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Search for "SEM" in Full Text gives 1090 result(s) in Beilstein Journal of Nanotechnology. Showing first 200.

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

Graphical Abstract
  • nanoparticles at 1.0% (NPs + Tsv 1.0%). Acknowledgements The authors acknowledge the Department of Materials and Engineering of the Federal University of Rio Grande do Norte for the SEM and AFM analyses. Funding The authors are grateful for the financial support from the National Council for Scientific and
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Published 17 Sep 2025

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

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  • retained over 90% of its efficiency even after 6 cycles demonstrates the stability of the CC/NW-450 °C photocatalyst. SEM and XRD data of the catalyst after the recycling experiment are shown in Figure S8 in Supporting Information File 1, from which no remarkable change can be seen because of its high
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Published 08 Sep 2025

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

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  • the SEM analysis (Supporting Information File 1, Figure S5d). The resulting fluence on the target was estimated to be 118.4 J·cm−2. A Bessel beam pattern was generated using a glass axicon with a base angle α = 7°, which was irradiated with a collimated Gaussian beam of a Nd:YAG laser. A Bessel zone
  • , 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
  • ) operating at an accelerating voltage of 10 kV. For SEM and Raman measurements, the colloidal solution was deposited onto Al foil by drop casting and dried at room temperature. The Raman measurements were performed under 488 nm excitation using a micro-Raman system (“NanoFlex”, Solar LS, Belarus). The UV–vis
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Published 04 Sep 2025

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

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  • spectroscopy was specifically used to confirm the Diels–Alder reaction on the surface of CNTs, and other characterization techniques (SEM, EDX, XRD, TGA, and FTIR) were applied to confirm the successive growth of the dendrimers. Highly dendrimerized CNTs were found to be more effective in removing heavy metal
  • with increasing dendrimer functionalization. SEM images are helpful to identify the morphological changes after the functionalization of CNTs. The comparative observation of SEM images of CNTs, CNTs-G1, CNTs-G3, and CNTs-G5 clearly reveals tube shape structure for all the materials confirming no
  • thoroughly characterized using FTIR, SEM, XRD, EDX, TGA, and Raman spectroscopy to confirm the successful functionalization and structural integrity of the materials. The applicability of these dendrimerized CNTs materials for the adsorption of Pb2+ and Cd2+ metal ions from aqueous media was thoroughly
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Published 01 Sep 2025

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

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  • caused oxidation, crystallinity loss, and reduced photoactivity due to enhanced grain boundaries. Figure 4 shows SEM images of Ba5Ta4O15 and BaTaOxNy-zp powders after successive laser fragmentation passages. Despite these challenges, prolonged fragmentation improved the photocurrent efficiency
  • ) synthesized by LAL were subjected to picosecond laser irradiation in the laser melting in liquids (LML) setup, the particles grew into significantly larger SMSPs (≈230 nm) after multiple laser passages [53]. Figure 5 presents SEM images and corresponding size distributions of Ge-based nanostructures. This
  • technique exhibit broader peaks compared to those deposited by laser ablation, where the peaks are narrower and sharper. SEM images of the surface and cross section of the films deposited by the doctor blade method, with varying ZnO layer thicknesses, reveal a noticeable difference in morphology. The films
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Published 27 Aug 2025

Parylene-coated platinum nanowire electrodes for biomolecular sensing applications

  • Chao Liu,
  • Peker Milas,
  • Michael G. Spencer and
  • Birol Ozturk

Beilstein J. Nanotechnol. 2025, 16, 1392–1400, doi:10.3762/bjnano.16.101

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  • complete as intended and these electrodes were discarded. A thin layer of copper deposition on the exposed platinum nanowire tip was further examined using SEM imaging and energy-dispersive X-ray spectroscopy (EDS) elemental composition analysis. Figure 2b presents an SEM image of the copper-coated
  • nanowire coated with parylene-C polymer, and (d) a laser-exposed platinum electrode. Scale bars are 10 μm. (a) Optical image of electrochemically deposited copper nodule on platinum nanowire tip. Scale bar is 10 μm. (b) SEM image of the deposited thin copper layer on the platinum nanowire tip of an
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Published 20 Aug 2025

