approaches enable researchers to uncover hidden relationships between composition, structure, morphology, processing, and properties, accelerating the discovery of

• unprecedented resolutions [11][12][13]. This aids in the understanding of fundamental properties and the identification of structure–property relationships. The integration of digital technologies with experimental techniques also enables real-time monitoring and control of materials synthesis processes

• of a broad range of advanced digital technologies (Figure 1). One significant area where these technologies can have a profound impact is in the design and development of advanced nanomaterials [15][16], where the relationship between structure and morphology at different scales, processing, and

Polymer lipid hybrid nanoparticles for phytochemical delivery: challenges, progress, and future prospects

• Iqra Rahat,
• Pooja Yadav,
• Aditi Singhal,
• Mohammad Fareed,
• Jaganathan Raja Purushothaman,
• Mohammed Aslam,
• Raju Balaji,
• Sonali Patil-Shinde and
• Md. Rizwanullah

Beilstein J. Nanotechnol. 2024, 15, 1473–1497, doi:10.3762/bjnano.15.118

• polyethylene glycol (PEG), poly(lactic-co-glycolic acid) (PLGA), polycaprolactone (PCL), and chitosan (CHS), provides structural integrity, controlled release properties, and protection against premature degradation [14][15]. This hybrid structure improves the encapsulation efficiency of phytochemicals/drugs

• , phospholipids help to form a carrier-like structure, which is an integral part of the system. In addition, the modification of lipoidal layers with a PEG chain provides flexibility to the nanocarrier. The ratio of the polymer and lipid can easily be adjusted to modulate the physicochemical characteristics of

• modification of PLHNPs begins with the preparation of the nanoparticles themselves. PLHNPs are typically synthesized using techniques such as solvent evaporation, nanoprecipitation, double emulsion, or solvent injection, resulting in the formation of nanoparticles with a lipid–polymer hybrid structure [60

Effect of radiation-induced vacancy saturation on the first-order phase transformation in nanoparticles: insights from a model

• Aram Shirinyan and
• Yuriy Bilogorodskyy

Beilstein J. Nanotechnol. 2024, 15, 1453–1472, doi:10.3762/bjnano.15.117

• or amorphization in metallic/ceramic nanoparticles, leading to changes in the crystal structure? Is it feasible to establish a fundamental basis to explain the behavior of materials under irradiation? Most nuclear materials have not been tested beyond an irradiation dose of 200 displacements per atom

• literature review reveals that the stability of materials under irradiation is influenced by numerous factors. Some of these characteristic factors include the elemental composition and chemical structure, the microstructure of the material (including grain boundaries, defects, dislocations, and interfaces

• ), the dose and energy of the radiation source, different types of radiation, environmental conditions, the purity and homogeneity of the material, and the crystal structure and phase stability. Let us briefly consider these publications and highlight characteristic factors to facilitate understanding

Strain-induced bandgap engineering in 2D ψ-graphene materials: a first-principles study

• Kamal Kumar,
• Nora H. de Leeuw,
• Jost Adam and
• Abhishek Kumar Mishra

Beilstein J. Nanotechnol. 2024, 15, 1440–1452, doi:10.3762/bjnano.15.116

• al. found a shift from an indirect bandgap to a direct bandgap in arsenene under uniaxial strain along the zig-zag direction [37]. Mohan et al. employed DFT to study the effect of strain on the electrical band structure of a silicene monolayer and found a bandgap (335 meV) opening in silicene at 4

• parameters, buckling heights, and electronic bandgap values of all strained structures in Table 2. Positive strain We applied positive strain toward deliberate expansion of the structure, particularly focusing on the lattice plane, varying its value from 1% to 17% (Supporting Information File 1, Figure S1

• structural and electronic properties of ψ-graphene (Table 2). We show structure geometries, PDOS, and EBS of different negatively strained structures in Supporting Information File 1, Figures S1, S4, and S5, respectively. Our investigation reveals that, on progressively increasing the magnitude of applied

Lithium niobate on insulator: an emerging nanophotonic crystal for optimized light control

• Midhun Murali,
• Amit Banerjee and
• Tanmoy Basu

Beilstein J. Nanotechnol. 2024, 15, 1415–1426, doi:10.3762/bjnano.15.114

• and hybrid devices with combined functionalities [16]. We focus on the DBR structure out of lithium niobate. To achieve PhC effects, one of the ways is creating alternating layers of LN and another material with a contrasting refractive index. We chose TiO2 and SiO2 as it has a considerable difference

