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Search for "contact" in Full Text gives 1150 result(s) in Beilstein Journal of Nanotechnology. Showing first 200.

Growing up in a rough world: scaling of frictional adhesion and morphology of the Tokay gecko (Gekko gecko)

  • Anthony J. Cobos and
  • Timothy E. Higham

Beilstein J. Nanotechnol. 2022, 13, 1292–1302, doi:10.3762/bjnano.13.107

Graphical Abstract
  • structure on speed and acceleration capacity in climbing geckos, and they found that acceleration was greatest on the smoothest surface (wood) where the most contact between the adhesive system and the surface could be made [27]. This illustrates that the main issue faced by geckos that are attaching via
  • adhesive pads is the contact area between the setae and the surface. With increasingly rough surfaces, the area for contact decreases, leading to decreased adhesive performance. In a modeling framework, the force of adhesion can be related to surface energy of the substrate, the area of the adhering pad
  • ][37]. A key factor that is relatively unexplored is that the morphology of the adhesive system likely changes with body size, which can then impact the amount of contact made between the adhesive system and the surface on which it is clinging or moving. For example, setal length and toepad area have
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Published 09 Nov 2022

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

Graphical Abstract
  • the case for these reasons: (1) Due to the smaller radius, the fiber also becomes softer. In consequence, the easier deflection can increase the contact area, resulting in larger forces. The van der Waals force is proportional to the root of the radius, μ ∼ √R, and the materials stiffness, expressed
  • by the area moment of inertia J, is proportional to the fourth power of the radius, J ∼ R4. Hence, the fiber gains more contact area much faster than the force decreases. (2) With a smaller radius, more fibers can attach simultaneously to the surface, which leads to a further increase in the total
  • approach related to the surface free energy of the fluid, we use an energy approach related to the bending energy of the nanofibers to describe the fiber adhesion on structured surfaces. An important point is that the theory presented here deals with cylindrical fibers that come into contact with the
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Published 07 Nov 2022

Studies of probe tip materials by atomic force microscopy: a review

  • Ke Xu and
  • Yuzhe Liu

Beilstein J. Nanotechnol. 2022, 13, 1256–1267, doi:10.3762/bjnano.13.104

Graphical Abstract
  • a homemade cantilevered non-contact atomic force microscopy (NC-AFM) system. As the first step of tip sharpening, the focus is on the controlled extraction of individual clusters. The experimental results show that controlled extraction of individual clusters induces a change in tip sharpness, which
  • assembly methods, direct growth of carbon nanotubes by chemical vapor deposition (CVD) allows for increased bond strength between CNT tips and AFM probes. A pore growth method was used by Hafner et al. [42]. The method uses AFM imaging in contact mode to flatten the silicon tip, followed by hydrogen
  • percussive mode AFM imaging, and the growth of PdNWCNT does not significantly decrease the cantilever spring constant and cantilever mass factor. PdNWCNTs showed better performance than standard CNTs in some SPM applications. For example, because it is difficult to form good ohmic contact CNTs, the existence
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Published 03 Nov 2022

Roll-to-roll fabrication of superhydrophobic pads covered with nanofur for the efficient clean-up of oil spills

  • Patrick Weiser,
  • Robin Kietz,
  • Marc Schneider,
  • Matthias Worgull and
  • Hendrik Hölscher

Beilstein J. Nanotechnol. 2022, 13, 1228–1239, doi:10.3762/bjnano.13.102

Graphical Abstract
  • unwanted dirt [5][6]. The lotus effect is commonly achieved by hierarchical nano- and micro-structuring of surfaces made from materials with low surface energy leading to very high contact angles (above 150°). This strategy is inspired by the lotus leaf [1] but can be found on many other surfaces in nature
  • a significant increase of the contact angle of water droplets. The fractal structure minimizes contact area as well as adhesion forces between surface and water droplet, thereby equipping the surface with self-cleaning properties equivalent to the lotus effect [24]. Additionally, the high increase
  • comparable high contact angle (95–100°, depending on the exact type [25][26][27]), which helps to achieve a high contact angle also for the structured surface. Second, we know from previous studies that it has a comparable wide process window for the hot pulling of nanofur [28]. Third, polypropylene is well
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Published 31 Oct 2022