Synthesis and antibacterial properties of nanosilver-modified cellulose triacetate membranes for seawater desalination

  • Lei Wang,
  • Shizhe Li,
  • Kexin Xu,
  • Wenjun Li,
  • Ying Li and
  • Gang Liu

Beilstein J. Nanotechnol. 2025, 16, 1380–1391, doi:10.3762/bjnano.16.100

Graphical Abstract
  • , which can manifest as a metallic sheen when they are present on a substrate [47]. Surface alterations of the membranes are documented using scanning electron microscopy (SEM) (Figure 4). The CTA membrane’s surface appears smooth and uniform, devoid of visible defects (Figure 4a). Cross-sectional SEM
  • the PDA layer (Figure 4e). These Ag nanoparticles, typically appearing as discrete entities, are interspersed among the PDA microspheres, contributing to the membrane’s antimicrobial properties essential for mitigating biofouling in desalination applications. The cross-sectional SEM images, along with
  • high-magnification views of the PCTA membrane (Figure 4d), reveal a dense and compact internal structure. At higher magnifications, a thin PDA layer is clearly visible on the surface of the CTA membrane, indicating successful modification of the CTA membrane with PDA. The cross-sectional SEM images of
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Published 19 Aug 2025

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

Graphical Abstract
  • ]. Different techniques are used to evaluate the characteristics of liposomes [122][123][124]. In the case of average particle size, DLS and microscopy techniques such as scanning electron microscopy (SEM), TEM, cryogenic TEM, and AFM are used to determine the size of liposomes [122]. The size of liposomes is
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Published 14 Aug 2025

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

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  • , finding numerous applications in scientific research. Deep learning models have been used to identify two-dimensional materials in microscopic images [6], characterize mineral composition in scanning electron microscopy (SEM) samples [7], and determine nanotube chirality from transmission electron
  • performed SEM characterization. V.P. performed the in situ optical imaging, developed the protocols of data treatment and analyzed the experimental data. This work is partially based on Vladimir Pimonov’s doctoral thesis (“Growth kinetics of individual carbon nanotubes studied by in situ optical microscopy
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Published 13 Aug 2025

Wavelength-dependent correlation of LIPSS periodicity and laser penetration depth in stainless steel

  • Nitin Chaudhary,
  • Chavan Akash Naik,
  • Shilpa Mangalassery,
  • Jai Prakash Gautam and
  • Sri Ram Gopal Naraharisetty

Beilstein J. Nanotechnol. 2025, 16, 1302–1315, doi:10.3762/bjnano.16.95

Graphical Abstract
  • conducted to examine the surface morphology of the samples and precisely measure the depth to which the laser heat affected or penetrated the zone. Imaging was performed using an FEI NOVA NANO SEM 450 scanning electron microscope. External etching was executed using a DC power supply machine, applying a
  • incident power at a wavelength of 800 nm. (a) 20 mW, (b) 150 mW, and (c) 300 mW. Showing the EDS elemental analysis for laser-treated and untreated stainless steel surface. (a) SEM image of laser-treated SS substrate, we picked three areas whose EDS spectra are shown in b, c, and d. (e) SEM image of bare
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Published 11 Aug 2025

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

Graphical Abstract
  • perfectly follow the crystallite size evolution. For instance, BiVO4(326) exhibits the largest crystallite size (≈40 nm) but has smaller surface particle aggregates (200–300 nm) than BiVO4(324). This mismatch arises because the particles observed via SEM are often composed of multiple crystalline grains
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Published 07 Aug 2025

