Application of nanoarchitectonics in moist-electric generation

• Jia-Cheng Feng and
• Hong Xia

Beilstein J. Nanotechnol. 2022, 13, 1185–1200, doi:10.3762/bjnano.13.99

• nanoparticles, nanowires, and nanosheets. In the construction of devices, nanomaterial units are stacked in thin layers or blocks, and gaps are formed between the units, allowing for the formation of nanoscale networks in the stacked regions. When the nanoparticles, nanowires, or nanosheets are stacked in a non

• maximum Voc of 0.6 V and an Isc of 0.3 μA (Figure 4b,c). TiO2 nanowires provided an open-circuit voltage of 0.5 V and microampere-level short-circuit currents through a rich 3D nanoscale network. In a Ti3C2Tx MXene nanosheet generator, the wicking rates of the samples after sonication were increased, and

• is the highest instantaneous current measured in nanomaterial MEG devices. Moreover, the preparation method of metal compound nanomaterials is mature, and different morphologies can be obtained, such as nanoparticles of Al2O3, nanowires of TiO2, Ni–Al layered structures, and nanosheets of MXene

Electrocatalytic oxygen reduction activity of AgCoCu oxides on reduced graphene oxide in alkaline media

• Iyyappan Madakannu,
• Indrajit Patil,
• Bhalchandra Kakade and
• Kasibhatta Kumara Ramanatha Datta

Beilstein J. Nanotechnol. 2022, 13, 1020–1029, doi:10.3762/bjnano.13.89

• et al. prepared supportless Ag nanowires and 1D mesoporous hollow AgPdPt nanotubes by micelle-assisted galvanic replacement followed by acid etching. They found that hollow AgPdPt structures exhibited a better ORR activity with onset and half-wave potential of 0.99 V and 0.90 V vs RHE, respectively

Effects of focused electron beam irradiation parameters on direct nanostructure formation on Ag surfaces

• Jānis Sniķeris,
• Vjačeslavs Gerbreders,
• Andrejs Bulanovs and
• Ēriks Sļedevskis

Beilstein J. Nanotechnol. 2022, 13, 1004–1010, doi:10.3762/bjnano.13.87

• . However, some studies suggest that this process may not always be so simple. Ueda and Yoshimura [27] reported the fabrication of free-standing nanowires on various metal surfaces (Al, Ag, Au, Cu, Pt, Ta, Ti, and W) via EBID with pump oil (hydrocarbons) as a precursor. It was observed that the substrate

• material greatly affects the growth rate of the nanowires, with the Cu surface providing the fastest growth. Energy-dispersive X-ray spectroscopy (EDX) revealed the presence of both carbon and substrate materials in the nanowires. The effect of substrate material on nanowire growth rate could be attributed

• to different adhesion coefficients between the surface and hydrocarbons. Results from EDX measurements strongly suggest that metal atoms or ions are capable of moving within carbon–metal nanowires under the influence of EB. High Ag ion mobility under electric fields or EB has also been reported in

Efficient liquid exfoliation of KP₁₅ nanowires aided by Hansen's empirical theory

• Zhaoxuan Huang,
• Zhikang Jiang,
• Nan Tian,
• Disheng Yao,
• Fei Long,
• Yanhan Yang and
• Danmin Liu

Beilstein J. Nanotechnol. 2022, 13, 788–795, doi:10.3762/bjnano.13.69

• Abstract The KP15 nanowires with one-dimensional properties has a defect-free surface, high anisotropy, and carrier mobility which is desirable for the development of novel nanodevices. However, the preparation of nanoscale KP15 is still inefficient. In this work, the Hansen solubility parameters of KP15

• were first obtained. Based on the Hansen's empirical theory, the concentration of liquid-exfoliated KP15 nanowires was improved to 0.0458 mg·mL−1 by a solution containing 50% water and 50% acetone. Approximately 79% of the KP15 nanowires had a thickness value below 50 nm and 60.9% of them had a width