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

Graphical Abstract
  • occurs when a liquid is in contact with a solid with a surface charge. This interaction is mainly dominated by the electric double layer (EDL), which consists of a layer of ions (Stern layer) that is tightly adsorbed to the charged surface and a layer of counter ions (diffusion layer) that is attracted
  • interaction. The actual charge transfer is much more complicated, involving the contact angle, dielectric function, temperature, and ion concentration [15][16][17]. In MEGs, compared to bulk materials, nanoarchitectonics yields a higher specific surface area to the active material, which makes the contact
  • ion species. Dropping a droplet of 80 μL 0.6 M CuCl2 solution from 15 cm above the contact point onto a 70° tilted graphene surface under gravity may create a pulse voltage of 30 mV and a short-circuit current of 1.7 μA, as shown in Figure 2c–f. Carbon nanoparticles form nanoscale networks by stacking
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Published 25 Oct 2022

Microneedle-based ocular drug delivery systems – recent advances and challenges

  • Piotr Gadziński,
  • Anna Froelich,
  • Monika Wojtyłko,
  • Antoni Białek,
  • Julia Krysztofiak and
  • Tomasz Osmałek

Beilstein J. Nanotechnol. 2022, 13, 1167–1184, doi:10.3762/bjnano.13.98

Graphical Abstract
  • a constant controlled rate according to zero-order kinetics [79][80][81]. Drug-loaded soft contact lenses can be classified as non-dissolving implants [82][83]. Satisfactory results are also obtained with in situ gelling liquid implants [84][85] or film forming liquids [86][87][88]. In addition to
  • ) [130], and poly(lactic-co-glycolic)acid (PLGA) [131] are widely investigated as microneedle materials. Among them, there are hydrogel-forming agents swelling upon the contact with interstitial fluid in the skin during microneedle application. These polymers include poly(ethylene glycol) diacrylate
  • swelling upon the contact with the fluid at the administration site. It is noteworthy that the polymer matrix does not dissolve under physiological conditions and can be removed after the drug is released [117][144]. As the microneedles absorb interstitial fluid from the surrounding tissue, they can be
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Published 24 Oct 2022

A cantilever-based, ultrahigh-vacuum, low-temperature scanning probe instrument for multidimensional scanning force microscopy

  • Hao Liu,
  • Zuned Ahmed,
  • Sasa Vranjkovic,
  • Manfred Parschau,
  • Andrada-Oana Mandru and
  • Hans J. Hug

Beilstein J. Nanotechnol. 2022, 13, 1120–1140, doi:10.3762/bjnano.13.95

Graphical Abstract
  • macroscopic wire tip to the free prong. Compared to the typically used microscopic AFM cantilevers, the tuning fork sensor has a rather high stiffness, k ≈ 2 kN/m. This facilitates AFM operation with small oscillation amplitudes (A < 100 pm) because a snap-to-contact or instabilities of the phase-locked loop
  • pulley system that locks in at the microscope bottom such that a mechanical contact between the Cu cone and the cone-shaped part of the LHe microscope shield is achieved. To obtain access to the microscope, the LN2 shield can be rotated such that it connects to the inner LHe shield to open up an access
  • sphere running on a hardened steel plate. Note that initially a sapphire plate was used. However, we found the plate cracked after a few days of piezo motor operation, presumably caused from an ultrasound-actuated contact resonance of the Al2O3 sphere on the sapphire plate arising from the triangular
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Published 11 Oct 2022

Green synthesis of zinc oxide nanoparticles toward highly efficient photocatalysis and antibacterial application

  • Vo Thi Thu Nhu,
  • Nguyen Duy Dat,
  • Le-Minh Tam and
  • Nguyen Hoang Phuong

