Thermal transport in kinked nanowires through simulation

• Alexander N. Robillard,
• Graham W. Gibson and
• Ralf Meyer

Beilstein J. Nanotechnol. 2023, 14, 586–602, doi:10.3762/bjnano.14.49

• phonon reflection specularity on the heat flux is also examined. It is found that, in general, the flow of heat through systems simulated through phonon Monte Carlo methods is concentrated into a channel smaller than the wire dimensions, while this is not the case in the classical solutions of the

• increase with increasing kink angle. With the scattering rate becoming large, and consequently the mean free path of phonons becoming short, the effect of scattering off surfaces becomes negligible, and the heat flow becomes more diffusive (it is also reduced in magnitude due to overall reduced transport

• small “shortcuts” that the heat flow can use to reduce its effective path length, much like a race-car driver taking the inside corners of a series of curves. This corner cutting has been seen and discussed previously in the context of right-angled serpentine nanowires [20][22][30]. To reiterate a point

Carbon nanotube-cellulose ink for rapid solvent identification

• Tiago Amarante,
• Thiago H. R. Cunha,
• Claudio Laudares,
• Ana P. M. Barboza,
• Ana Carolina dos Santos,
• Cíntia L. Pereira,
• Vinicius Ornelas,
• Bernardo R. A. Neves,
• André S. Ferlauto and
• Rodrigo G. Lacerda

Beilstein J. Nanotechnol. 2023, 14, 535–543, doi:10.3762/bjnano.14.44

• two important properties of the liquids, namely dielectric constant and vapor pressure, on the transduction of the MFC-MWCNT sensors. These results were corroborated by independent heat flow measurements (thermogravimetric analysis). The proposed MFC-MWCNT sensor platform may help paving the way to

• contact mode. AC160TS silicon cantilevers from Olympus with a typical spring constant of k ≈ 46 N/m, a nominal radius of curvature of r ≈ 7 nm, and a resonant frequency of ω0 ≈ 300 kHz were employed. Heat flow and weight changes of selected solvents were determined by thermogravimetric analysis (TGA

• produced by the impinging liquid drops over the heated surface of the transducer. The temperature change and the heat flow produced by the liquid as it gets in contact with the heated surface were estimated by dripping a liquid (of about 6.5 µL) into an empty crucible kept at 55 °C inside a

Nanoarchitectonics to entrap living cells in silica-based systems: encapsulations with yolk–shell and sepiolite nanomaterials

• Celia Martín-Morales,
• Jorge Fernández-Méndez,
• Pilar Aranda and
• Eduardo Ruiz-Hitzky

Beilstein J. Nanotechnol. 2023, 14, 522–534, doi:10.3762/bjnano.14.43

• , fresh yeast). All employed materials and equipment have been sterilized by heating to 120 °C for 25 min and subsequent cool down to room temperature within the autoclave chamber. All culture handling operations have been performed within a sterile laminar flow hood, which before and after its usage had

A mid-infrared focusing grating coupler with a single circular arc element based on germanium on silicon

• Xiaojun Zhu,
• Shuai Li,
• Ang Sun,
• Yongquan Pan,
• Wen Liu,
• Yue Wu,
• Guoan Zhang and
• Yuechun Shi

Beilstein J. Nanotechnol. 2023, 14, 478–484, doi:10.3762/bjnano.14.38

• membrane Ge waveguide [1]. The maximum coupling efficiency was −11 dB at the focusing SWG’s center wavelength of 2.37 μm. The high coupling efficiency was obtained experimentally. However, the fabrication flow of the suspended membrane Ge waveguide with focusing SWGs greatly increased the complexity of the

The steep road to nonviral nanomedicines: Frequent challenges and culprits in designing nanoparticles for gene therapy

• Yao Yao,
• Yeongun Ko,
• Grant Grasman,
• Jeffery E. Raymond and
• Joerg Lahann

Beilstein J. Nanotechnol. 2023, 14, 351–361, doi:10.3762/bjnano.14.30

• are assessed with the use of fluorescent-labeling carriers and the expression of fluorescent proteins (e.g., enhanced green fluorescent protein). Both of which are typically assessed by widefield fluorescent microscopy/confocal microscopy (referred to as “imaging”) and/or flow cytometry (Table 1

• after image capture (26%, Figure 1a2). Flow cytometry, also a fluorescence-based method, is an alternate assessment of uptake and transfection. It is commonly used for high-throughput cell studies and is known for both rapid data acquisition and large data sets [17]. Flow cytometry can generate large

