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

• method and characterized using various techniques, including X-ray diffraction, Fourier-transform infrared spectroscopy, Brunauer–Emmett–Teller analysis, and X-ray photoelectron spectroscopy. The MOF mixture exhibited a particle size ranging from 40 to 100 nm, a high surface area of 1147 m2/g, a pore

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

• include their small particle size, high encapsulation efficiency, enhanced stability, and improved dissolution in harsh gastrointestinal (GI) fluids. Following oral administration, PLHNPs demonstrate superior intestinal absorption and bioavailability, attributed to their enhanced stability and dissolution

• therapeutic effects [30][31]. Poor permeability and penetration are additional obstacles. Phytochemicals may have difficulties crossing biological membranes, such as the intestinal epithelium or the blood–brain barrier, because of their molecular size, polarity, or lipophilicity. Poor permeability limits the

• within the hybrid system. During the development of LPHNPs, different physicochemical characteristics such as size, loading capacity, charge, solubility, release, and colloidal stability can be modulated by modification in the polymer/lipid ratio [45][46][47]. Monolithic PLHNPs Monolithic PLHNPs are the

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

• , and cavities [1][2]. Experimental studies on Pd have shown that the defect density generally increases with grain size; in grains smaller than 30 nm, no defects were observed [3], suggesting that large defects (clusters and dislocations) do not exist in small nanoparticles. One possible explanation is

• -induced vacancies, assuming that the concentration of radiation-induced point defects at characteristic temperatures (far from melting) exceeds the concentration of thermal-equilibrium defects. The behavior of HDCMs under irradiation highly depends on their size. For example, when TiN nanograins are

• irradiated with He+ ions, their amorphization leads to a reduction in nanohardness, and this reduction is strongly correlated with the grain size [12]. Phase instability (radiation-induced amorphization) is observed in zirconia nanoparticles (ZrO2) embedded in nanocrystalline composites. ZrO2 nanoparticles

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

• "super-emission" scales with the system size, meaning larger systems shine brighter. The reverse phenomenon (i.e., superabsorption [35][36]) enhances light absorption for larger systems and holds promise for creating high-performance quantum batteries. However, directly observing superabsorption is

• potential as a next-generation photovoltaic technology [41][42]. These cells offer a compelling alternative to traditional silicon solar cells because of the low manufacturing cost. Additionally, CQDs possess a unique property – their bandgap can be tuned by adjusting the size of the dots. This allows them

• layer to absorb four times more near-infrared light [43]. Flip-chip micro light-emitting diodes (micro-LEDs) are a revolutionary technology with the potential to create next-generation HDR displays due to their tiny size, exceptional brightness, wide color gamut, and energy efficiency [44][45][46

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

• for CNS targeting. For example, size, shape, and surface characteristics of a DDS directly affect cellular transport and uptake, biodistribution, and the interaction with biological interfaces [64][65]. Regarding particle size, NPs with a size of approx. 15 nm or below were observed to penetrate the

• olfactory bulb thanks to the paracellular space in the olfactory epithelium [66]. However, because of their small particle size, they could be more suitable for imaging applications rather than drug delivery. Moreover, NPs with sizes up to 300 nm were found and considered suitable for intranasal delivery

• [67][68]. Significant portions of the NPs studied for N2B delivery are approx. 200 nm, which is the average size of olfactory exons [44][60]. Rejman et al. demonstrated that the clathrin-mediated pathway of endocytosis has an upper limit for internalization of approximately 200 nm. Their study also

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

• thermal sublimation [18][23], thermal evaporation [21], hydrothermal method [31][32][33], and other facile chemical/physical routes [34]. The changes in fabrication and processing conditions will influence the shape and size of ZnO nanostructures. When using CVD, vapour sources can be Zn powder or a

• . They converge at the origin with a size of ≈100 nm. For the second morphology, named T2 in Figure 3b, the tetrapods have long arms of 8–10 μm, where arms are nanorods with diameters of 200–500 nm. Another tetrapod type shown in Figure 3c, named T3, has a morphology similar to that of T2 but with

• intensity. Conclusion We used CVD to grow ZnO nanostructures, such as rods, pencils, pins, sheets, combs, tetrapods, and multilegs. Their size can be changed in the range from several tens to hundreds of nanometres. These structures usually grow at a temperature range of T = 600–650 °C. Raman spectra