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

Graphical Abstract
  • stability, making PE-CEO-infused films promising candidates for biopackaging applications requiring controlled moisture permeability. The surface morphology of the biopackaging materials was examined using scanning electron microscopy (SEM) (Figure 3). As shown in our previous research, nanocellulose in
  • suspension has a size of around 20–30 nm and a length below 300 nm, and size increase due to structural collapse would be seen upon drying [24][46]. A SEM image of the nanocellulose sample is given in Figure 3a. After freeze-drying, some coagulation occurred, increasing the size of the sample to reach ≈4 µm
  • materials (BP, rBP, and rCBP) was observed using a scanning electron microscope (SEM), model Primas E (US). The samples were coated with Pt for 30 s prior to measurement. Bioactive properties UV absorption. Transparency and UV absorption of the films were determined using UV–vis spectroscopy in the
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Published 04 Aug 2025

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

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  • are in good agreement with the near-equimolar composition of the bulk target (Cr21Mn18Fe21Co18Ni22), determined by both XRF and SEM-EDX measurements, quantifying not only the surface compositions of the corresponding targets but also bulk compositions determined from a target cross-section (Supporting
  • sizes of 108 and 153 nm, respectively. Furthermore, the elemental composition of the target was analyzed by SEM-EDX and XRF, differentiating compositions on the upper and lower surfaces of the target as well as the core composition determined by EDX after target slicing. The overall composition of the
  • elements in the target is fully homogeneous though it should be noted that the diameter of the used SEM-EDX probe beam is 1 µm. Thus, potential differences in the composition between the different crystallites with average diameters of 108 and 153 nm may not have been resolved. So, it is conceivable that
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Published 17 Jul 2025

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

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  • (Supporting Information File 1, Section S12) and the non-tilted condenser model was much easier to compute. To enable a more precise quantitative analysis, we first extensively characterized the gold nanospheres by both scanning and transmission electron microscopy (SEM and TEM, Supporting Information File 1
  • , Section S13) to determine the nanosphere’s shape, composition, diameter, and density. Both SEM and TEM showed that the nanospheres were indeed roughly spherical and of similar size (Supporting Information File 1, Section S13). Specifically, we measured the diameter of 35 nanospheres by SEM and obtained a
  • enables us to accurately calculate their expected radial intensity profiles and absorptions. We then collected 3D TXM images of nine different nanospheres, each of which had been pre-imaged by SEM to determine its diameter. Based on the SEM images, these nine nanospheres were selected to exclude the
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Published 15 Jul 2025

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

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  • occurred for all coatings. In particular, an increase in ion beam current led to a reduction in crystallite size by approximately 30% compared to coatings prepared by conventional EBE process. The average anatase crystallite size for annealed films was in the range of 30.8 to 43.5 nm. A detailed SEM
  • Fisher Scientific Raman Microscope), and SEM imaging (FEI Nova NanoSEM 230) were carried out to evaluate the structural properties and morphology of the prepared coatings. The optical characteristics of the prepared films were investigated with the use of an Ocean Optics QE65000 spectrophotometer in the
  • observed at approximately 139, 193, 393, 512, and 635 cm−1 confirms the occurrence of the anatase phase in the annealed coatings (Figure 2) [40][41]. Figure 3 presents SEM images of the surface and cross sections of TiO2 thin films before and after post-process annealing. In the case of as-prepared TiO2
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Published 14 Jul 2025

Multifunctional properties of bio-poly(butylene succinate) reinforced with multiwalled carbon nanotubes

  • Volodymyr Krasinskyi,
  • Krzysztof Bajer,
  • Ludmila Dulebova,
  • Nickolas Polychronopoulos,
  • Oksana Krasinska and
  • Daniel Kaczor