Beilstein J. Nanotechnol. 2022, 13, 1108–1119, doi:10.3762/bjnano.13.94

Graphical Abstract
  • adding ZnO NPs into the solutions containing E. coli, the suspensions were stirred. Samples were taken out at different contact times of 1, 3, and 6 h to evaluate the influence of time on the antibacterial efficiency. The solution was obtained after being diluted to decimal concentrations of 1/10, 1/100
  • with ZnO NPs doses of 1, 5, and 10 mg/mL and contact time intervals of 1, 3, and 6 h. The ZnO NP concentration of 1 mg/mL is not enough to inhibit all E. coli bacteria after 6 h of treatment. By increasing the concentration of ZnO NPs to 5 mg/mL at contact times of 3 and 6 h, the inhibitory efficiency
  • reached 99.83 and 100%, respectively. When the dose of the photocatalyst increased to 10 mg/mL, the E. coli inhibition efficiency reached 99.35% with a contact time of 1 h and the efficiency was 100% when the contact time was 3 h. The results of E. coli bacteria inhibition by ZnO NPs synthesized by the
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Published 07 Oct 2022

Recent advances in green carbon dots (2015–2022): synthesis, metal ion sensing, and biological applications

  • Aisha Kanwal,
  • Naheed Bibi,
  • Sajjad Hyder,
  • Arif Muhammad,
  • Hao Ren,
  • Jiangtao Liu and
  • Zhongli Lei

Beilstein J. Nanotechnol. 2022, 13, 1068–1107, doi:10.3762/bjnano.13.93

Graphical Abstract
  • surface of CDs. They observed the change in PL characteristics of CDs during a period of one to four weeks and concluded that when amino-rich CDs come in contact with oxygen in the air, agglomeration of CDs is induced, and, hence, luminescence changes slowly from red to green color (Figure 5) [102]. A
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Published 05 Oct 2022

Biomimetic chitosan with biocomposite nanomaterials for bone tissue repair and regeneration

  • Se-Kwon Kim,
  • Sesha Subramanian Murugan,
  • Pandurang Appana Dalavi,
  • Sebanti Gupta,
  • Sukumaran Anil,
  • Gi Hun Seong and
  • Jayachandran Venkatesan

Beilstein J. Nanotechnol. 2022, 13, 1051–1067, doi:10.3762/bjnano.13.92

Graphical Abstract
  • tensile strength of ≈7.05 MPa. According to the findings in vitro, the combination of scaffolds promotes fast cell-to-cell contact, which boosts the regeneration impact on pre-osteoblast (MC3T3-E1) cell proliferation, growth, and differentiation [94]. The impact of a hybrid nanocomposite of poly(3
  • wettability of the chitosan/reduced graphene oxide composites with specific acetic acid and lactic acid shows water contact angles of (75.40° ± 4.32°) and (36.71° ± 4.53°) [60]. The anticancer agent cisplatin was loaded into graphene oxide/hydroxyapatite/chitosan composites to enable proliferation of
  • computed tomography (CT) scan radiographs which show good bone lodging in all implants. There are noticeable holes at the hydroxyapatite implant interface. Ag–Si hydroxyapatite implants, on the other hand, have a smooth contact between the host bone and the implant. Acemannan and chitosan coatings have
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Published 29 Sep 2022

Spindle-like MIL101(Fe) decorated with Bi2O3 nanoparticles for enhanced degradation of chlortetracycline under visible-light irradiation

  • Chen-chen Hao,
  • Fang-yan Chen,
  • Kun Bian,
  • Yu-bin Tang and
  • Wei-long Shi

Beilstein J. Nanotechnol. 2022, 13, 1038–1050, doi:10.3762/bjnano.13.91

Graphical Abstract
  • ). Figure 3d shows an HRTEM image of BOM-20 composites. The lattice fringes of 0.37 nm correspond to the (120) facet of α-Bi2O3 [55]. Meanwhile, the tight contact interface between Bi2O3 and MIL101(Fe) can be clearly observed. Furthermore, the elemental mapping images of BOM-20 (Figure 3e–h) reveal the
  • nanoparticles and tridimensional MIL101(Fe). This 0D/3D heterojunction is conducive to fast separation and migration of the photoproduced electron–hole pairs due to more contact areas between Bi2O3 and MIL101(Fe) and shorter transfer distances of photoinduced charge carriers [8], which results in enhanced
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Published 28 Sep 2022

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

Graphical Abstract
  • the interaction between electrolyte and the electrode surface. We probed the water wetting ability of supported ACC-2 and supportless ACC-2* by measuring the water contact angles (Figure S8a,b, Supporting Information File 1). The rGO-supported ACC-2 material showed a higher water wettability (14 ± 1
  • , materials, characterization data, electrochemical measurements, water contact angle measurements, and comparison of reported ORR activities of Ag-based catalysts. Acknowledgements Authors thank SRM IST for providing Microwave reactor facility and DST-FIST, Department of Chemistry [SR/FST/CST-66/2015(c
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Published 26 Sep 2022