• value below 100 nm. The thinnest KP15 nanowires reached 5.1 nm and had smooth boundaries. Meanwhile, strong temperature-dependent Raman response in exfoliated KP15 nanowires has been observed, which indicates a strong phonon–phonon coupling in those nanowires. This is helpful for non-invasive

Comparative molecular dynamics simulations of thermal conductivities of aqueous and hydrocarbon nanofluids

• Adil Loya,
• Antash Najib,
• Fahad Aziz,
• Asif Khan,
• Guogang Ren and
• Kun Luo

Beilstein J. Nanotechnol. 2022, 13, 620–628, doi:10.3762/bjnano.13.54

• nanoparticles change thermal conductivity, as investigated by Zhu et al. [24]. In their research, CuO nanowires and nanospheres were dispersed in a dimethicone base fluid, and it was found that changes in the crystalline structure of nanoparticles change the kinetics of the base fluid [24]. In addition to this

• , it was further investigated that the thermal conductivity increases more with CuO nanowires than with CuO nanospheres. Only 6.98% of improvement was recorded with nanospheres, while 60.78% was recorded with nanowires. Ibrahim et al. [25] conducted a study using a neural network model (ANN) to study

Zinc oxide nanostructures for fluorescence and Raman signal enhancement: a review

• Ioana Marica,
• Fran Nekvapil,
• Maria Ștefan,
• Cosmin Farcău and
• Alexandra Falamaș

Beilstein J. Nanotechnol. 2022, 13, 472–490, doi:10.3762/bjnano.13.40

• controllable morphology [28]. Various morphologies including nanoworms, nanowires, and nanorods with excellent crystallinity were also obtained using the solvothermal method [25]. According to Chieng et al., the particle sizes of the synthesized ZnO nanoparticles are in correlation with the glycol chain length

• substrate covered with polystyrene spheres by atomic layer deposition, followed by electrodeposition, which was used to grow ZnO nanowires onto the surface. The Au layer was deposited after burning off the polystyrene spheres by electron beam evaporation while monitoring its thickness. Considering the

• alone, an effect which the authors assigned to the amplification of the chemical effect of the ZnO layer by the LSPR of the Au cores. In another study, Ag nanowires were prepared by a polyol process and core–shell Ag–ZnO heteronanowires were synthesized by a simple solution process adding Zn(NO3)2 and

A chemiresistive sensor array based on polyaniline nanocomposites and machine learning classification

• Jiri Kroutil,
• Alexandr Laposa,
• Ali Ahmad,
• Jan Voves,
• Vojtech Povolny,
• Ladislav Klimsa,
• Marina Davydova and
• Miroslav Husak

Beilstein J. Nanotechnol. 2022, 13, 411–423, doi:10.3762/bjnano.13.34

• FERA3 GM), as shown in Figure 1a–h. All nanocomposite active layers, that is, PANI/ZnO, PANI/WO3 (nanopowder), PANI/WO3 (nanowires), PANI/In2O3, PANI/C60, PANI/NCD, and PANI/BaTiO3 have similar morphological features with a uniform distribution of additives in polyaniline. We can observe small ZnO

• flakes and WO3 nanowires homogeneously distributed in the layers. Pristine PANI was examined by SEM (Figure 1h) and Raman spectroscopy (Raman spectrometer Renishaw inVia Qontor) at room temperature with 633 nm excitation wavelength (Figure 2). The spectrum of pristine PANI is typical of the emeraldine

• Sn0.63Pb0.37. The sensor size array is 16.2 mm (width) × 16.2 mm (length) with the sensing layer size of 1.7 mm × 1.7 mm. A pin header connector is used for connection of the sensor array. Sensor arrays with PANI/nanocomposite (PANI/ZnO, PANI/WO3 (nanopowder), PANI/WO3 (nanowires), PANI/In2O3, PANI/C60, PANI