Beilstein J. Nanotechnol. 2025, 16, 1014–1024, doi:10.3762/bjnano.16.76

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  • . The surface morphology of the original substances and the PBS/CNTs nanocomposites was studied using SEM (Figure 1). In Figure 1a, the typical surface structure of PBS is visible. CNTs appear as agglomerates ranging from 500 nm to 200 μm, composed of woven nanotubes with an outer diameter of 14 to 28
  • nm and a length of up to 40 μm (Figure 1b). The microstructure of PBS/CNT_10 (Figure 1c) and PBS/CNT_0.5 (Figure 1d) samples is quite similar. In the SEM images of both samples, small white inclusions (nanotubes) ranging from 24 to 200 nm in size are evenly distributed over the surface. On the
  • film sample made of original PBS (denoted PBS) was also prepared. A schematic diagram of the two-stage process for obtaining the nanocomposite and the film based on it is shown in Figure 8. Characterizations A scanning electron microscope (SEM), Hitachi SU8010 (Hitachi, Tokyo, Japan), was used to
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Published 03 Jul 2025

Shape, membrane morphology, and morphodynamic response of metabolically active human mitochondria revealed by scanning ion conductance microscopy

  • Eric Lieberwirth,
  • Anja Schaeper,
  • Regina Lange,
  • Ingo Barke,
  • Simone Baltrusch and
  • Sylvia Speller

Beilstein J. Nanotechnol. 2025, 16, 951–967, doi:10.3762/bjnano.16.73

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  • –sample interaction, often leading to an underestimation of mitochondrial apparent height due to applied cantilever pressure [22][25]. Similarly, scanning electron microscopy (SEM) offers high-resolution imaging but requires mitochondria to be chemically fixed, stained, and sectioned, which precludes the
  • membrane fluctuations; S6: SEM measurements of the polystyrene microspheres; S7: Details of the imaging dishes and SICM setup; S8: SEM measurements and other details of the nanopipettes; S9: Further information about the hopping mode at our SICM setup. Supporting Information File 4: Additional experimental
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Published 30 Jun 2025

Synthesis of biowaste-derived carbon-dot-mediated silver nanoparticles and the evaluation of electrochemical properties for supercapacitor electrodes

  • Navya Kumari Tenkayala,
  • Chandan Kumar Maity,
  • Md Moniruzzaman and
  • Subramani Devaraju

Beilstein J. Nanotechnol. 2025, 16, 933–943, doi:10.3762/bjnano.16.71

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  • storage. The size distribution, morphology, and crystallinity of PG-CDs-AgNPs were further characterized by SEM and TEM analysis. The SEM image of PG-CDs-AgNPs (Supporting Information File 1, Figure S2a) reveals that PG-CDs-AgNPs possess spherical and distorted spherical structure. Supporting Information
  • Information Supporting Information File 2: Experimental procedures including materials details and characterizations; Schematic representation; BET isotherm and pore size distribution plot; SEM, EDX, and elemental mapping of PG-CDs-AgNPs; ASC device fabrication method; Table for the comparison of cyclic
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Published 24 Jun 2025

Structural and magnetic properties of microwave-synthesized reduced graphene oxide/VO2/Fe2O3 nanocomposite

  • Sumanta Sahoo,
  • Ankur Sood and
  • Sung Soo Han

Beilstein J. Nanotechnol. 2025, 16, 921–932, doi:10.3762/bjnano.16.70

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  • and 6.50 mA using an Al Kα. The morphologies and elemental analyses of rGO and the NCs were analyzed through scanning electron microscopy (SEM, Hitachi, S-4800). The structural analysis of these fabricated NCs was examined using high-resolution transmission electron microscopy (HRTEM, FEI Tecnai G2
  • exfoliation of graphene sheets. On the other hand, the SEM micrograph of GVF demonstrates the dispersion of the nanorods of VO2 and NPs on Fe2O3 on the graphene surface (Figure 4c,d). It is important to note that the morphological analysis of GVF displays a porous nature, which is also favorable for
  • demonstrating improved magnetic characteristics due to alterations in the electronic structure. To further comprehend the elemental composition of GVF, the elemental analysis was also performed, and the corresponding elemental distribution and EDX spectrum are shown in Figure 5a,b. The SEM image displays a wide
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Published 20 Jun 2025

Focused ion beam-induced platinum deposition with a low-temperature cesium ion source