• papers, Figure 1b). Despite the robust data it can provide, flow cytometry counts the total number of cells associated with NPs and cannot distinguish internalized cargo from surface-bound NPs [1][17]. To precisely quantify internalization, a secondary method is required that can differentiate between

Overview of mechanism and consequences of endothelial leakiness caused by metal and polymeric nanoparticles

• Magdalena Lasak and
• Karol Ciepluch

Beilstein J. Nanotechnol. 2023, 14, 329–338, doi:10.3762/bjnano.14.28

• vasoconstrictions factors (e.g., thromboxane, prostaglandin, and endothelin-1), regulating vessel tension and, thus, blood flow and pressure [4][5][6][7][8]. The endothelium also produces mediators involved in angiogenic processes (e.g., vascular endothelial growth factor (VEGF) and fibroblast growth factor (FGF

• nutrient molecules to NPs could change the toxicity of NPs (NP protein corona), and the physiological conditions, such as blood flow and physiological stretch, will also play a role [37][38][39]. NanoEL mechanism Adherens junctions between endothelial cells are maintained by a complex set of proteins

• EPR effect, but transport strictly depends on the stage of the tumor. Hence, the use of the EPR effect may be justified only in the case of mature tumors. Moreover, leaky vessels and heterogeneous blood flow limit its use for therapeutic purposes. By contrast, NanoEL is a mechanism completely

Biocatalytic synthesis and ordered self-assembly of silica nanoparticles via a silica-binding peptide

• Mustafa Gungormus

Beilstein J. Nanotechnol. 2023, 14, 280–290, doi:10.3762/bjnano.14.25

• molecular crowding-like effects, preventing efficient assembly of the particles. Therefore, tailoring intermolecular interactions between nanoparticles by modifying the particle surfaces or through external influences such as temperature, pH value, templates, and magnetic or flow fields, is important to

• –MS analyses were done with a fused silica capillary column a (Restek 14623, Thermo Fischer Scientific Inc, Waltham, MA, USA), 150 °C injection temperature, 250 °C detection temperature, 1 µL injection volume, and 1 mL/min He flow rate. Dionex Chromeleon 7.2 software (Thermo Fischer Scientific Inc

Spin dynamics in superconductor/ferromagnetic insulator hybrid structures with precessing magnetization

• Yaroslav V. Turkin and
• Nataliya Pugach

Beilstein J. Nanotechnol. 2023, 14, 233–239, doi:10.3762/bjnano.14.22

• proximity effect”. Distributions of spin current and induced magnetization were calculated in recent works [20][21], where the authors investigate spin current flow through Josephson-like trilayer structures. The proximity effect is the penetration of superconducting correlations in an adjacent

• proximity effect. The spin current can be induced only by the nonstationary flow of triplet Cooper pairs, just as in a conventional spin-pumping bilayer structure with a normal metal [33]. Thus, spin currents cannot emerge when the magnetization is stationary inside the ferromagnetic insulator layer

A novel approach to pulsed laser deposition of platinum catalyst on carbon particles for use in polymer electrolyte membrane fuel cells

• Bogusław Budner,
• Wojciech Tokarz,
• Sławomir Dyjak,
• Andrzej Czerwiński,
• Bartosz Bartosewicz and
• Bartłomiej Jankiewicz

Beilstein J. Nanotechnol. 2023, 14, 190–204, doi:10.3762/bjnano.14.19

• the catalytic and diffusion layers. The microscopic water droplets must leave the MEA and the cell, but in some cases, they are temporarily trapped in the diffusion layer or the flow fields. The presence of water results in a temporary decrease of the current due to the transport resistance increase

• of 20% Pt Vulcan XC-72R catalyst, while the anode was made of 20% Pt HiSpec 3000 catalyst. MEA tests were carried out on a single-cell fuel cell assembly with a single serpentine flow field on both electrodes. The assembled cells were fed with ambient air supplied by an oil-free compressor and H2 5.0

A distributed active patch antenna model of a Josephson oscillator

• Vladimir M. Krasnov

Beilstein J. Nanotechnol. 2023, 14, 151–164, doi:10.3762/bjnano.14.16

• ; Introduction A flux-flow oscillator (FFO) is the most extensively studied Josephson source of high-frequency electromagnetic waves (EMW) [1][2][3][4][5][6][7][8][9][10][11][12]. A FFO was used in the first direct demonstration of Josephson emission by Yanson et al., back in 1965 [13][14]. State of the art FFOs