• interface engineering are crucial for success [25][26][27]. The primary motivation for choosing lithium niobate is to utilize materials whose optical properties are sensitive to one or more externally controllable factors, such as electric or magnetic fields, enabling the manipulation of the structure

• wavelength can be tuned by changing the electric field without altering the reflectance values [32]. Shuai et al. introduce a bulk acoustic resonator (BAW) comprised of a sandwich-like structure with an LN film positioned between two aluminum electrodes. In this setup, acoustic waves are generated and

Nanotechnological approaches for efficient N2B delivery: from small-molecule drugs to biopharmaceuticals

• Selin Akpinar Adscheid,
• Akif E. Türeli,
• Nazende Günday-Türeli and
• Marc Schneider

Beilstein J. Nanotechnol. 2024, 15, 1400–1414, doi:10.3762/bjnano.15.113

• considered a challenge because of the existence of the blood–brain barrier (BBB, Figure 1), which is composed of several cell types [7]. The BBB is a dynamic and selective interface between the systemic circulation and the brain [8]. The structure of the healthy BBB relies on the endothelial cells and the

• challenges for drug delivery. In intranasal administration, the structure of the nose allows for an anatomical option to overcome some of those barriers. Looking at N2B, one of the most significant barriers is the nasal mucosa, where the drugs can be rapidly cleared through mucociliary clearance. While it is

• developments in N2B delivery and discuss the structure of the nasal anatomy and the principles of intranasal administration, the principles of the DDSs for N2B delivery, and the N2B delivery of biopharmaceuticals. To provide a current overview on the studies conducted in this field, we focus on work published

Various CVD-grown ZnO nanostructures for nanodevices and interdisciplinary applications

• The-Long Phan,
• Le Viet Cuong,
• Vu Dinh Lam and
• Ngoc Toan Dang

Beilstein J. Nanotechnol. 2024, 15, 1390–1399, doi:10.3762/bjnano.15.112

• annealing Zn powder under atmospheric pressure conditions, we collected nanocrystals with various morphologies, including rods, pencils, sheets, combs, tetrapods, and multilegs. Raman scattering study reveals that the samples are monophasic with a hexagonal structure, and fall into the P63mc space group

• surface effects dependent on the surface-to-volume ratio, which directly influences the electronic structure and the crystal structure symmetry. Thus, the study and fabrication of nanomaterials not only aim at exploring novel approaches of quantum physics, but also at realizing new multifunctional

• SEM micrographs of some 1D-type nanostructures. They were grown at temperatures T = 620–630 °C. The first structure is typical of hexagonal-prism-shaped nanorods, named R1 and R2 in Figure 2a,b. Their diameter can be of several tens to hundreds of nanometres, and their length is about 10–15 μm. The

A biomimetic approach towards a universal slippery liquid infused surface coating

• Ryan A. Faase,
• Madeleine H. Hummel,
• AnneMarie V. Hasbrook,
• Andrew P. Carpenter and
• Joe E. Baio

Beilstein J. Nanotechnol. 2024, 15, 1376–1389, doi:10.3762/bjnano.15.111

• composition of the layer was determined by XPS. Surface roughness was evaluated using AFM to confirm successful formation of a porous structure. Finally, ordering of specific chemical groups within our PDA SLIPS layer was explored via SFG spectroscopy. Initially, each functionalization step was assessed

• through static water contact angle measurements, the results of which can be found in Figure 2. The observed static water contact angles taken from the three different bare substrates varied slightly, with COC as the most hydrophobic one because of its hydrocarbon chemical structure. As these substrates

• roughness of all samples with the final layer of the coating were not significantly different from one another, suggesting universal attachment of the SLIPS porous component. The final structure of oxidative polymerization for dopamine into PDA is not fully agreed upon [20][44][45]. Therefore, information

Green synthesis of carbon dot structures from Rheum Ribes and Schottky diode fabrication

• Muhammed Taha Durmus and
• Ebru Bozkurt

Beilstein J. Nanotechnol. 2024, 15, 1369–1375, doi:10.3762/bjnano.15.110

• steady-state fluorescence measurements. In the second part of the study, CDs were dripped onto silicon substrates, and a CDs thin film was formed by evaporation. A diode structure was obtained by evaporating gold with the shadow mask technique on the CDs film, and the current–voltage characteristics of