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

• platelet adhesion, longer fibrin generation time, and lower clot stability compared to other surfaces. Experimental Sample preparation COC (microfluidic ChipShop, Jena, Germany) was first cut to size, into 1 × 1 cm2 squares. These COC substrates were cleaned by sequential sonication in DI water and then in

• –4000 cm−1). Each beam was overlapped in space and time to produce SFG photons at a spot size of approximately 1 mm. Spectra were collected and offset with a 4 cm−1 step size at 200 acquisitions per step. Spectra were collected in an ssp, ppp, and sps polarization combinations (SFG, visible, IR) in a

• flood gun. Scans were collected with a takeoff angle of 55° at a pressure below 3 × 10−9 Torr. A pass energy of 187.5 eV with a step size of 0.8 eV was used for the survey scans, and the high resolution had a pass energy of 23.5 eV and a step size of 0.5 eV/step. Spectra were collected with an X-ray

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

• this diode were examined. The synthesized CDs are spherical with an average size of 5.5 nm, have a negative surface charge and contain 73.3 atom % C, 24.0 atom % O, and 2.7 atom % N. The CDs exhibit fluorescence at approximately 394 nm. The layer thickness and bandgap energy of the prepared CDs film

• 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

• substrate was cut to approximately 1 cm2 in size and cleaned by washing it in acetone, methanol, and pure water for 10 min each. An ohmic contact was made with aluminum on the cleaned sample at 1 × 10−7 Torr vacuum in a PVD thermal evaporation device. Approximately 30 μL of the CDs stock solution was taken

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

• regions the critical temperature is different. Furthermore, such a protracted transition can be explained by the effect of phase separation in a film of large size, that is, it becomes superconducting in parts. The film sample C1, unlike samples A1–A4 and B1, shows thermal hysteresis, which is expressed

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

• %, with experimental measurements showing an increase of up to 433%, without altering the tool’s size [66]. Mandibles can offer structural adaptations to deliver powerful and high-speed strikes, as in trap-jaw ants (e.g., Odontomachus monticola) [67] (Figure 1B). In these species, hollow mandibles

• sliding along each other [154] (Figure 7A,B). The size of this structure can vary significantly, ranging from micrometers to the longest ovipositors documented in Arthropoda with lengths of over 100 mm [155][156], facilitating oviposition in diverse substrates such as wood, soil, or within other organisms

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

• metals and efficient degradation of 4-NP. For enabling linker-free/ligand-free detection of heavy metal ions and catalytic degradation of 4-NP, CTAB was engineered as a versatile capping agent on gold and silver nanoparticles. Various factors, including nanoparticle characteristics such as shape, size

• agents on the metal surface and further dominates functionalization. Various capping agents such as citrate, PVP, and surfactants have been the choice for metal nanoparticles. Controlled size, shape, and surface properties have been achieved using strong capping and reducing agents. Capping agents

• maintain size, shape, and stability of the nanoparticles, and suitable capping agents can modulate the nanoarchitectonics of the nanoparticles from atomic to molecular levels [2]. The surface capping can also influence the surface properties of the nanoparticles, making them compatible with specific

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

• complete characterization of the GO sample is available in [36]. Atomic force microscopy (AFM), Raman spectroscopy, and X-ray photoelectron spectroscopy (XPS) were used to assess size, morphology, number of layers, and surface chemistry of GO. The GO sample used in this study consists of single layers with

• less than 1.5 nm thickness and a flake size distribution from 18 to 308 nm. The calculated ratio between the intensity of the D (ID) and G (IG) bands of Raman is ID/IG = 0.85, indicating that the material has a high number of defects, an indirect indication of oxidation. The surface chemical

• on the well’s bottom most of the time. At 5 mg·L−1, GO aggregates and precipitates in EPA medium, which increases the exposure to C. elegans. The amount of material ingested by the nematode is limited by the size of its mouth, which is where most of the uptake occurs. C. elegans exhibits a size

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

• (SG) has gained increasing prominence in materials science because of its versatility and its capacity to produce homogeneous products with high purity. Additionally, it facilitates the incorporation of dopants in significant quantities, which enables precise control over the shape and size

• nucleation in a supersaturated solution) can be experimentally identified [18] and correlated with specific parameters of the systems exposed to microwaves [18][19][20]. For instance, the use of microwaves in nanoparticle production may increase the reaction rate, also contributing to a narrow particle size

