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Search for "step" in Full Text gives 1509 result(s) in Beilstein Journal of Nanotechnology. Showing first 200.

Time of flight secondary ion mass spectrometry imaging of contaminant species in chemical vapour deposited graphene on copper

  • Barry Brennan,
  • Vlad-Petru Veigang-Radulescu,
  • Philipp Braeuninger-Weimer,
  • Stephan Hofmann and
  • Andrew J. Pollard

Beilstein J. Nanotechnol. 2026, 17, 200–213, doi:10.3762/bjnano.17.13

Graphical Abstract
  • of the material and lead to a step change in terms of high speed [11][12][13], transparent [14] and flexible electronic devices [15], membranes [16][17], and sensors [18][19]. A large amount of work has been dedicated to the optimisation of the growth process to aid in the formation of large area
  • were prepared as described in detail previously [43]. For two of the samples, (labelled Ar and Ar:H2) the as-received Cu foils were used without any pre-treatment. The other two samples (labelled EP and BO) underwent two different pre-treatments, namely, either an electro-polishing step intended to
  • precursor was introduced for 30 min. The graphene growth atmosphere consisted of 250 SCCM Ar, 26 SCCM H2 and 9 SCCM CH4 (0.1% diluted in Ar) for all samples except the BO sample where a flow rate of 30 SCCM CH4 (0.1% diluted in Ar) was used due to the very low nucleation density. After the growth step the
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Published 21 Jan 2026

Influence of surface characteristics on the in vitro stability and cell uptake of nanoliposomes for brain delivery

  • Dushko Shalabalija,
  • Ljubica Mihailova,
  • Nikola Geskovski,
  • Andreas Zimmer,
  • Otmar Geiss,
  • Sabrina Gioria,
  • Diletta Scaccabarozzi and
  • Marija Glavas Dodov

Beilstein J. Nanotechnol. 2026, 17, 139–158, doi:10.3762/bjnano.17.9

Graphical Abstract
  • concentrations of 5, 10 or 100 μg/mL). Incubation was performed for 1, 2, and 4 h (37 °C, 5% CO2), followed by a washing step with PBS and lysis with 2% Triton X-100 (2 h, 37 °C, 5% CO2). The resulting fluorescence was measured on a plate reader at an excitation wavelength of 535 nm and an emission wavelength of
  • at the initial time points of incubation) contains more proteins than the hard corona formed at later time intervals, resulting in a larger particle diameter at early incubation periods. High-resolution automated electrophoresis of adsorbed proteins onto the nanoliposomal surface In the next step
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Published 13 Jan 2026

Capabilities of the 3D-MLSI software tool in superconducting neuron design

  • Irina E. Tarasova,
  • Nikita S. Shuravin,
  • Liubov N. Karelina,
  • Fedor A. Razorenov,
  • Evgeny N. Zhardetsky,
  • Aleksandr S. Ionin,
  • Mikhail M. Khapaev and
  • Vitaly V. Bol’ginov

Beilstein J. Nanotechnol. 2026, 17, 122–138, doi:10.3762/bjnano.17.8

Graphical Abstract
  • increase in the main mesh step to ah = 2 μm and the edge step to ahb = 0.25 μm in order to meet the limitations on the amount of allocated RAM and execution time (see Section “Extraction Details”). Results are presented in Figure 6 as a dependence of calculated vs measured values, similar to Figure 3 and
  • . Calculations are performed on a highly graded mesh of triangular cells (see inset on Figure 8a) based on two mesh step parameters. The first parameter, ah, defines the size of triangular cells inside the superconducting film far enough from the nearest boundary. The other parameter, ahb, is related to the cell
  • step ah, which is related to the complexity of assembling the matrix O(N2). Thus, for the most accurate calculations performed on structures of the smallest size (C-shaped two-junction SQUIDs, Figure 2), the smallest steps ah = 1 μm and ahb = 0.125 μm (default parameters) were chosen. For certain
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Published 13 Jan 2026

Development and in vitro evaluation of liposomes and immunoliposomes containing 5-fluorouracil and R-phycoerythrin as a potential phototheranostic system for colorectal cancer