• and the flux-flow phenomenon. Therefore, a JJ can be considered as an actively pumped patch antenna with a distributed feed-in current. In this work, I present a distributed, active patch antenna model of a Josephson oscillator. It expands the TL model of a patch antenna [36], taking into account the

• and the flux-flow phenomenon. (iii) The slow propagation speed of EMWs inside the JJ, c0 ≪ c. This is caused by a large kinetic inductance of superconducting electrodes. For Nb-based JJs, c/c0 ≈ 40 (see the estimation in section Discussion). For atomic-scale intrinsic JJs in layered cuprates, c0 can

Batch preparation of nanofibers containing nanoparticles by an electrospinning device with multiple air inlets

• Dong Wei,
• Chengwei Ye,
• Adnan Ahmed and
• Lan Xu

Beilstein J. Nanotechnol. 2023, 14, 141–150, doi:10.3762/bjnano.14.15

• that under the appropriate voltage (50 kV) and air flow (50 m3/h), the device could keep ZnO nanoparticles contained in the spinning solution evenly dispersed during the spinning process, thus obtaining functional nanofibers with more uniform distribution of ZnO nanoparticles, whose quality and yield

• enabled the ZnO nanoparticles contained in the spinning solution to maintain uniform dispersion in the batch preparation process of nanofibers by means of air flow produced through multiple pores. The airflow reduces the agglomeration of nanoparticles, thus yielding nanofibers with uniform ZnO loading. In

• experiments were performed at 25 °C and 60% relative humidity. The following MEAI parameters were used. The receiving distance was 18 cm, the speed of the receiving drum was 300 r/min, the air flow rates were 0, 50, 100, and 150 m3/h, and the spinning voltages were 40, 50, and 60 kV. Measurement and

Formation of nanoflowers: Au and Ni silicide cores surrounded by SiO_x branches

• Feitao Li,
• Siyao Wan,
• Dong Wang and
• Peter Schaaf

Beilstein J. Nanotechnol. 2023, 14, 133–140, doi:10.3762/bjnano.14.14

• out in a rapid thermal processing (RTP, Jipelec Jetstar 100) furnace. First, the chamber was evacuated and purged with Ar three times at room temperature, then a flow of forming gas of Ar + H2 (volume ratio 30:1) was kept till the end of the experiment. The temperature was ramped up to 300 °C in 20 s

Characterisation of a micrometer-scale active plasmonic element by means of complementary computational and experimental methods

• Ciarán Barron,
• Giulia Di Fazio,
• Samuel Kenny,
• Silas O’Toole,
• Robin O’Reilly and
• Dominic Zerulla

Beilstein J. Nanotechnol. 2023, 14, 110–122, doi:10.3762/bjnano.14.12

• scanning. While leaving the probe floating is counterproductive from the perspective of minimising electrostatic interaction, the possibility of current flow through the tip to ground is eliminated. As with the LIA phase selection for the SPR measurements discussed above, the phase was selected so as to

• effect. The presence of a constriction in the metal (the bridge) results in a localised heating effect. A schematic of the enhanced SPR experiment. Schematic describing the experimental setup used to perform SJEM measurements on a modulated element. Flow diagram of simulation process. FEM optical

Frontiers of nanoelectronics: intrinsic Josephson effect and prospects of superconducting spintronics

• Anatolie S. Sidorenko,
• Horst Hahn and
• Vladimir Krasnov

Beilstein J. Nanotechnol. 2023, 14, 79–82, doi:10.3762/bjnano.14.9

• : artificial neural networks; functional nanostructures; intrinsic Josephson effect; nanoelectronics; spintronics; The twenty-first century is marked by an explosive growth in the flow of information, which is necessary to process, archive, and transmit data through communication systems. For that purpose

Gap-directed chemical lift-off lithographic nanoarchitectonics for arbitrary sub-micrometer patterning

• Chang-Ming Wang,
• Hong-Sheng Chan,
• Chia-Li Liao,
• Che-Wei Chang and
• Wei-Ssu Liao

Beilstein J. Nanotechnol. 2023, 14, 34–44, doi:10.3762/bjnano.14.4

• , sequentially rinsed with acetone and isopropanol, and blown dry with nitrogen gas. To conduct CLL processes, a PDMS stamp was activated by 30 s of oxygen plasma exposure at a power of 18 W with 0.5 mbar oxygen flow. The stamp was then conformally sealed onto the SAM-modified Au substrate for 2 h under ambient