• samples were thermally treated at 350 °C and 500 °C for 1 h each. Scanning electron microscopy The morphology and chemical composition (inset) of the thermally treated samples is illustrated in Figure 4. Homogeneously distributed, quasi-spherical nanoparticles (mean size diameter of 70 nm) are observed in

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

• cause leakage, that is, parasitic current flow through the insulating layer. Eliminating the halo effect is virtually impossible; however, the size of the halo can be measured, and its negative effects can be eliminated by proper spacing between conducting FEBID deposits [22]. Another approach is to

• (Si3N4) layer was deposited via CVD. The 40 nm thick platinum paths were then patterned by lift-off photolithography. The opMEMS bridge body was defined photolithographically with a feature size of 2 µm, etched by dry oxygen plasma etching (DRIE) and then released by KOH anisotropic wet silicon etching

• stresses in thin films by deflecting a cantilever of defined size from a uniform membrane. We see a need for such experiments for future improvement of our proposed RoI spacing tuning method. The proposed approach allowed us to evaluate the leakage currents separately from the nanodevice properties. It was

Functional morphology of cleaning devices in the damselfly Ischnura elegans (Odonata, Coenagrionidae)

• Silvana Piersanti,
• Gianandrea Salerno,
• Wencke Krings,
• Stanislav Gorb and
• Manuela Rebora

Beilstein J. Nanotechnol. 2024, 15, 1260–1272, doi:10.3762/bjnano.15.102

• with the concave cuticular lamina (Figure 1d,f). No sexual dimorphism has been observed regarding shape, size, and number of the grooming devices. The CLSM analyses revealed that each tibial grooming device shows a different relative amount of resilin from its basal to its distal portion and from the

• mouthparts and ingestion of debris is the most likely strategy, but the behavior involving antennal cleaning with mouthparts cannot be performed owing to the short antennae. Odonata antennae in adults are reduced in size, but they possess different kind of sensilla, such as chemoreceptors [44][45][46][47

The role of a tantalum interlayer in enhancing the properties of Fe₃O₄ thin films

• Hai Dang Ngo,
• Vo Doan Thanh Truong,
• Van Qui Le,
• Hoai Phuong Pham and
• Thi Kim Hang Pham

Beilstein J. Nanotechnol. 2024, 15, 1253–1259, doi:10.3762/bjnano.15.101

• . More importantly, changes in grain size and structure due to the effect of the MgO/Ta buffering layers have a strong impact on saturation magnetization and coercivity of Fe3O4 thin films compared to cases of no or just a single buffering layer. Keywords: buffer layer; Fe3O4; magnetite; RF magnetron

• substrates (referred to as samples 1, 2, and 3, recpectively). Topography images, with dimensions of 1 × 1 μm2, are shown in Figure 1. They show spherical particles with rather consistent grain sizes. In particular, samples 1 and 2 present grain size values of 7.6 ± 0.5 nm and 9.9 ± 0.6 nm, respectively

• highest value has the roughest surface among the three. These results indicate that the substrate type does have an effect on grain size and roughness of Fe3O4 thin films. Tantalum in the multilayer structure prevents the diffusion of oxygen atoms from SiO2 into MgO leading to enhanced stability of MgO

Dual-functionalized architecture enables stable and tumor cell-specific SiO₂NPs in complex biological fluids

• Iris Renata Sousa Ribeiro,
• Raquel Frenedoso da Silva,
• Romênia Ramos Domingues,
• Adriana Franco Paes Leme and
• Mateus Borba Cardoso

Beilstein J. Nanotechnol. 2024, 15, 1238–1252, doi:10.3762/bjnano.15.100

• , 5 μM particle size, New Objective). The source temperature was set to 275 °C and the nanoelectrospray voltage to 2.2 kV. The mass spectrometer operated in data-dependent acquisition mode, where full scan MS1 spectra (m/z 300–1,600) were acquired at resolution r = 60,000 after accumulation of 1 × 106

• ions. The 20 most intense peptide ions with charge state ≥2 were sequentially isolated to a target value of 5000 and fragmented by collision-induced dissociation in the linear ion trap using a normalized collision energy of 35%. Dynamic exclusion was enabled with an exclusion size list of 500 peptides