  • Raissa Rodrigues Camelo,
  • Vivianne Cortez Sombra Vandesmet,
  • Octavio Vital Baccallini,
  • José de Brito Vieira Neto,
  • Thais da Silva Moreira,
  • Luzia Kalyne Almeida Moreira Leal,
  • Claudia Pessoa,
  • Daniel Giuliano Cerri,
  • Maria Vitória Lopes Badra Bentley,
  • Josimar O. Eloy,
  • Ivanildo José da Silva Júnior and
  • Raquel Petrilli

Beilstein J. Nanotechnol. 2026, 17, 97–121, doi:10.3762/bjnano.17.7

Graphical Abstract
  • , SPC) and amount (25 and 50 mg) followed by sonication. In summary, the lipids were solubilized in 5 mL of chloroform and evaporated for 30 min at 65 °C. In the next step, the lipid film was hydrated with 5 mL of phosphate buffer saline (PBS, pH 7.4) during 60 min at 100 rpm and 37 °C or with PBS, pH
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Published 09 Jan 2026

Functional surface engineering for cultural heritage protection: the role of superhydrophobic and superoleophobic coatings – a comprehensive review

  • Giuseppe Cesare Lama,
  • Marino Lavorgna,
  • Letizia Verdolotti,
  • Federica Recupido,
  • Giovanna Giuliana Buonocore and
  • Bharat Bhushan

Beilstein J. Nanotechnol. 2026, 17, 63–96, doi:10.3762/bjnano.17.6

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  • imparting long-lasting hydrophobicity, reducing water uptake, and maintaining dimensional and biological stability of wood, even under UV exposure and outdoor conditions (Figure 7). To do so, nano/sub-microlignin (NL), derived from beechwood via a one-step organosolv process, was used as a filler and
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Published 07 Jan 2026

Reduced graphene oxide paper electrode for lithium-ion cells – towards optimized thermal reduction

  • Agata Pawłowska,
  • Magdalena Baran,
  • Stefan Marynowicz,
  • Aleksandra Izabela Banasiak,
  • Adrian Racki,
  • Adrian Chlanda,
  • Tymoteusz Ciuk,
  • Marta Wolczko and
  • Andrzej Budziak

Beilstein J. Nanotechnol. 2026, 17, 24–37, doi:10.3762/bjnano.17.3

Graphical Abstract
  • easy to scale up and, which is worth emphasizing, eliminates the use of any binder or harmful solvent. In order to obtain rGO paper sheets, the produced paper sheets underwent a mild, three-step thermal procedure described in [34] (i.e., sample M300 mentioned in the current article) with further
  • modification, that is, an additional thermal step was applied. For this research, three different additional steps were applied, namely, 400, 600, and 800 °C (the samples were named accordingly T400, T600, and T800). The additional thermal step was conducted for 6 h in an inert atmosphere in a tube furnace
  • eV (0.1 eV step) pass energy in the analyzer and the photoelectron take-off angle at 45°. In order to maintain a constant sample surface potential, a dual beam charge compensation with 7 eV Ar+ ions and 1 eV electrons was used. The aliphatic carbon C 1s line at 285.0 eV was used as a charge reference
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Published 05 Jan 2026

Quantitative estimation of nanoparticle/substrate adhesion by atomic force microscopy

  • Aydan Çiçek,
  • Markus Kratzer,
  • Christian Teichert and
  • Christian Mitterer

Beilstein J. Nanotechnol. 2026, 17, 1–14, doi:10.3762/bjnano.17.1

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  • conditions influence how Cu NP move and detach during manipulation. Similar trajectories as observed by Rao et al. occurred very rarely in our experiments. In this study, a frequently applied standard protocol for AFM manipulation was used [32]. The protocol consists of a two-step method and is schematically
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Published 02 Jan 2026

Internal 3D temperature mapping in biological systems using ratiometric light-sheet imaging and lipid-coated upconversion nanothermometers

  • Dannareli Barron-Ortiz,
  • Enric Pérez-Parets,
  • Rubén D. Cadena-Nava,
  • Emilio J. Gualda,
  • Jacob Licea-Rodríguez,
  • Juan Hernández-Cordero,
  • Pablo Loza-Álvarez and
  • Israel Rocha-Mendoza