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

Graphical Abstract
  • -contact atomic force microscopy (AFM) using the model Park NX10 AFM. The first experiment was conducted with beam current I as the variable parameter ranging from 7 to 500 pA. However, changing the value of I also changed the beam diameter d, which is a function of I and the working distance (WD). The
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Published 22 Sep 2022

Interaction between honeybee mandibles and propolis

  • Leonie Saccardi,
  • Franz Brümmer,
  • Jonas Schiebl,
  • Oliver Schwarz,
  • Alexander Kovalev and
  • Stanislav Gorb

Beilstein J. Nanotechnol. 2022, 13, 958–974, doi:10.3762/bjnano.13.84

Graphical Abstract
  • development process that led to the anatomical investigation of honeybee mandibles. The hypothesis is that animal species that regularly have close contact with resinous plants or even actively harvest resins may have developed counter-stickiness strategies. This is because animals that permanently stick to a
  • surface is in intensive contact with the sticky material during biting and shaping it. Therefore, the anatomy of bee mandibles was studied, focusing on the medial surface of the mandible tip to find possible reasons for reduced adhesion. Once physical and adhesive propolis properties as well as the
  • , Germany) was attached to the metal spring with cyanoacrylate glue (5925 Ergo® Elastomer–Kisling GmbH, Bad Mergentheim, Germany). The freshly formed, cone-shaped sample of propolis was then mounted on the tip of the capillary without any additional glue. The propolis sample was brought into contact with
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Published 14 Sep 2022

Design of a biomimetic, small-scale artificial leaf surface for the study of environmental interactions

  • Miriam Anna Huth,
  • Axel Huth,
  • Lukas Schreiber and
  • Kerstin Koch

Beilstein J. Nanotechnol. 2022, 13, 944–957, doi:10.3762/bjnano.13.83

Graphical Abstract
  • electron microscopy, gas chromatography–mass spectrometry, and by the determination of water contact angles, contact angle hysteresis, and tilting angles. Wheat leaves of different ages were covered exclusively with wax platelets. The extracted wheat wax was composed of alcohols, aldehydes, esters, and
  • the plant cuticle and, thus, the first contact site of the plant with its biotic and abiotic environment. They form a thin crystalline wax film (less than 1 µm) and often various three-dimensional emerging wax crystals in the nano- and micrometer range (0.5–100 µm) [14][15][16]. Recrystallization of
  • formation of biofilms [25][26]. A measure of the degree of wetting is the contact angle θ (CA). It describes the angle between the liquid–vapor interface and the liquid–solid interface. According to the CA, surfaces can be classified as superhydrophilic (0° < θ < 10°), hydrophilic (10° ≤ θ < 90
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Published 13 Sep 2022

Comparing the performance of single and multifrequency Kelvin probe force microscopy techniques in air and water

  • Jason I. Kilpatrick,
  • Emrullah Kargin and
  • Brian J. Rodriguez

Beilstein J. Nanotechnol. 2022, 13, 922–943, doi:10.3762/bjnano.13.82

Graphical Abstract
  • governing the performance of single and multifrequency Kelvin probe force microscopy (KPFM) techniques in both air and water. Metrics such as minimum detectable contact potential difference, minimum required AC bias, and signal-to-noise ratio are compared and contrasted both off resonance and utilizing the
  • local contact potential difference (CPD) between the probe and the sample. This, in turn, allows the work function of the sample to be measured if the work function of the probe is known and vice versa. The mapping of local electrical properties of the interface is essential to further our understanding
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Published 12 Sep 2022

Bioselectivity of silk protein-based materials and their bio-inspired applications

  • Hendrik Bargel,
  • Vanessa T. Trossmann,
  • Christoph Sommer and
  • Thomas Scheibel