Electrostatic pull-in application in flexible devices: A review

• Teng Cai,
• Yuming Fang,
• Yingli Fang,
• Ruozhou Li,
• Ying Yu and
• Mingyang Huang

Beilstein J. Nanotechnol. 2022, 13, 390–403, doi:10.3762/bjnano.13.32

• structure of the flexible devices. Nanoelectromechanical (NEM) switches made of carbon nanotubes (CNTs) [2][3][4], graphene (GR) [5][6][7], nanowires (NWs) [8][9][10], and other flexible materials are the most basic devices for a variety of component and system level applications, such as low-loss switches

• electrode materials include CNTs, GR, and silicon/germanium nanowires. CNT-NEM switches CNTs are an ideal flexible material for NEM electrodes because of the high aspect ratio, current density, and excellent tensile strength. In 2000, Rueckes et al. [13] observed the electromechanical conversion in CNTs for

• can greatly simplify the circuit volume of traditional PN junctions and increase the circuit integration. NWs-NEM switches Single-crystal nanowires are excellent candidates for NEM switches due to their uniform chemical and physical structure, and good reproducibility of structure and composition

Plasma modes in capacitively coupled superconducting nanowires

• Alex Latyshev,
• Andrew G. Semenov and
• Andrei D. Zaikin

Beilstein J. Nanotechnol. 2022, 13, 292–297, doi:10.3762/bjnano.13.24

• Moscow, Russia Institute for Quantum Materials and Technologies, Karlsruhe Institute of Technology (KIT), 76021 Karlsruhe, Germany 10.3762/bjnano.13.24 Abstract We investigate plasma oscillations in long electromagnetically coupled superconducting nanowires. We demonstrate that in the presence of inter

• the low-temperature behavior of the systems under consideration. Keywords: plasma modes; quantum fluctuations, quantum phase slips; superconducting nanowires; Introduction Physical properties of ultrathin superconducting nanowires differ strongly from those of bulk superconductors owing to a

• |Δ| in superconducting nanowires one finds [5]: where Rξ is the normal-state resistance of the wire segment of length equal to the superconducting coherence length ξ and Rq = 2π/e2 ≃ 25.8 kΩ is the quantum resistance unit. For generic metallic nanowires one typically has Rξ ≪ Rq, implying that

Investigation of a memory effect in a Au/(Ti–Cu)Ox-gradient thin film/TiAlV structure

• Damian Wojcieszak,
• Jarosław Domaradzki,
• Michał Mazur,
• Tomasz Kotwica and
• Danuta Kaczmarek

Beilstein J. Nanotechnol. 2022, 13, 265–273, doi:10.3762/bjnano.13.21

• [2][21][39]. Some examples of resistive switching behavior were also found in structures based on nanowires [40] or nanotubes [25][40], where the resistive switching device is characterized by the presence of a pinched or nonpinched hysteresis loop in the I–V characteristics in the DC plane. Our

Engineered titania nanomaterials in advanced clinical applications

• Padmavati Sahare,
• Paulina Govea Alvarez,
• Juan Manual Sanchez Yanez,
• Gabriel Luna-Bárcenas,
• Samik Chakraborty,
• Sujay Paul and
• Miriam Estevez

Beilstein J. Nanotechnol. 2022, 13, 201–218, doi:10.3762/bjnano.13.15

• nanostructures such as nanotubes and nanowires have been utilized in photoelectrochemical sensing for the rapid and precise identification of biological analytes at low concentrations, useful for clinical diagnosis. These nanostructures have been employed for sensing humidity, oxygen, and hydrogen, inclusive of

• , were also used to improve the titania implant properties, and the material showed significant antibacterial activity against Staphylococcus aureus with sustained release of vancomycin [64]. Furthermore, the biological activity of TiO2 nanowires, nanofibres, and nanoneedles, was investigated and