Beilstein J. Nanotechnol. 2025, 16, 2306–2316, doi:10.3762/bjnano.16.159

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  • essential step for advancing non-invasive thermal imaging in living biological systems. We recently demonstrated the feasibility of combining light-sheet fluorescence microscopy (LSFM) with UC micro- and nanocomposites for volumetric temperature mapping across scales ranging from tens of micrometers to
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Published 22 Dec 2025

Terahertz-range on-chip local oscillator based on Josephson junction arrays for superconducting quantum-limited receivers

  • Fedor V. Khan,
  • Lyudmila V. Filippenko,
  • Andrey B. Ermakov,
  • Mikhail Yu. Fominsky and
  • Valery P. Koshelets

Beilstein J. Nanotechnol. 2025, 16, 2296–2305, doi:10.3762/bjnano.16.158

Graphical Abstract
  • quasiparticle current step more than 0.25 of the current at the gap voltage of the mixer junction. Second, the oscillator frequency should be tunable in a wide range. Third, the ability to phase-lock to the external stable synthesizer should be implemented. Fourth, the spectral ratio (ratio of the signal power
  • tunneling through the tunnel barrier increases. This leads to a rise in current at voltages below the gap and the emergence of the so-called quasiparticle steps. This process is known as photon-assisted tunneling. The magnitude of the current on a quasiparticle step within the investigated range is linearly
  • section we will discuss the results of the spectral measurements and the feasibility of the LO in SIR based on a JJ array of the proposed topology. First, for the SIR to operate, the power of the LO coupled to the SIS junction induces the current on the quasiparticle step greater than 25% of the Ig [13
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Published 22 Dec 2025

Chiral plasmonic nanostructures fabricated with circularly polarized light

  • Tian Qiao and
  • Ming Lee Tang

Beilstein J. Nanotechnol. 2025, 16, 2245–2264, doi:10.3762/bjnano.16.154

Graphical Abstract
  • ]. The simulations considered the polarization vectors of the incident light. The dissymmetric shapes of the gold nano-twisters led to the mixing of different plasmon modes, generating a nonzero CD. The first step in calculating the CD of experimentally obtained cPNSs is to import the morphological
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Published 08 Dec 2025

Optical bio/chemical sensors for vitamin B12 analysis in food and pharmaceuticals: state of the art, challenges, and future outlooks

  • Seyed Mohammad Taghi Gharibzahedi and
  • Zeynep Altintas

Beilstein J. Nanotechnol. 2025, 16, 2207–2244, doi:10.3762/bjnano.16.153

Graphical Abstract
  • lysosomes in a distinct base-off conformation. In this process, the protein replaces the 5,6-dimethylbenzimidazole ligand of VB12 with one of its histidine residues. Furthermore, MMACHC plays a pivotal role in converting all variants of VB12 into the cob(II)alamin intermediate. This crucial step includes
  • , and the β-oxidation of odd-chain fatty acids [34]. This function of Ado-Cbl in the body supports energy production by facilitating the conversion of methylmalonyl-CoA to succinyl-CoA, a key step in the Krebs cycle, which is central to cellular energy generation [61]. The metabolic pathway of VB12 in
  • –citrate buffer at pH 4.5. This buffer was then added to an infant formula sample, which was subsequently autoclaved at 121 °C for 25 min. The purpose of this step was to denature the VB12 binding protein present in the sample and liberate the vitamin for the subsequent analysis. Low repeatability based on
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Published 05 Dec 2025

Ultrathin water layers on mannosylated gold nanoparticles

  • Maiara A. Iriarte Alonso,
  • Jorge H. Melillo,
  • Silvina Cerveny,
  • Yujin Tong and
  • Alexander M. Bittner

Beilstein J. Nanotechnol. 2025, 16, 2183–2198, doi:10.3762/bjnano.16.151

Graphical Abstract
  • functionalization was performed as reported in [24]. Silicon wafers were washed first in methanol, then in a 1:1 v/v mixture of methanol and chloroform, and finally in chloroform under 5 min sonication at every step. Afterwards, the surfaces were immersed in a 7:2:1 (v/v) mixture of decalin (cis and trans)/toluene
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Published 04 Dec 2025