• synthesis methods to obtain CDs from natural products are generally divided into top-down and bottom-up approaches, depending on the carbon source and the process used. In top-down syntheses, materials of desired size and structure are obtained from a bulk material. In bottom-up syntheses, larger

• herbaceous plant with yellowish-white flowers grows from May to June. Rheum ribes is the only Rheum species growing in Turkey. Flavonoids, stilbenes, and anthraquinones in its structure are the main phenolic components that provide a potential antioxidant effect to this plant. The young shoots and leaf stems

Out-of-plane polarization induces a picosecond photoresponse in rhombohedral stacked bilayer WSe₂

• Guixian Liu,
• Yufan Wang,
• Zhoujuan Xu,
• Zhouxiaosong Zeng,
• Lanyu Huang,
• Cuihuan Ge and
• Xiao Wang

Beilstein J. Nanotechnol. 2024, 15, 1362–1368, doi:10.3762/bjnano.15.109

• , bilayer WSe2 can be divided into 3-rhombohedral (3R) and 2-hexagonal (2H) phases [24][26][38]. When two layers are stacked antiparallel, bilayer WSe2 exhibits a hexagonal stacked (H-stacked) structure with inversion symmetry. In contrast, artificially stacking two layers in parallel to form a rhombohedral

• stacked (R-stacked) structure (as illustrated in Figure 1a) disrupts the OOP mirror symmetry. Because of differences in the stacking order, 3R WSe2 can exist in two forms, AB and BA, which determine the polarization direction (see Supporting Information File 1, Figure S1). We define the bilayer WSe2

• probe, weakening the photocurrent suppression. This results in an exponential recovery with a response time τ, causing a typical symmetric dip in the TRPC curve at zero delay. Crystal structure and the OOP polarization of 3R WSe2. (a) Crystal structure of 3R bilayer WSe2. The blue and purple spheres

Investigation of Hf/Ti bilayers for the development of transition-edge sensor microcalorimeters

• Victoria Y. Safonova,
• Anna V. Gordeeva,
• Anton V. Blagodatkin,
• Dmitry A. Pimanov,
• Anton A. Yablokov and
• Andrey L. Pankratov

Beilstein J. Nanotechnol. 2024, 15, 1353–1361, doi:10.3762/bjnano.15.108

• compared to the full-size films. This is because at the edges of the structure, the film thickness may differ from that at the center. Smooth edges are also necessary for good contact with subsequent layers. For this reason, special attention is paid to the development of technology for creating structures

• Figure 3. Samples A1–A4 One can see from Table 1 and Figure 3 that the width of the superconducting transition in all the measured samples A1–A4 of square geometry decreases with the size of the structure. The smallest sample A4 (Figure 3d) exhibited the narrowest transition. This bridge has been

• effects are still observed in samples A1 and A2, as discussed in the previous section. Discussion To answer the question of what determines the transition width of R(T) of the measured samples, we compare the sharpest transition in structure A4 with the theoretical curve calculated using the Aslamazov

Hymenoptera and biomimetic surfaces: insights and innovations

• Vinicius Marques Lopez,
• Carlo Polidori and
• Rhainer Guillermo Ferreira

Beilstein J. Nanotechnol. 2024, 15, 1333–1352, doi:10.3762/bjnano.15.107

• ]. Traditionally, this order is divided into “Symphyta” (sawflies) and Apocrita. The primary distinction between sawflies and Apocrita lies in their body structure: Sawflies lack a “wasp waist” and exhibit a broad connection between the abdomen and thorax, similar to other insects. In contrast, Apocrita are

• region of the insect. This structure is fundamental for generating flight power and precise wing adjustments. The remainder of the abdomen is known as the metasoma. The articulation between the mesosoma and metasoma, marked by the wasp waist (or petiole), enhances the maneuverability of the metasoma and

• could achieve enhanced compactness and versatility, allowing for easy transport and storage, as well as efficient adaptation to various environments and mission requirements. Microwasps exhibit remarkable adaptations in their wing structure, offering unique insights for biomimetic applications. Many

Nanoarchitectonics with cetrimonium bromide on metal nanoparticles for linker-free detection of toxic metal ions and catalytic degradation of 4-nitrophenol

• Akash Kumar and
• Raja Gopal Rayavarapu

Beilstein J. Nanotechnol. 2024, 15, 1312–1332, doi:10.3762/bjnano.15.106

• high strength to nanoparticles, the use of such nanoparticles is limited in sensing, catalysis, and biomedical applications because of post-synthesis functionalization, morphology, and toxicity [6][7][8]. CTAB is a resilient molecule on the nanoparticle surface because of its micellar structure and