Beilstein J. Nanotechnol. 2022, 13, 902–921, doi:10.3762/bjnano.13.81

Graphical Abstract
  • , natural biological adhesives are complex materials that have evolved to meet the various functional demands. Bioadhesion can be found in the range of the micro- to the macroscale [7]. Adhesion principles include contact mechanical principles such as capillary interactions, viscous forces, non-covalent
  • achieve proper organization and communication, cells produce a large number of adhesion molecules that mediate cell contact phenomena based on receptor–ligand interactions [8]. The ability of mammalian cells to adhere to other cells, tissues, or the extracellular matrix (ECM) via specific molecular
  • cells but to even display antiviral attachment properties [58]. Superhydrophobic surfaces inspired by the Lotus-effect® (>150° contact angle) have been found to diminish bacterial adhesion due to reduced protein surface adsorption [59][60][61]. Superhydrophobicity relies on the combination of chemical
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Published 08 Sep 2022

DNA aptamer selection and construction of an aptasensor based on graphene FETs for Zika virus NS1 protein detection

  • Nathalie B. F. Almeida,
  • Thiago A. S. L. Sousa,
  • Viviane C. F. Santos,
  • Camila M. S. Lacerda,
  • Thais G. Silva,
  • Rafaella F. Q. Grenfell,
  • Flavio Plentz and
  • Antero S. R. Andrade

Beilstein J. Nanotechnol. 2022, 13, 873–881, doi:10.3762/bjnano.13.78

Graphical Abstract
  • B2902A Precision Source/Measure Unit, immediately after the functionalization process. The source–drain bias was fixed at 1 mV, and we applied the gate voltage via a gold electrode in contact with 100 mM PBS or human serum. PBS was used as electrolyte for validation of the graphene functionalization with
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Published 02 Sep 2022

Numerical modeling of a multi-frequency receiving system based on an array of dipole antennas for LSPE-SWIPE

  • Alexander V. Chiginev,
  • Anton V. Blagodatkin,
  • Dmitrii A. Pimanov,
  • Ekaterina A. Matrozova,
  • Anna V. Gordeeva,
  • Andrey L. Pankratov and
  • Leonid S. Kuzmin

Beilstein J. Nanotechnol. 2022, 13, 865–872, doi:10.3762/bjnano.13.77

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  • of 1.1 × 10−16 W/Hz1/2. This was achieved by replacing one of two superconductor–insulator–normal tunnel junctions with a superconductor–normal metal contact. Keywords: cosmic microwave background (CMB); cold-electron bolometer; dichroic antenna; dipole antenna; LSPE-SWIPE; waveguide horn
  • current noise of 4–10 pA/Hz1/2. To optimize the receiver for better noise characteristics, we consider optimized CEBs with a single superconductor–insulator–normal (SIN) tunnel junction and a single superconductor–normal (SN) contact [12]. Combined together, they form a SINS structure. This solution can
  • NEP level for photon-noise limited operations, we have performed a very important optimization for cold-electron bolometer design. We changed one of two SIN tunnel junctions to the SN contact, so it became a SINS structure. This change allowed us to increase current responsivity twice and to improve
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Published 01 Sep 2022

Micro-structures, nanomechanical properties and flight performance of three beetles with different folding ratios

  • Jiyu Sun,
  • Pengpeng Li,
  • Yongwei Yan,
  • Fa Song,
  • Nuo Xu and
  • Zhijun Zhang

Beilstein J. Nanotechnol. 2022, 13, 845–856, doi:10.3762/bjnano.13.75

Graphical Abstract
  • nanomechanical characteristics were tested using a nanoindenter (TriboIndenter, Hysitron Inc., USA). The reduced Young’s modulus, Er, is calculated as where β is a constant related to the shape of the head (for a Berkovich indenter, the value is 1.034). Ac is contact the area and a polynomial function of
  • contact depth. S is the contact stiffness. A Berkovich tip with a tip radius of approximately 100 nm was used for the tests. In order to study the effect of nanomechanical properties of different veins on the lift of the beetle hind wings, the same location of the same vein of three beetles was selected
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Published 26 Aug 2022

Temperature and chemical effects on the interfacial energy between a Ga–In–Sn eutectic liquid alloy and nanoscopic asperities

  • Yujin Han,
  • Pierre-Marie Thebault,
  • Corentin Audes,
  • Xuelin Wang,
  • Haiwoong Park,
  • Jian-Zhong Jiang and
  • Arnaud Caron