• ± 0.5 nm for the SiO2NPs-ZW-FO. The DLS measurements provided the hydrodynamic diameter of SiO2NPs and SiO2NPs-ZW-FO, indicating values of 106.8 ± 1.6 nm and 114.7 ± 1.0 nm (Figure 1d), respectively. In both cases, the polydispersity index (PDI) was less than 0.08, suggesting a homogeneous size. The

Enhanced catalytic reduction through in situ synthesized gold nanoparticles embedded in glucosamine/alginate nanocomposites

• Chi-Hien Dang,
• Le-Kim-Thuy Nguyen,
• Minh-Trong Tran,
• Van-Dung Le,
• Nguyen Minh Ty,
• T. Ngoc Han Pham,
• Hieu Vu-Quang,
• Tran Thi Kim Chi,
• Tran Thi Huong Giang,
• Nguyen Thi Thanh Tu and
• Thanh-Danh Nguyen

Beilstein J. Nanotechnol. 2024, 15, 1227–1237, doi:10.3762/bjnano.15.99

• AuNPs exhibited uniform size with an average diameter of 10.0 nm. The nanocomposites facilitated the recyclable reduction of organic dyes, including 2-nitrophenol, 4-nitrophenol, and methyl orange, employing NaBH4 as the reducing agent. Kinetic studies further underscored the potential of this

• electrostatic bonds with multivalent metal cations (such as Ca2+, Ba2+, and Cu2+) to create an extensive gel network in water [15][16]. The cross-linking of saccharide chains within alginate generates macromolecules ranging in size from micrometers to millimeters, resulting in gelispheres insoluble in water

• temperature, and the reaction time, by using UV–vis spectroscopy. Changes in the physicochemical properties, such as morphology and particle size of AuNPs, were monitored through absorbance and the λmax values of the surface plasmon resonance (SPR) band. Figure 2 illustrates the impact of synthesis conditions

Realizing active targeting in cancer nanomedicine with ultrasmall nanoparticles

• André F. Lima,
• Giselle Z. Justo and
• Alioscka A. Sousa

Beilstein J. Nanotechnol. 2024, 15, 1208–1226, doi:10.3762/bjnano.15.98

• , iron oxide, copper sulfide), and rare earth-based usNPs (cerium oxide, gadolinium oxide) [22]. Ultrasmall NPs have dimensions comparable to those of a typical globular protein of 3 to 6 nm in diameter [22][25], although the precise size criteria can vary among researchers. For the purpose of this

• proteins (Figure 2A) [52][53][54][55][56][57][58]. This occurs because of the small size and high surface curvature of usNPs, which restrict the binding interface for proteins. As a result, protein spreading and denaturation on the usNP surface are minimized, and fewer non-covalent interactions form

• , indicating the formation of a “permanently” bound (hard) protein corona. Moreover, given the appropriate combination of size and surface chemistry, nonspecific interactions between usNPs and proteins can be virtually eliminated (Figure 2C). Notably, achieving highly stable and “stealth” usNPs is feasible

A low-kiloelectronvolt focused ion beam strategy for processing low-thermal-conductance materials with nanoampere currents

• Annalena Wolff,
• Nico Klingner,
• William Thompson,
• Yinghong Zhou,
• Jinying Lin and
• Yin Xiao

Beilstein J. Nanotechnol. 2024, 15, 1197–1207, doi:10.3762/bjnano.15.97

• program SRIM (Monte Carlo simulation) was used to determine the heat flux that 5 keV gallium ions (Ga+) induce in skin. 50000 ions were simulated for each incident ion energy. The methods “surface sputtering/monolayer collision steps” was selected as the calculation type. The plotting window size was

• analysis [31][32], the differential time step has been calculated to Δt ≤ Δx2/(8α) = 23 ps. A sample volume of 600 nm × 600 nm × 400 nm (depth) has been simulated with a voxel size of Δx = 5 nm and the boundary voxels, with exception of the sample surface, have been fixed to room temperature. This approach

Synthesis, characterization and anticancer effect of doxorubicin-loaded dual stimuli-responsive smart nanopolymers

• Ömür Acet,
• Pavel Kirsanov,
• Burcu Önal Acet,
• Inessa Halets-Bui,
• Dzmitry Shcharbin,
• Şeyda Ceylan Cömert and
• Mehmet Odabaşı