Hartree–Fock interaction in superconducting condensate fractals

  • Edward G. Nikonov,
  • Yajiang Chen,
  • Mauro M. Doria and
  • Arkady A. Shanenko

Beilstein J. Nanotechnol. 2025, 16, 2177–2182, doi:10.3762/bjnano.16.150

Graphical Abstract
  • the entire procedure is repeated until convergence is achieved. The calculation is considered converged when the relative changes in the order parameter and the HF field are below 10−7. To model quasicrystal superconducting properties, as the first step, we consider a finite Fibonacci sequence
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Published 04 Dec 2025

Missing links in nanomaterials research impacting productivity and perceptions

  • Santosh K. Tiwari and
  • Nannan Wang

Beilstein J. Nanotechnol. 2025, 16, 2168–2176, doi:10.3762/bjnano.16.149

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  • . This registry would catalog product categories, safety data, and approved applications, facilitating transparency, traceability, and coordinated post-market surveillance. A further step would be the formation of a global regulatory authority analogous to the international council for harmonization in
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Published 03 Dec 2025

Quality by design optimization of microemulsions for topical delivery of Passiflora setacea seed oil

  • Daniel T. Pereira,
  • Douglas Dourado,
  • Danielle T. Freire,
  • Dayanne L. Porto,
  • Cícero F. S. Aragão,
  • Myla L. de Souza,
  • Guilherme R. S. de Araujo,
  • Ana Maria Costa,
  • Wógenes N. Oliveira,
  • Anne Sapin-Minet,
  • Éverton N. Alencar and
  • Eryvaldo Sócrates T. Egito

Beilstein J. Nanotechnol. 2025, 16, 2116–2131, doi:10.3762/bjnano.16.146

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  • step when non-normal distribution is detected [25]. Following transformation, analysis of variance (ANOVA) was conducted to evaluate the statistical significance of the overall model and the individual formulation factors. To enhance model parsimony, backward regression elimination was applied to
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Published 20 Nov 2025

Calibration of piezo actuators and systems by dynamic interferometry

  • Knarik Khachatryan and
  • Michael Reichling

Beilstein J. Nanotechnol. 2025, 16, 2086–2091, doi:10.3762/bjnano.16.143

Graphical Abstract
  • -step fit method based on Equation 1 as detailed in [13]. Here, VDC represents the DC part of the interferometer signal voltage, V0 is the voltage amplitude of the modulated signal, and φ is the phase shift introduced by the electronics in the signal path, which may be determined from the fit
  • interferometer, various voltages are applied to the fiber tube piezo, and, after each step of voltage change, the cantilever excitation voltage is varied from 1 V to 7 V in steps. For each step, the interferometer signal is analyzed to extract the oscillation amplitude A corresponding to the respective voltage
  • step. Figure 2 shows plots of A against the cantilever excitation voltage Vexc, where the data are fitted by straight lines. Note that all straight lines should coincide; however, they are shifted for each step along the Vexc axis for better clarity. The measurements presented in Figure 2a have been
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Published 17 Nov 2025

Multifrequency AFM integrating PeakForce tapping and higher eigenmodes for heterogeneous surface characterization

  • Yanping Wei,
  • Jiafeng Shen,
  • Yirong Yao,
  • Xuke Li,
  • Ming Li and
  • Peiling Ke

Beilstein J. Nanotechnol. 2025, 16, 2077–2085, doi:10.3762/bjnano.16.142

Graphical Abstract
  • include topographic step-like distortions and sudden phase-contrast inversions arising from bistable transitions between co-existing oscillation states, which complicate data interpretation [13][14][15][16][17]. Additionally, operational complexity escalates in liquid environments, where low-quality
  • ) and a stiff probe (NSC15/Al BS) demonstrates that our method yields closely matched topography (~4 nm step height between the thinner and thicker nanosheet regions), confirming the robust height fidelity of the present approach. Quantitative modulus maps exhibit pronounced probe-dependence; the soft
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Published 17 Nov 2025

Molecular and mechanical insights into gecko seta adhesion: multiscale simulations combining molecular dynamics and the finite element method

  • Yash Jain,
  • Saeed Norouzi,
  • Tobias Materzok,
  • Stanislav N. Gorb and
  • Florian Müller-Plathe

