Performance optimization of a microwave-coupled plasma-based ultralow-energy ECR ion source for silicon nanostructuring

• Joy Mukherjee,
• Safiul Alam Mollick,
• Tanmoy Basu and
• Tapobrata Som

Beilstein J. Nanotechnol. 2025, 16, 484–494, doi:10.3762/bjnano.16.37

• maximum eccentric tilt angle of ±70°. Sample preparation for cross sectional TEM measurement involved mechanically grinding the substrate into a circular disk with a diameter of 3 mm and a thickness of approximately 100 μm. The disk was then subjected to dimpling to achieve uniform thinning. To further

• sputtering of silicon oxide and the elemental silicon is different, which leads to instabilities during bombardment and the development of nanopatterns on the surface. Further, the exposure of the nanopatterned silicon surface to air during optical measurement ensures the formation of non-uniform silicon

ReactorAFM/STM – dynamic reactions on surfaces at elevated temperature and atmospheric pressure

• Tycho Roorda,
• Hamed Achour,
• Matthijs A. van Spronsen,
• Marta E. Cañas-Ventura,
• Sander B. Roobol,
• Willem Onderwaater,
• Mirthe Bergman,
• Peter van der Tuijn,
• Gertjan van Baarle,
• Johan W. Bakker,
• Joost W. M. Frenken and
• Irene M. N. Groot

Beilstein J. Nanotechnol. 2025, 16, 397–406, doi:10.3762/bjnano.16.30

• are deposited on an oxide layer representing realistic and relevant industrial catalysts. Here, the reaction conditions exceed the temperature limit of the qPlus sensor used in that measurement. Therefore, we show AFM images taken below the reaction temperature, before and after the reaction takes

Engineered PEG–PCL nanoparticles enable sensitive and selective detection of sodium dodecyl sulfate: a qualitative and quantitative analysis

• Soni Prajapati and
• Ranjana Singh

Beilstein J. Nanotechnol. 2025, 16, 385–396, doi:10.3762/bjnano.16.29

• within the 0.01 μg/mL measurement range, rendering the process cumbersome [21]. Also, an instrument is required among all the reported techniques, making detecting SDS at a target site complicated for the non-technical person. Therefore, there is an urge to develop a simple, colorimetric, rapid, nontoxic

• , UK). Dried 10 mg/mL PEG–PCL NPs were dissolved in PBS and sonicated for 30 min. The sonicated sample was taken in a cuvette for measurement. The sample pH was in the range of 7.2–7.4. Separate cuvettes (DTS1072 and DTS0012) were used to measure the surface charge and average size of the nanoparticles

• presence of peaks at 2349 and 2073 cm−1 might be due to ambient CO2 absorption or other environmental factors during measurement. This spectral analysis confirms the successful incorporation of PEG and PCL into the nanoparticle structure, showing their characteristic functional groups and molecular

Pulsed laser in liquid grafting of gold nanoparticle–carbon support composites

• Madeleine K. Wilsey,
• Teona Taseska,
• Qishen Lyu,
• Connor P. Cox and
• Astrid M. Müller

Beilstein J. Nanotechnol. 2025, 16, 349–361, doi:10.3762/bjnano.16.26

• slit, a 5.0 mm secondary slit, and a 2.5 mm anti-scatter screen, and a Lynxeye detector. Each measurement was performed with a resolution of 0.020° in 2θ and 0.5 s per step dwell time, resulting in approximately 40 min per sample. Background subtraction was performed using Bruker DIFFRAC.SUITE software

Tailoring of physical properties of RF-sputtered ZnTe films: role of substrate temperature

• Kafi Devi,
• Usha Rani,
• Arun Kumar,
• Divya Gupta and
• Sanjeev Aggarwal

Beilstein J. Nanotechnol. 2025, 16, 333–348, doi:10.3762/bjnano.16.25

• ZnTe film samples (width of film × thickness of film), and l corresponds to the distance between the probes (1 cm) while taking the measurement. The measured values of resistance, resistivity, and conductivity are presented in Table 5. The conductivity of the ZnTe films increases (from 1.42 × 10−8 to

Graphene oxide–chloroquine conjugate induces DNA damage in A549 lung cancer cells through autophagy modulation

• Braham Dutt Arya,
• Sandeep Mittal,
• Prachi Joshi,
• Alok Kumar Pandey,
• Jaime E. Ramirez-Vick,
• Govind Gupta and
• Surinder P. Singh