  • Thomas Henning Loeber,
  • Bert Laegel,
  • Meltem Sezen,
  • Feray Bakan Misirlioglu,
  • Edgar J. D. Vredenbregt and
  • Yang Li

Beilstein J. Nanotechnol. 2025, 16, 910–920, doi:10.3762/bjnano.16.69

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  • of the ion beam is specified as ranging from 10 to 159 nm, changing with acceleration voltage (5, 8, 16, and 30 kV) and ion beam current. The actual thickness of each layer was measured with a standard cross section using the Ga+ FIB. All scanning electron microscopy (SEM) images were taken with the
  • . All deposition parameters are shown in Table 1. To calculate the resistivity of the deposits, the NanoLab 650 dual beam system was used to determine the length and the cross section of each deposited layer. The TEM lamellas were prepared with a JEOL JIB 4601F FIB-SEM MultiBeam system. The sample
  • layers, which have a length of 40 μm and a width 1 μm, were deposited across the boundary between the bare Si and the Si with its native oxide intact. A visual inspection with the SEM reveals surface bubbles on layers deposited at 2 and 5 kV (as shown in Figure 1a). No significant differences can be seen
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Published 16 Jun 2025

Characterization of ion track-etched conical nanopores in thermal and PECVD SiO2 using small angle X-ray scattering

  • Shankar Dutt,
  • Rudradeep Chakraborty,
  • Christian Notthoff,
  • Pablo Mota-Santiago,
  • Christina Trautmann and
  • Patrick Kluth

Beilstein J. Nanotechnol. 2025, 16, 899–909, doi:10.3762/bjnano.16.68

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  • and a wider size distribution. Results and Discussions Figure 1 shows plan-view scanning electron microscopy (SEM) images of nanopores fabricated in thermal (Figure 1a) and PECVD (Figure 1b) SiO2 by etching ion tracks produced with 1.6 GeV Au ion irradiation (see Experimental and Theory section for
  • values result from challenges in precisely defining nanopore boundaries due to charging effects during SEM imaging (see Figure 1). To address this, four cross-sectional measurements were taken across each pore and averaged. The standard deviation of these measurements provides the reported uncertainty
  • values. Although only three pores are shown, they illustrate the larger size variation in PECVD SiO2 compared to the uniform pore size in thermal SiO2. From SEM measurements, the standard deviation in the pore radius was measured to be ≈1.8 nm for thermal SiO2 but ≈8 nm for PECVD SiO2. The reader must
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Published 12 Jun 2025

Heat-induced transformation of nickel-coated polycrystalline diamond film studied in situ by XPS and NEXAFS

  • Olga V. Sedelnikova,
  • Yuliya V. Fedoseeva,
  • Dmitriy V. Gorodetskiy,
  • Yuri N. Palyanov,
  • Elena V. Shlyakhova,
  • Eugene A. Maksimovskiy,
  • Anna A. Makarova,
  • Lyubov G. Bulusheva and
  • Aleksandr V. Okotrub

Beilstein J. Nanotechnol. 2025, 16, 887–898, doi:10.3762/bjnano.16.67

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  • . Additionally, angle-resolved NEXAFS spectra of annealed Ni-coated SCD were measured to reveal the orientation of the formed graphitic layers. After synchrotron measurements, the samples were exposed to air and further analyzed using Raman spectroscopy and scanning electron microscopy (SEM). The obtained
  • (110) and (111) crystallographic planes on the surface of the PCD film (Supporting Information File 1, Figure S1b). The mapping did not show regions with the (100) orientation, although cubic faces are visible in the SEM images. The signal from these faces is probably weakened due to the tilt of the
  • the vacuum chamber for further SEM and Raman analysis under ambient conditions. Figure 4 shows SEM images of some large crystallites of about 100 μm in size on the surfaces of the annealed PCD and Ni-PCD. These crystallites have well-defined triangular (111) faces and truncated rectangular faces
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Published 12 Jun 2025

Synchrotron X-ray photoelectron spectroscopy study of sodium adsorption on vertically arranged MoS2 layers coated with pyrolytic carbon