Beilstein J. Nanotechnol. 2025, 16, 2055–2076, doi:10.3762/bjnano.16.141

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  • geometry was sufficient as a first step in validating our concurrent MD–FEM approach and extracting fundamental insights about contact formation, load transfer, and spatula detachment mechanisms. Simulating each spatula in its own MD simulation, while coupling them all with the seta FEM model, becomes
  • greater mesh deformation and, thus, represents a larger step towards the final FEM solution. This requires fewer iterations but also increases the risk of numerical instabilities. Conversely, a larger spring constant results in smaller steps towards equilibrium but requires more iterations. External
  • loading (e.g., displacement or force) on the full system, such as moving the entire seta, is applied in increments called load steps. Each load step consists of (1) applying a portion of the total load (a displacement of 1 nm in our case) to the driver nodes and (2) running multiple FEM–MD iterations (ten
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Published 14 Nov 2025

Stereodiscrimination of guests in chiral organosilica aerogels studied by ESR spectroscopy

  • Sebastian Polarz,
  • Yasar Krysiak,
  • Martin Wessig and
  • Florian Kuhlmann

Beilstein J. Nanotechnol. 2025, 16, 2034–2054, doi:10.3762/bjnano.16.140

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  • according to [64], and the racemate was separated by fractional crystallization using (S)-(−)-1-phenylethylamine for (+)-3CP and (R)-(+)-1-phenylethylamine for (−)-3CP as indicated in Supporting Information File 1, Figure S10. The enantiomeric purity was checked after each crystallization step using the
  • ), we prepared two new materials, namely, TEMPONHxSIL and TEMPONHyoSIL (Figure 12). Via amide coupling chemistry, in a post-functionalization step, we attached a pentafluorophenol-activated 4-carboxy-2,2,6,6-tetramethylpiperidinyloxyl (R = TEMPO; Figure 12) group. The reaction delivers an ESR-active
  • ). One sees in Figure 13b that already for x > 0.05, the distance between the TEMPO units is around 1.4 nm. One may assume that a larger number of amines/x does not necessarily lead to a higher degree of functionalization in the post-functionalization step. The introduction of phenyl spacers in the oSIL
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Published 13 Nov 2025

Beyond the shell: exploring polymer–lipid interfaces in core–shell nanofibers to carry hyaluronic acid and β-caryophyllene

  • Aline Tavares da Silva Barreto,
  • Francisco Alexandrino-Júnior,
  • Bráulio Soares Arcanjo,
  • Paulo Henrique de Souza Picciani and
  • Kattya Gyselle de Holanda e Silva

Beilstein J. Nanotechnol. 2025, 16, 2015–2033, doi:10.3762/bjnano.16.139

Graphical Abstract
  • preparation, a flow rate ratio of 6.25 was maintained, with an outer flow rate of 0.25 mL/h and an inner flow rate of 0.04 mL/h, as this ratio prevented severe dripping and ensured a more stable Taylor cone. Having characterized the influence of core composition on fiber formation, the next step involved
  • polymer powders, sieving was conducted using an ASTM 70 mesh (212 µm) before compressing the powders onto the sample holder to ensure grain homogeneity. The analyses were carried out using a LabX XRD-6100 diffractometer (Shimadzu, Japan) in an angle ranging from 2° to 50° (2θ), using a step size of 0.02
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Published 12 Nov 2025

Laser ablation in liquids for shape-tailored synthesis of nanomaterials: status and challenges

  • Natalie Tarasenka

Beilstein J. Nanotechnol. 2025, 16, 1963–1997, doi:10.3762/bjnano.16.137

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  • by unfocused laser irradiation as a second step. This strategy has developed into several methods usually categorized as laser-induced fragmentation, laser-induced melting, or laser-induced modification. Such multistep processes open up ways for precise manipulation and fine tuning of NP parameters
  • in acetone–water solution to induce further re-shaping into cubic nanostructures (Figure 7b–d). The formation of the nanocubes occurred upon ageing of the colloid during several days, and the authors emphasize the importance of the laser fragmentation step in this process. If the laser fluence is too
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Published 10 Nov 2025