Beilstein J. Nanotechnol. 2025, 16, 316–332, doi:10.3762/bjnano.16.24

• (or comet assay) reveals a significant dose-dependent increase in tail length, tail DNA percentage, and Olive tail moment as a measurement of genotoxicity in GO–Chl-exposed A549 cells. To access the role of autophagy modulation by the GO–Chl nanoconjugate, we have employed MDC staining, confocal

• ), and deconvoluted fitting components (multicolored regions) are also shown here. Quantitative estimation of Chl binding onto GO nanosheets using UV–vis spectroscopy: (a) Optical density measurement of various concentrations (2.5–25 µg/mL) of Chl for the preparation of a standard calibration curve. (b

• ) Linearity plot (R2 ≈ 0.997) prepared by measuring the relative optical density for different concentrations of Chl, and (c) optical density measurement of the supernatant having unattached Chl. Analysis of cellular internalization of GO–Chl nanoconjugates in A549 cells: (a) Transmission electron micrographs

Enhancing mechanical properties of chitosan/PVA electrospun nanofibers: a comprehensive review

• Nur Areisman Mohd Salleh,
• Amalina Muhammad Afifi,
• Fathiah Mohamed Zuki and
• Hanna Sofia SalehHudin

Beilstein J. Nanotechnol. 2025, 16, 286–307, doi:10.3762/bjnano.16.22

• modulus (or elastic modulus) is a measurement of elasticity, which describes the stiffness of nanofibers and is calculated as the ratio of stress to strain in the elastic deformation region, which is the slope of the initial linear region of the stress–strain curve. Elongation at break measures the extent

• concentration because of improved coverage of the chitosan shell layer as observed from TEM images of the fiber. The different methods used in the measurement of chitosan/PVA nanofiber properties are summarized in Table 6. These methods allow for comprehensive characterization of the mechanical properties of

Radiosensitizing properties of dual-functionalized carbon nanostructures loaded with temozolomide

• Radmila Milenkovska,
• Nikola Geskovski,
• Dushko Shalabalija,
• Ljubica Mihailova,
• Petre Makreski,
• Dushko Lukarski,
• Igor Stojkovski,
• Maja Simonoska Crcarevska and
• Kristina Mladenovska

Beilstein J. Nanotechnol. 2025, 16, 229–251, doi:10.3762/bjnano.16.18

Synthesis and the impact of hydroxyapatite nanoparticles on the viability and activity of rhizobacteria

• Bedah Rupaedah,
• Indrika Novella,
• Atiek Rostika Noviyanti,
• Diana Rakhmawaty Eddy,
• Anna Safarrida,
• Abdul Hapid,
• Zhafira Amila Haqqa,
• Suryana Suryana,
• Irwan Kurnia and
• Fathiyah Inayatirrahmi

Beilstein J. Nanotechnol. 2025, 16, 216–228, doi:10.3762/bjnano.16.17

• ) and precise digital measurement of electrical conductivity (Mettler Toledo, MC 226 conductivity meter). Preparation of inoculum and formulation of rhizobacteria-nHA nHA was carefully placed into 2 mL EP tubes and underwent sterilization through autoclaving. The rhizobacteria were introduced into

Probing the potential of rare earth elements in the development of new anticancer drugs: single molecule studies

• Josiane A. D. Batista,
• Rayane M. de Oliveira,
• Carlos H. M. Lima,
• Milton L. Lana Júnior,
• Virgílio C. dos Anjos,
• Maria J. V. Bell and
• Márcio S. Rocha

Beilstein J. Nanotechnol. 2025, 16, 187–194, doi:10.3762/bjnano.16.15

• the two main mechanical parameters in the entropic regime, that is, the contour and persistence lengths of the DNA molecule. To guarantee the accuracy of the results, the chosen DNA is stretched using only low forces (<5 pN); this type of measurement is repeated six times, obtaining the average values

Characterization of ZnO nanoparticles synthesized using probiotic Lactiplantibacillus plantarum GP258

• Prashantkumar Siddappa Chakra,
• Aishwarya Banakar,
• Shriram Narayan Puranik,
• Vishwas Kaveeshwar,
• C. R. Ravikumar and
• Devaraja Gayathri

Beilstein J. Nanotechnol. 2025, 16, 78–89, doi:10.3762/bjnano.16.8

• the scattering angle. Using this formula, we determined an average crystallite size of around 25 nm for the 2θ angle of 35.8°. This measurement provided valuable insight into the dimensions of the ZnO NPs and is depicted in Figure 2a. FTIR analysis The FTIR spectra of ZnO NPs were examined in the