Atmospheric water harvesting using functionalized carbon nanocones

• Fernanda R. Leivas and
• Marcia C. Barbosa

Beilstein J. Nanotechnol. 2023, 14, 1–10, doi:10.3762/bjnano.14.1

• occurs due to the presence of hydrophilic sites at the nanocone entrance. The functionalization, together with the high mobility of water inside nanostructures, leads to a fast water flow through the nanostructure. We show using molecular dynamics simulations that this device is able to collect water if

• addition to the hydrophobicity described above. The phenomena of density increasing with temperature at constant pressure and diffusion coefficients increasing with density at constant temperature were observed in experiments and simulations in bulk water [22][23][24]. Water presents both super flow and

• slowing down when confined in biological structures with the presence of hydrophobic and hydrophilic sites [25]. Water confined in hydrophobic structures, such as carbon nanotubes with diameters below 2 nm, exhibits a fast flow that exceeds values provided by classical hydrodynamics [26]. This super flow

Utilizing the surface potential of a solid electrolyte region as the potential reference in Kelvin probe force microscopy

• Nobuyuki Ishida

Beilstein J. Nanotechnol. 2022, 13, 1558–1563, doi:10.3762/bjnano.13.129

• negative direction, a cathodic current due to the reduction of Ti ions started to flow at around 2.8 V (vs Li/Li+). KPFM measurements were performed in the region across the solid electrolyte (Figure 1a). Figure 3a and Figure 3b display the topography and CPD images, respectively, obtained when 0 V was

• toward the negatively biased electrode, resulting in an ionic current flow. The ion current decays with time and, in principle, becomes zero when the electric field in the solid electrolyte is shielded by the accumulation and depletion of Li ions. Before starting each KPFM measurement, we waited 2–4 min

• measurement The KPFM measurements were performed at room temperature using a commercial atomic force microscope (Park Systems, NX10) placed in an Ar flow glove box (O2: <1 ppm, H2O: <1 ppm). We used Cr/Pt-coated Si cantilevers (Budget Sensors, Multi75E-G) with a nominal resonance frequency of 75 kHz and a

Induced electric conductivity in organic polymers

• Konstantin Y. Arutyunov,
• Anatoli S. Gurski,
• Vladimir V. Artemov,
• Alexander L. Vasiliev,
• Azat R. Yusupov,
• Danfis D. Karamov and
• Alexei N. Lachinov

Beilstein J. Nanotechnol. 2022, 13, 1551–1557, doi:10.3762/bjnano.13.128

• : the flow of supercurrent between two superconductors separated by a dielectric barrier. However, the correlation of the order parameters of two spatially separated superconductors is a subtle quantum mechanical effect, which in all practical cases is observed at dielectric thicknesses of the order of

Non-stoichiometric magnetite as catalyst for the photocatalytic degradation of phenol and 2,6-dibromo-4-methylphenol – a new approach in water treatment

• Joanna Kisała,
• Anna Tomaszewska and
• Przemysław Kolek

Beilstein J. Nanotechnol. 2022, 13, 1531–1540, doi:10.3762/bjnano.13.126

• C18 H, with precolumn). The analysis conditions were as follows: mobile phase: 70% acetonitrile and 30% water; flow rate: 1.0 cm3·min−1; injection volume: 20 × 10−3 cm3; absorbance detection: 270 and 310 nm for PhOH and DBMP, respectively. External standards of seven concentration levels ranging from

Facile preparation of Au- and BODIPY-grafted lipid nanoparticles for synergized photothermal therapy

• Yuran Wang,
• Xudong Li,
• Haijun Chen and
• Yu Gao

Beilstein J. Nanotechnol. 2022, 13, 1432–1444, doi:10.3762/bjnano.13.118

• 30 μM) at 37 °C for 0.5, 1, 2, 4, 6, and 8 h. Then, the cells were washed, digested, and suspended in 500 μL PBS. The fluorescence was detected by flow cytometry (Becton Dickinson FACSAriaIII cell sorter) in PerCP-Cy5.5 channel to detect the fluorescence of BDP according to our previous report [22

• complex nanoparticles with suitable particle size (73 nm) for in vivo application. Besides, at this molar ratio, BDP could be successfully grafted onto the LNPs. Flow cytometry was employed to study the cellular uptake efficiencies of AB-LNPs and free BDP by detecting the fluorescence of BDP in the PerCP

• nanoparticles, which was consistent with the results obtained from flow cytometry. For comparison, no fluorescence could be found in cells treated with Au-LNPs. AB-LNPs showed the highest cellular uptake efficiency after 6 h of incubation. Hence, we chose 6 h incubation time to study the anti-proliferative