Evaluating metal-organic precursors for focused ion beam-induced deposition through solid-layer decomposition analysis

  • Benedykt R. Jany,
  • Katarzyna Madajska,
  • Aleksandra Butrymowicz-Kubiak,
  • Franciszek Krok and
  • Iwona B. Szymańska

Beilstein J. Nanotechnol. 2025, 16, 1942–1951, doi:10.3762/bjnano.16.135

Graphical Abstract
  • -organic precursors involves a series of steps that are crucial to ensure accurate and comprehensive results. These stages include: (1) Deposition of the precursor onto a Si(111) substrate through sublimation using previously established parameters [22][29][32][34]. This step allows for precise control of
  • hyperspectral data, which involves acquiring multiple X-ray spectra from different points of the final sample morphology. This step allows for a more detailed analysis of the chemical composition and distribution of elements within the irradiated sample. (5) Decomposing SEM EDX hyperspectral data using advanced
  • technique, which is a high-resolution analytical method that can provide elemental information at the nanoscale. This step ensures precise identification and quantification of all elements present in the grown structures. (7) The final step involves examining the chemical composition of the resulted
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Published 04 Nov 2025

Programmable soliton dynamics in all-Josephson-junction logic cells and networks

  • Vsevolod I. Ruzhickiy,
  • Anastasia A. Maksimovskaya,
  • Sergey V. Bakurskiy,
  • Andrey E. Schegolev,
  • Maxim V. Tereshonok,
  • Mikhail Yu. Kupriyanov,
  • Nikolay V. Klenov and
  • Igor I. Soloviev

Beilstein J. Nanotechnol. 2025, 16, 1883–1893, doi:10.3762/bjnano.16.131

Graphical Abstract
  • exploit this sparsity when solving the system. The equations are integrated numerically using an adaptive-step-size solver based on the explicit Runge–Kutta (4th and 5th order) formula, commonly known as the Dormand–Prince pair [44][45], which is well suited for this class of non-stiff problems. The
  • the kinetic soliton’s propagation rate. As a preliminary step, we characterized the dependence of the kinetic soliton propagation velocity on the damping parameter of the connecting junctions, α (see Figure 1b). We define the velocity as the number of grounded junctions traversed per unit of
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Published 28 Oct 2025

Low-temperature AFM with a microwave cavity optomechanical transducer

  • Ermes Scarano,
  • Elisabet K. Arvidsson,
  • August K. Roos,
  • Erik Holmgren,
  • Riccardo Borgani,
  • Mats O. Tholén and
  • David B. Haviland

Beilstein J. Nanotechnol. 2025, 16, 1873–1882, doi:10.3762/bjnano.16.130

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  • driving the coarse z-positioner with the Attocube ANC-300 control unit that provides the 60 V saw-tooth pulses to the piezo actuators. The stick–slip motion of the actuator under high-voltage saw-tooth pulses (≈50 nm/step) produces significant heating at the 10 mK stage. Under continuous operation, the
  • tracking with abrupt changes in topography. The latter occurred during the scan; in multiple instances, the feedback temporarily loses track of the surface immediately after the tip encounters a step. The single scan line on the fast axis (i.e., x-axis) shown in Figure 4b,c clearly shows different behavior
  • resonance frequency shift as a function of the tip–surface distance. (a) AM-AFM imaging of the calibration grating over a 1 µm × 1 µm scan area containing a single vertical stripe with a 10 nm step height. The dashed lines in the image mark the location of the scan lines in (b) and (c). (a) FM-AFM imaging
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Published 24 Oct 2025

Self-assembly and adhesive properties of Pollicipes pollicipes barnacle cement protein cp19k: influence of pH and ionic strength

  • Shrutika Sawant,
  • Anne Marie Power and
  • J. Gerard Wall

Beilstein J. Nanotechnol. 2025, 16, 1863–1872, doi:10.3762/bjnano.16.129

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  • . coli BL21 (DE3) cells as previously described [21] and purified by two step purification, that is, immobilised metal affinity chromatography (IMAC) followed by ion exchange chromatography (IEC). For IMAC, the Co-IDA resin column was washed with 25 mM Tris-HCl buffer (pH 8.0) containing 150 mM NaCl and
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Published 23 Oct 2025
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