• ) EDX spectroscopy for elemental composition. (e) Zeta potential measurement. (f) DLS results showing the size distribution of ZnO NPs. (a, b) Cyclic voltammetry response of the ZnO electrode in 0.1 M KCl solution at varying scan rates, showing redox behavior and electron transfer characteristics. (c

Instance maps as an organising concept for complex experimental workflows as demonstrated for (nano)material safety research

• Benjamin Punz,
• Maja Brajnik,
• Joh Dokler,
• Jaleesia D. Amos,
• Litty Johnson,
• Katie Reilly,
• Anastasios G. Papadiamantis,
• Amaia Green Etxabe,
• Lee Walker,
• Diego S. T. Martinez,
• Steffi Friedrichs,
• Klaus M. Weltring,
• Nazende Günday-Türeli,
• Claus Svendsen,
• Christine Ogilvie Hendren,
• Mark R. Wiesner,
• Martin Himly,
• Iseult Lynch and
• Thomas E. Exner

Beilstein J. Nanotechnol. 2025, 16, 57–77, doi:10.3762/bjnano.16.7

• be linked to the corresponding resources documenting the steps in the form of text documents, protocol repository entries, or ELN pages. For data produced in the study, a strong linkage between protocols and data using a workflow with stages for sample preparation, measurement, raw data (collection

• /samples (instances), characteristics and endpoints to be collected (experimentally and via text/database mining), and nodes describing modification steps applied to materials and samples (transformation protocols) and testing SOPs (sample preparation, measurement, and data processing), as described in the

• of properties in combination with sample preparation, measurement, and processing protocols, as well as the resulting data. For example, the combination of sample preparation → measurement → raw data → processing → processed data, could be placed before or after the node defining the measured

Advanced atomic force microscopy techniques V

• Philipp Rahe,
• Ilko Bald,
• Nadine Hauptmann,
• Regina Hoffmann-Vogel,
• Harry Mönig and
• Michael Reichling

Beilstein J. Nanotechnol. 2025, 16, 54–56, doi:10.3762/bjnano.16.6

• not involving any tip–surface interaction. The measurement of electrostatic properties at the nanoscale emerged as a most relevant subfield of atomic force microscopy, especially driven by electrostatic force microscopy (EFM), Kelvin probe force microscopy (KPFM), and closely related techniques

• cantilever eigenmode, which is particularly relevant when generating the time-periodic potential by optical or electrical pumping. With this development, the authors could present the detection of modulated components that are below the detection limit of other KPFM measurement modes. Da Lisca et al

• doping of the graphene nanoribbons is reflected by the local work function. They also measure and calculate the local work function as a function of tip–sample distance and compare results to those of simple electrostatic models of a graphene nanoribbon, validating the overall approach of measurement and

Precursor sticking coefficient determination from indented deposits fabricated by electron beam induced deposition

• Alexander Kuprava and
• Michael Huth

Beilstein J. Nanotechnol. 2025, 16, 35–43, doi:10.3762/bjnano.16.4

• regime assumptions. This favors shorter deposition times and consequently results in a height decrease. On the other hand, to reliably resolve deposit profile and reduce measurement errors, the height should not be too small. The chosen exposure time for each deposit was eventually a compromise between

Bioinspired nanofilament coatings for scale reduction on steel

• Siad Dahir Ali,
• Mette Heidemann Rasmussen,
• Jacopo Catalano,
• Christian Husum Frederiksen and
• Tobias Weidner

Beilstein J. Nanotechnol. 2025, 16, 25–34, doi:10.3762/bjnano.16.3

• for the coated and uncoated samples. (A) SEM image of the SNF coating after the shear stress test. The SNF coating is still visible. (B) Composition of the SNF-coated steel before and after the shear stress test based on EDX analysis. (C) Image showing the contact angle measurement of the sample after

Orientation-dependent photonic bandgaps in gold-dust weevil scales and their titania bioreplicates

• Norma Salvadores Farran,
• Limin Wang,
• Primoz Pirih and
• Bodo D. Wilts

Beilstein J. Nanotechnol. 2025, 16, 1–10, doi:10.3762/bjnano.16.1

• the replica, and the increase of the fill fraction. The measured reflectance spectra, both of the native templates and the replicas, are broader than those produced by the idealized model. This difference is partially attributed to the measurement geometry: While the model assumes a plane wave, in the