• compared to that of Ti6Al4V, which is typically utilized in implants. Results revealed that more fibroblast cells proliferated on all specimens of nanofibers as well as on the nanowires arrays when the incubation period was increased; however, this behavior was not observed in the case of nanoneedles [65

Topographic signatures and manipulations of Fe atoms, CO molecules and NaCl islands on superconducting Pb(111)

• Carl Drechsel,
• Philipp D’Astolfo,
• Jung-Ching Liu,
• Thilo Glatzel,
• Rémy Pawlak and
• Ernst Meyer

Beilstein J. Nanotechnol. 2022, 13, 1–9, doi:10.3762/bjnano.13.1

• between two materials, exhibiting particle–hole symmetry and spin–orbit interaction [8]. Among the most promising platforms to realize MZMs are semiconducting nanowires with large spin–orbit coupling [9][10][11][12] or atomic chains [13][14][15][16][17][18] in proximity to an s-wave superconductor. The

Chemical vapor deposition of germanium-rich CrGe_x nanowires

• Vladislav Dřínek,
• Stanislav Tiagulskyi,
• Roman Yatskiv,
• Jan Grym,
• Radek Fajgar,
• Věra Jandová,
• Martin Koštejn and
• Jaroslav Kupčík

Beilstein J. Nanotechnol. 2021, 12, 1365–1371, doi:10.3762/bjnano.12.100

• Sciences, Chaberská 1014/57, 182 51 Prague 8, Czech Republic 10.3762/bjnano.12.100 Abstract Chemical vapor deposition was applied to synthetize nanostructured deposits containing several sorts of nanoobjects (i.e., nanoballs, irregular particles, and nanowires). Analytical techniques, that is, high

• . The nanowires possessed a complex structure, namely a thin crystalline germanium core and amorphous CrGex coating. The composition of the nanowire coating was [Cr]/[Ge] = 1:(6–7). The resistance of the nanowire–deposit system was estimated to be 2.7 kΩ·cm using an unique vacuum contacting system

• reasonable choice for DMS alloys with chromium for the best compatibility with silicon-based industry. However, precipitation of transition metals is the main obstacle; but in low-dimensional semiconductors the precipitation is significantly reduced. Therefore, CrGe nanowires (NWs) were prepared to study

Morphology-driven gas sensing by fabricated fractals: A review

• Vishal Kamathe and
• Rupali Nagar

Beilstein J. Nanotechnol. 2021, 12, 1187–1208, doi:10.3762/bjnano.12.88

• metal oxide (SMO) sensors are most popular due to their low cost, simplicity, easy fabrication, and wide range of gas detection capabilities [9]. Thin films and nanostructures exhibit better sensing characteristics. Various researchers have reported structures with morphologies such as nanowires (NWs

• sample, exhibiting a combination of hillocks and pores, showed the maximum sensitivity (S = 0.29) towards NO2. Another study reported dendritic nanowires (DNWs) of SnO2 on a gold-coated silicon substrate for NO2 sensing [66]. The samples were prepared by evaporation–condensation. Figure 6a and Figure 6b

• not subject to CC BY 4.0. SnO2 dendritic nanowires. SEM images of SnO2 DNWs at low (a) and high (b) magnifications, respectively. (c) The sensitivity versus temperature curve for 10–50 ppm NO2. Figure 6a–c was reprinted from [66], Journal of Alloys and Compounds, vol. 510, by S.H. Mohamed, “SnO2

Self-assembly of amino acids toward functional biomaterials

• Huan Ren,
• Lifang Wu,
• Lina Tan,
• Yanni Bao,
• Yuchen Ma,
• Yong Jin and
• Qianli Zou

Beilstein J. Nanotechnol. 2021, 12, 1140–1150, doi:10.3762/bjnano.12.85

• various nanostructures, such as nanowires [17], nanofibers [18], nanospheres [19], nanovesicles [20], nanogels [21], nanobelts [22], and nanotubes [23]. Self-assembly not only conveys higher stability and mechanical strength to proteins and peptides, but also further enhances their natural activity and