  • Alexander V. Okotrub,
  • Anastasiya D. Fedorenko,
  • Anna A. Makarova,
  • Veronica S. Sulyaeva,
  • Yuliya V. Fedoseeva and
  • Lyubov G. Bulusheva

Beilstein J. Nanotechnol. 2025, 16, 847–859, doi:10.3762/bjnano.16.64

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  • . The scanning electron microscopy (SEM) images of the surface of raw MoS2 film, hydrogen-annealed film, and PyC film are compared in Figure 1b,c,e. The raw MoS2 film covers the entire area of the substrate and contains polysulfide nanoparticles on the surface (Figure 1b). These nanoparticles are absent
  • molybdenum layer sputtered for 90 s. Part of the film surface was covered with a protective Pt layer and a lamella was cut using a focused ion beam (FIB) system (see the Experimental section for details). Figure 1d shows the SEM image of the cross section of the lamella. The bright round spots on the film
  • different sizes formed during CVD synthesis (Figure 1b). The thickness of the MoS2 film estimated from the cross-sectional SEM image is about 33 nm (Figure 1d). Therefore, it can be estimated that the MoS2 film obtained using a molybdenum layer sputtered for 10 s has a thickness of no more than 4 nm. The
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Published 10 Jun 2025

Facile one-step radio frequency magnetron sputtering of Ni/NiO on stainless steel for an efficient electrode for hydrogen evolution reaction

  • Ha Huu Do,
  • Khac Binh Nguyen,
  • Phuong N. Nguyen and
  • Hoai Phuong Pham

Beilstein J. Nanotechnol. 2025, 16, 837–846, doi:10.3762/bjnano.16.63

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  • and metal oxide phases, offering a potential for HER. These outcomes indicated the successful Ni/NiO thin film fabrication on SS substrates. The uniformity of the electrocatalyst material is a vital factor that has a direct effect on electrode performance. Scanning electron microscopy (SEM) was
  • /SS-10 electrode for alkaline water electrolysis. To explain the high HER efficiency of the Ni/NiO/SS-10 electrode, we analyzed SEM and EDX after the stability test (Supporting Information File 1, Figure S5). It is noted that there is no significant change in the morphological structure and elemental
  • . Materials characterization The crystal structure of materials was confirmed by XRD using Cu Kα radiation with a wavelength of 0.154 nm on a X-ray diffractometer (D8 Advance, Bruker). The morphology of the obtained products was analyzed utilizing SEM on an S-4800 Hitachi. Chemical components and element
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Published 06 Jun 2025

Synthesis and magnetic transitions of rare-earth-free Fe–Mn–Ni–Si-based compositionally complex alloys at bulk and nanoscale

  • Shabbir Tahir,
  • Tatiana Smoliarova,
  • Carlos Doñate-Buendía,
  • Michael Farle,
  • Natalia Shkodich and
  • Bilal Gökce

Beilstein J. Nanotechnol. 2025, 16, 823–836, doi:10.3762/bjnano.16.62

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  • ground, polished, and analyzed by SEM (JEOL JSM-7600 F, Japan). The chemical composition was determined using energy-dispersive X-ray spectroscopy (EDX) with an Oxford Inca spectrometer. The crystal structure of bulk CCAs was characterized by X-ray diffraction (XRD) using a DRON-4–07 diffractometer with
  • diffractograms. EDX data was processed using AZtec software. Results and Discussion Microstructural characterization of bulk CCAs The SEM images and EDX elemental maps of the polished surface of the Ge-based CCA (Figure 2a) revealed a homogeneous microstructure, with no significant elemental segregation on the
  • by XRD peaks. The microsegregation of Mn can be due to a phenomenon consistent with observations in other CCAs, often attributed to the elastic strain energy [58] or due to the presence of oxygen on the surface forming MnO [59]. As expected, the SEM images and EDX elemental mapping of the polished Al
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Published 05 Jun 2025
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