• of the side port’s tube lens. The light was reflected to the side via a slide-in mirror and focused by the tube lens on a 200 μm fiber (FC-UVIR200, Avantes, Apeldoorn NL EU) attached to a CCD spectrometer (AvaSpec-ULS2048XL-EVO, Avantes). The measurement spot could be translated using the micrometer

Mechanistic insights into endosomal escape by sodium oleate-modified liposomes

• Ebrahim Sadaqa,
• Satrialdi,
• Fransiska Kurniawan and
• Diky Mudhakir

Beilstein J. Nanotechnol. 2024, 15, 1667–1685, doi:10.3762/bjnano.15.131

• transformation of resazurin (initially blue and non-fluorescent) into resorufin (pink and fluorescent) by metabolically active cells, facilitating the measurement of cell viability [35][36]. Briefly, 4T1 cells were cultured in DMEM supplemented with 10% FBS and 1% penicillin–streptomycin in a humidified

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

• technical capabilities of modern TEMs allow for the measurement of object sizes with high accuracy, directly on the computer monitor of a digital camera. Determining the sizes is important for identifying the types of LPs and EVs. TEM was the main method of our study, the aim of which was to visualize the

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

• -spacings of the outer shells are indicated with yellow lines). SAED measurement locations and patterns for (a, b) nanofibres and (c, d) NPs obtained in DW. EDX spectra and elemental composition of (a) HfNPs-D, (b) HfNPs-T, and (c) HfNPs-A. Reflectance spectra of NPs drop-cast on Si substrates measured

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

• supernatant. GPx activity was defined as the formation of 1 mg of purpurogallin from pyrogallol in 20 s. Liver GPx activity was calculated using the formula: where A is the enzyme activity in pkat, ΔD is the change in optical density, t is the measurement time in seconds, and c is the protein concentration

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

• edge filter using 532 nm as an excitation source. The Raman signal of the silicon wafer at 520 cm−1 was considered the reference point for spectrometer calibration, ensuring a spectral measurement accuracy better than 1 cm−1. The Raman spectra acquisition times were approximately 25 s for solid ʟ

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

• the MOFs. A sensor for simultaneously detecting hydroquinone and catechol in water using a Cu-MOF–graphene composite was developed by Li and colleagues. Measurement ranges beginning at 1.0 × 10−6 and 1.0 × 10−3 M were achieved, with LODs of 5.9 × 10−7 M and 3.3 × 10−7 M for hydroquinone and catechol

• require shorter times to reach equilibrium. Repeatability and reproducibility of the (Cu)(Fe)BTC@CPE electrode Figure 11a depicts eight successive measurements conducted in 0.20 µM ENR solution using a single electrode without renewing the electrode surface. Clearly, in the second measurement, the ENR

• electrode reproducibility performance was evaluated by comparing SWV signals in 0.2 µM ENR solution obtained on an electrode whose surface was renewed before each measurement (Figure 11b). The data indicated slight fluctuations in peak currents among eight measurements, with a relative standard deviation

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 driving coherent interactions with the organic semiconductor molecules. Secondly, enabling the measurement of the evolution of stored energy and the differential reflectivity induced by the pump pulse, which is essential for monitoring the charging dynamics at a femtosecond resolution. The

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

• photodetectors. Keywords: broken inversion symmetry; out-of-plane polarization; picosecond photoresponse; time-resolved photocurrent measurement (TRPC); WSe2; Introduction Two-dimensional (2D) van der Waals (vdW) ferroelectrics with dangling-bond-free surfaces exhibit ferroelectricity by effectively resisting

• ][41][42]. Figure 2b shows the power-law relationship between photocurrent (Iph) and excitation power (P), Iph = P0.6, indicating that the photocurrent exhibits sublinear growth, consistent with the saturation effect. In Figure 2c, the TRPC measurement curve shows a symmetric dip at zero time delay

• ) at room temperature. The electrical properties of the devices were characterized using an Agilent B1500 semiconductor analyzer in a Lake Shore vacuum chamber (10−4 Pa). SPCM and TRPC measurement The photocurrent maps were all obtained under zero bias using a custom-built scanning photocurrent

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

• . Otherwise, the critical temperature of the structures would vary significantly, which we do not observe, as shown below. Cryogenic Measurement Results Low-temperature measurements of the chips with structures were performed in a Triton 200 dilution cryostat. The chips were placed in a 16-pin sample holder

• critical temperature of sample A3 compared to the others is due to the lower measurement current. The resistance peak on the R(T) dependence for samples A1 and A2 (Figure 3a and Figure 3b) may appear due to non-equilibrium effects and the presence of NS borders in the setup [16][17]. But presently, we have