• average size of the nanoparticles was calculated using ImageJ software (USA). The crystal structure of CTAB-capped gold and silver nanoparticles was determined using XRD (Rigaku Smartlab, Japan) in a 2θ range of 35° to 80°. The nanoparticle solutions were air-dried, and the obtained powders (20 mg) were

• structure of the synthesized silver and gold nanoparticles, silver and gold nanospheres capped with CTAB were measured with XRD (Figure 2e). The most common crystal structure of gold and silver in nanoparticles is face-centered cubic (FCC). In the XRD pattern of FCC CTAB-AuNS, we observe major diffraction

Interaction of graphene oxide with tannic acid: computational modeling and toxicity mitigation in C. elegans

• Romana Petry,
• James M. de Almeida,
• Francine Côa,
• Felipe Crasto de Lima,
• Diego Stéfani T. Martinez and
• Adalberto Fazzio

Beilstein J. Nanotechnol. 2024, 15, 1297–1311, doi:10.3762/bjnano.15.105

• , phototransformation, and degradation [8]. Furthermore, because of the presence of sites for different types of interaction mechanisms (i.e., hydrogen bonding, van der Waals interaction, and π–π stacking), its structure favors the adsorption of different molecules (i.e., biomolecules and organic pollutants) and metal

• processes is missing. Tannic acid (TA) is an environmentally abundant and commercially available polyphenol with relevant industrial and technological applications [17][18][19][20]. TA’s structure comprises five digallic acid units ester-linked to a glucose core. These pyrogallol hydroxy groups participate

• possible to identify interactions between these groups and GO’s carbon structure and between carbon atoms of both structures. Furthermore, we analyzed the maximum heights of TA-plus-GO conformations among the snapshots. The values range from 1.5 to 3.0 nm, which corroborates with AFM topography results and

Mn-doped ZnO nanopowders prepared by sol–gel and microwave-assisted sol–gel methods and their photocatalytic properties

• Cristina Maria Vlăduț,
• Crina Anastasescu,
• Silviu Preda,
• Oana Catalina Mocioiu,
• Simona Petrescu,
• Jeanina Pandele-Cusu,
• Dana Culita,
• Veronica Bratan,
• Ioan Balint and
• Maria Zaharescu

Beilstein J. Nanotechnol. 2024, 15, 1283–1296, doi:10.3762/bjnano.15.104

• and biological sensing [38][39][40]. The optical, thermal, and photocatalytic [40] reactivity of ZnO can also be improved with this method without changing its basic hexagonal structure. Consequently, the photodegradation of aqueous organic compounds triggered by manganese-doped ZnO still provides

• characteristic of Mn–O bond vibrations [44]. Based on the FTIR spectra, we can assume that during the gelation process a zinc-based gel with a structure similar to the one reported by Moezzi [46] was obtained. The primary distinction between the samples prepared by the two methods discussed in this article (SG

• crystallization, consistent with the results from XRD and SEM analyses. Additionally, bands at 3437 and 1613 cm−1 correspond to the vibrational modes of hydroxy groups (OH) bonded to the surface of the ZnO powders. X-ray diffraction The crystalline structure of the samples thermally treated at 500 °C was analyzed

New design of operational MEMS bridges for measurements of properties of FEBID-based nanostructures

• Bartosz Pruchnik,
• Krzysztof Kwoka,
• Ewelina Gacka,
• Dominik Badura,
• Piotr Kunicki,
• Andrzej Sierakowski,
• Paweł Janus,
• Tomasz Piasecki and
• Teodor Gotszalk

Beilstein J. Nanotechnol. 2024, 15, 1273–1282, doi:10.3762/bjnano.15.103

• shown to work as traceable displacement generators [34]. When a MEMS bridge is cut in the middle to form two separate cantilevers (Figure 2a), the two coincident edges create a region of interest (RoI) where the distance between the cantilevers is a function of the structure deflection (Figure 2a

• analyser to assess the properties of the active device. The measured level of vibration of the MEMS bridge at a known temperature allows its stiffness to be determined with an accuracy of 5% [38]. First, the thermomechanical noise of the structure vibration was measured, then the displacement of the

• only for the visual assessment of the shape and dimensions of a structure, but also for the observation of movement and deflection of an opMEMS. At the same time, the ion beam allows for local doping of the substrate and anisotropic milling. The NanoLab 600i also provides three gas injection systems