Beilstein J. Nanotechnol. 2024, 15, 1189–1196, doi:10.3762/bjnano.15.96

• than free DOX. To date, several types of nanoparticles, such as liposomes, micelles, and metal-organic frameworks, have been studied to encapsulate DOX to obtain effective and non-toxic drugs [7][8]. Great attention has been paid to nanoparticles because of their specific properties, such as small size

• . Physicochemical features such as size, shape, and surface charge play an extremely important role in the internalization of nanostructures. The uptake of nanoparticles into cells requires two steps. The first is the binding to the cell membrane, and the second is the uptake into the cell [34]. The zeta potential

AI-assisted models to predict chemotherapy drugs modified with C₆₀ fullerene derivatives

• Jonathan-Siu-Loong Robles-Hernández,
• Dora Iliana Medina,
• Katerin Aguirre-Hurtado,
• Marlene Bosquez,
• Roberto Salcedo and
• Alan Miralrio

Beilstein J. Nanotechnol. 2024, 15, 1170–1188, doi:10.3762/bjnano.15.95

• C60 [21]. The unmodified fullerene C60 is known as a “free radical sponge” because its double bonds tend to accept free radicals [22]. Because of its size, surface area, and capacity to extinguish or generate reactive oxygen species, C60 is very promising in medicine and clinical therapy [23][24]. It

• because of the large size of the complexes. The atypical chemokine receptor 3, also known as CXCR7 or G-protein-coupled receptor 159 (GPR159) [16][18][43], was selected as the target protein for molecular docking. The iterative assembly refinement server (I-Tasser) was used to produce an initial structure

Introducing third-generation periodic table descriptors for nano-qRASTR modeling of zebrafish toxicity of metal oxide nanoparticles

• Supratik Kar and
• Siyun Yang

Beilstein J. Nanotechnol. 2024, 15, 1142–1152, doi:10.3762/bjnano.15.93

• of their unique properties. However, their size, surface area, and reactivity can cause toxicity, potentially leading to oxidative stress, inflammation, and cellular or DNA damage. In this study, a nano-quantitative structure–toxicity relationship (nano-QSTR) model was initially developed to assess

• ; Introduction Nanomaterials, which are defined as materials that fall in the range of 1–100 nanometers two-dimensionally, are commonly used in the fields of biomedicine, catalysis, and electricity because of their stable and unique performance, small size, and large surface area [1]. Nanomaterials encompass a

• of an element. In the context of nanoparticles, the size of the metal atoms directly affects the overall size and surface area of the nanoparticles, which are critical factors in their reactivity and interaction with other materials. The ionic radius is essential for understanding the metal’s

Local work function on graphene nanoribbons

• Daniel Rothhardt,
• Amina Kimouche,
• Tillmann Klamroth and
• Regina Hoffmann-Vogel

Beilstein J. Nanotechnol. 2024, 15, 1125–1131, doi:10.3762/bjnano.15.91

• opening a size-dependent energy gap [6][9]. As in graphene, the Fermi level of GNRs is also strongly influenced by charge transfer between the substrate and the GNR [10], again related to differences in the work function. Here, we take the work function as a local property influenced by local charge, that

• nm at far distance, resulting from the size of the graphene nanoribbon. The experimental results (blue squares in Figure 3) generally follow the shape of the calculated curve with a shift. There are several possibilities to understand the origin of this shift. First, we discuss the possibility of a z

Direct electron beam writing of silver using a β-diketonate precursor: first insights

• Katja Höflich,
• Krzysztof Maćkosz,
• Chinmai S. Jureddy,
• Aleksei Tsarapkin and
• Ivo Utke

Beilstein J. Nanotechnol. 2024, 15, 1117–1124, doi:10.3762/bjnano.15.90

• (H1) has a relatively bright appearance with particles of about 10–40 nm size that are most pronounced in the direction of the molecule delivery (indicated by the white arrow in Figure 1a). Below, smaller particles of about 5–10 nm can be seen. Particles of about 5–20 nm size are observed in the

• second part of the first halo region (H1’), where the background forms irregularly shaped dark and bright regions of several hundreds of nanometers in size. After taking the high-resolution images, the imaged regions showed an increase in particle size and brightness (cf. Supporting Information File 1

• fluorine in the halo region but showed a significant amount of both in the carbon-rich deposit (cf. Supporting Information File 1 for more details). Of note is that the surrounding of the deposit as well as the surface topography changed after deposition. Tiny particles of few nanometers in size appeared