Assessment of the optical and electrical properties of light-emitting diodes containing carbon-based nanostructures and plasmonic nanoparticles: a review

• Keshav Nagpal,
• Erwan Rauwel,
• Frédérique Ducroquet and
• Protima Rauwel

Beilstein J. Nanotechnol. 2021, 12, 1078–1092, doi:10.3762/bjnano.12.80

• of ITO. Furthermore, a decrease in sheet resistance (from 500 to 30 Ω) when Ag nanowires are added to graphene increases the ability of graphene to function as a current-spreading layer [43]. Equivalent to Ag, SPR of AuNP can also be applied to the anode in order to enhance the overall EL of the LED

Revealing the formation mechanism and band gap tuning of Sb₂S₃ nanoparticles

• Maximilian Joschko,
• Franck Yvan Fotue Wafo,
• Christina Malsi,
• Danilo Kisić,
• Ivana Validžić and
• Christina Graf

Beilstein J. Nanotechnol. 2021, 12, 1021–1033, doi:10.3762/bjnano.12.76

• findings suggest a fiber-like growth at the tips and a layered growth around the individual bristles and the whole rod. However, the particles did not seem to be bundles of nanowires, leading to the assumption that the different, fiber-like growing parts of one particle were fusing. Since the tips remained

Uniform arrays of gold nanoelectrodes with tuneable recess depth

• Elena O. Gordeeva,
• Ilya V. Roslyakov,
• Alexey P. Leontiev,
• Alexey A. Klimenko and
• Kirill S. Napolskii

Beilstein J. Nanotechnol. 2021, 12, 957–964, doi:10.3762/bjnano.12.72

• same time, only a minor part of nanowires is known to grow through the whole thickness of a template when potentiostatic electrodeposition is used [22][23][24][25]. Not only electrodeposition conditions but also thickness and structural defects in the AAO template influence the completeness of the

• surface in the proposed NEAs. At the third stage (Figure 1c), Cu was grown until the nanowires reached the AAO top surface and a continuous metal layer was formed on it. This Cu layer served as current collector during operation of the Au NEAs. Finally, the initial Cu current collector and the first Cu

• surface. Segment 3 – copper At this step, a key quality parameter is the percentage of pores filled by the metals completely from the bottom to the top of the AAO template. Only nanowires in this type of pores can take part in an electrochemical reaction during the operation of the NEAs because only these

The role of deep eutectic solvents and carrageenan in synthesizing biocompatible anisotropic metal nanoparticles

• Nabojit Das,
• Akash Kumar and
• Raja Gopal Rayavarapu

Beilstein J. Nanotechnol. 2021, 12, 924–938, doi:10.3762/bjnano.12.69

• nanowires through a NaBH4-assisted rapid reduction of HAuCl4 in a DES (mixture of reline and ethaline) [94]. The strong coordination of [AuCl4]− in reline exhibited a sixfold enhanced catalytic activity. Apart from the high catalytic activity, nanoparticles produced in DESs showed no cytotoxicity in vitro

The role of convolutional neural networks in scanning probe microscopy: a review

• Ido Azuri,
• Irit Rosenhek-Goldian,
• Neta Regev-Rudzki,
• Georg Fantner and
• Sidney R. Cohen

Beilstein J. Nanotechnol. 2021, 12, 878–901, doi:10.3762/bjnano.12.66

• image types was achieved, such as in images of cells and worms, enabling efficient cell-counting and viability prediction, as well as of silver nanowires. Image classification and segmentation CNNs are popular for cell classification. A CNN model based on actin-labeled fluorescence microscopy images

Comprehensive review on ultrasound-responsive theranostic nanomaterials: mechanisms, structures and medical applications