Dry under water: air retaining properties of large-scale elastomer foils covered with mushroom-shaped surface microstructures

• Matthias Mail,
• Stefan Walheim,
• Thomas Schimmel,
• Wilhelm Barthlott,
• Stanislav N. Gorb and
• Lars Heepe

Beilstein J. Nanotechnol. 2022, 13, 1370–1379, doi:10.3762/bjnano.13.113

• liquids flow over solid surfaces [29][30]. The highest economic and ecological potential for this technology is the shipping industry [31]. The optimal parameters for stable air retention have been previously investigated [1][32] and theoretical calculations have been performed [33][34][35]. Four criteria

Straight roads into nowhere – obvious and not-so-obvious biological models for ferrophobic surfaces

• Wilfried Konrad,
• Christoph Neinhuis and
• Anita Roth-Nebelsick

Beilstein J. Nanotechnol. 2022, 13, 1345–1360, doi:10.3762/bjnano.13.111

• , Rosenstein 1, D-70191 Stuttgart, Germany 10.3762/bjnano.13.111 Abstract There are currently efforts to improve strategies for biomimetic approaches, to identify pitfalls and to provide recommendations for a successful biomimetic work flow. In this contribution, a case study of a concrete biomimetic project

• both biological models for the tuyère problem. Instead, a seemingly not obvious biological model was identified, namely micropores within the cell walls of water-transporting conduits of plants that connect the conduits to a three-dimensional flow network. These specially shaped pores are assumed to be

• represented by a sequence of projects in which the co-authors of this paper were involved in different combinations. The underlying biomimetic problems and physical as well as biological topics just provided the vehicle to describe the flow of concepts, inspirations and transfer problems. Perspective The

Recent trends in Bi-based nanomaterials: challenges, fabrication, enhancement techniques, and environmental applications

• Vishal Dutta,
• Ankush Chauhan,
• Ritesh Verma,
• C. Gopalkrishnan and
• Van-Huy Nguyen

Beilstein J. Nanotechnol. 2022, 13, 1316–1336, doi:10.3762/bjnano.13.109

• -type Bi2S3 is somewhat close to the CB. In a heterojunction from n-type Bi2O3 and p-type Bi2S3, electrons flow from n-type Bi2O3 to p-type Bi2S3, and holes flow from p-type Bi2S3 with a low Fermi level to n-type Bi2O3 with a high Fermi level. As a consequence of this, negative charges build up in Bi2S3

• often employed to offer an intermediary conduit for electrons to flow from the CB of semiconductor II (SC II) to the VB of semiconductor I (SC I), making the charge transfer easier [38]. A solid substance or a redox couple in solution may serve as a mediator in the Z-scheme. This dual absorber system

• performance of heterojunction photocatalysts, researchers have recently proposed an S-scheme heterojunction [45]. Separating photoinduced electrons and holes with an S-scheme heterojunction efficiently preserves the promising redox properties of semiconductors. It is common for electrons to flow from the CB

Bending and punching characteristics of aluminum sheets using the quasi-continuum method

• Man-Ping Chang,
• Shang-Jui Lin and
• Te-Hua Fang

Beilstein J. Nanotechnol. 2022, 13, 1303–1315, doi:10.3762/bjnano.13.108

• the cutting surfaces. According to previous research, this phenomenon is due to a too small taper that hinders the material flow during punching [64]. In contrast, the 10° taper angle punch shows smooth cutting surfaces; therefore, this taper angle is more suitable for this punching process

Laser-processed antiadhesive bionic combs for handling nanofibers inspired by nanostructures on the legs of cribellate spiders

• Sebastian Lifka,
• Kristóf Harsányi,
• Erich Baumgartner,
• Lukas Pichler,
• Dariya Baiko,
• Karsten Wasmuth,
• Johannes Heitz,
• Marco Meyer,
• Anna-Christin Joel,
• Jörn Bonse and
• Werner Baumgartner

Beilstein J. Nanotechnol. 2022, 13, 1268–1283, doi:10.3762/bjnano.13.105

• Standard Gr. 1 G20 x 1 ½’’, B. Braun SE, Melsungen, Germany) using a custom-made syringe pump at a flow rate between 0.2 to 0.3 mL/h (Figure 11a) equipped with a 1 mL plastic syringe (Omnifix-F, B. Braun SE, Melsungen, Germany). The sample fixed on an aluminium sample carrier was placed horizontally