• Sepand Tehrani Fateh,
• Lida Moradi,
• Elmira Kohan,
• Michael R. Hamblin and
• Amin Shiralizadeh Dezfuli

Beilstein J. Nanotechnol. 2021, 12, 808–862, doi:10.3762/bjnano.12.64

Recent progress in magnetic applications for micro- and nanorobots

• Ke Xu,
• Shuang Xu and
• Fanan Wei

Beilstein J. Nanotechnol. 2021, 12, 744–755, doi:10.3762/bjnano.12.58

• magnetoelectric core–shell composite nanowires had a magnetostrictive core and a piezoelectric shell, and it exhibited a strain-mediated magnetoelectric effect. In terms of device design and manufacturing, this biphasic core–shell configuration offered greater flexibility than single-phase magnetoelectric

• trigger drug release. The fabrication method of Chen’s team yielded not only easily adjustable length and diameter of the nanowires, but also excellent interface coupling between the piezoelectric and magnetostrictive phases. It enabled precise magnetic manipulation on patterned surfaces and 3D swimming

• also showed greater stability and faster rate of stabilization [87]. There are also differences in the form of the magnetic field. Chen et al. [76] introduced a type of conical rotating magnetic field for actuating a 3D propulsion mode for nanowires, when studying hybrid magnetoelectric nanowires for

Electromigration-induced formation of percolating adsorbate islands during condensation from the gaseous phase: a computational study

• Alina V. Dvornichenko,
• Vasyl O. Kharchenko and
• Dmitrii O. Kharchenko

Beilstein J. Nanotechnol. 2021, 12, 694–703, doi:10.3762/bjnano.12.55

• [42], control of surface roughness [43] and morphology of islands or nanowires [26][44][45][46][47], as well as control of adsorbate transfer to graphene [48]. Thus, the effects of EM induced by the presence of a potential difference on opposite sides of the substrate can significantly affect the

Nanogenerator-based self-powered sensors for data collection

• Yicheng Shao,
• Maoliang Shen,
• Yuankai Zhou,
• Xin Cui,
• Lijie Li and
• Yan Zhang

Beilstein J. Nanotechnol. 2021, 12, 680–693, doi:10.3762/bjnano.12.54

• direction of future medicine. Zhang et al. [31] developed a self-powered implantable blood glucose meter based on the piezo-enzymatic-reaction coupling effect of GOx@ZnO (GOx: glucose oxidase) nanowires. By collecting the mechanical energy generated by human movement, the output voltage provided information

• . Lee et al. proposed a based Hg2+ ion sensor based on ZnO nanowires and carbon nanotubes for detecting toxic pollutants [17]. The ZnO nanowire (NW) array acted as power source. When Hg2+ ions were detected, the system powered a light-emitting diode (LED). Li et al. designed a self-powered heavy metal

• largely influenced by the surface carrier density on the surface of the nanowires. The adsorption of gas molecules can change the surface carrier density by the shielding effect, so the output of the sensor is very sensitive to the gas concentration. Compared with traditional metal oxide semiconductor

A review of defect engineering, ion implantation, and nanofabrication using the helium ion microscope

• Frances I. Allen

Beilstein J. Nanotechnol. 2021, 12, 633–664, doi:10.3762/bjnano.12.52

• into the YBCO thin film and thus be used to define precise sample geometries, without material removal. For example, high-dose irradiation over larger areas leaving a narrow gap in between has been used to define YBCO nanowires, which were then line-irradiated at lower dose to form nanowire-based

• properties Further defect engineering studies using the HIM have been concerned with tuning the thermal properties of materials. The first example of this demonstrated site-selective engineering of thermal conductivity along the length of individual nanowires [70]. Here, Zhao et al. irradiated discrete

• sections of free-standing crystalline silicon nanowires of 160 nm diameter to a series of target doses. It was found that a dramatic decrease in thermal conductivity occurred already at relatively low doses, corresponding to point defect concentrations of only a few percent. This result indicated a strong