Beilstein J. Nanotechnol. 2022, 13, 817–827, doi:10.3762/bjnano.13.72

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  • . The authors compared different modifications of the Hertzian contact mechanical model for elastic solids to account for adhesion. The authors found that the measured adhesion significantly depends on the maximum load applied before retraction. In the case of a plastic contact, adhesion was larger than
  • for an elastic contact, owing to the formation and rupture of chemical bonds between tip and sample in the former case. Furthermore, we used the approach part of the curves to calculate the force–penetration curves according to δ = Z − Fn/Cn. The determination of the interfacial energy γ between an
  • AFM tip and a metallic liquid alloy is based on a balance between the pressure applied by the tip onto the liquid surface and the restoring pressure due to the line tension at the liquid interface, that is, p(δ) = Fn(δ)/A(δ) = γ/P(δ), where A(δ) is the contact area and P(δ) is the perimeter between
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Published 23 Aug 2022

Hierachical epicuticular wax coverage on leaves of Deschampsia antarctica as a possible adaptation to severe environmental conditions

  • Elena V. Gorb,
  • Iryna A. Kozeretska and
  • Stanislav N. Gorb

Beilstein J. Nanotechnol. 2022, 13, 807–816, doi:10.3762/bjnano.13.71

Graphical Abstract
  • . macrophylla Jebb and Cheek, N. mirabilis (Lour.) Druce, and N. rafflesiana Jack [16][17]. The waxy (slippery) zone located inside the pitchers is highly specialized for trapping and retaining of insect prey mainly due to contamination of attachment organs of insects [16], reduction of the real contact area
  • epicuticular wax structures [36]. It was found that on waxy leaves, icing started from nucleation sites on the surface of wax projections or in nanoscale depressions between them. This is why the real contact area of ice crystals was limited to a few sites at the nanoscale on or between wax projections. After
  • thawing, water drops flow off the surface and therefore cannot be potentially re-frozen. The study demonstrated the following effects caused by the wax coverage: (i) Air pockets between wax projections prevent direct contact between the plant cuticle and ice crystals, and (ii) after thawing, the fluid
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Published 22 Aug 2022

Optimizing PMMA solutions to suppress contamination in the transfer of CVD graphene for batch production

  • Chun-Da Liao,
  • Andrea Capasso,
  • Tiago Queirós,
  • Telma Domingues,
  • Fatima Cerqueira,
  • Nicoleta Nicoara,
  • Jérôme Borme,
  • Paulo Freitas and
  • Pedro Alpuim

Beilstein J. Nanotechnol. 2022, 13, 796–806, doi:10.3762/bjnano.13.70

Graphical Abstract
  • , on which the graphene film would make electrical contact. The B2 PMMA/graphene films were then transferred onto the wafer and patterned by O2 plasma, followed by the sacrificial layer removal. Previous to the passivation, Al2O3 was selectively removed to improve the adhesion of the oxide passivation
  • contact pads and graphene transistor channels. Finally, the stopping layer was removed by wet etching, exposing the graphene channel. In both wafers, the GFET channels had nominal dimensions of W = 75 µm and L = 25 µm. The total number of GFETs condidered in this study was 1755 on Wafer 1 and 4200 on
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Published 18 Aug 2022

Gelatin nanoparticles with tunable mechanical properties: effect of crosslinking time and loading

  • Agnes-Valencia Weiss,
  • Daniel Schorr,
  • Julia K. Metz,
  • Metin Yildirim,
  • Saeed Ahmad Khan and
  • Marc Schneider

Beilstein J. Nanotechnol. 2022, 13, 778–787, doi:10.3762/bjnano.13.68

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  • single nanoparticles. For the values of Young’s moduli, the respective curves were treated as follows: The determined spring constant and sensitivity must be applied to calibrate the cantilever deflection. To correct the vertical offset, a baseline subtraction is applied, and the contact point is
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Published 16 Aug 2022

Hierarchical Bi2WO6/TiO2-nanotube composites derived from natural cellulose for visible-light photocatalytic treatment of pollutants

  • Zehao Lin,
  • Zhan Yang and
  • Jianguo Huang

Beilstein J. Nanotechnol. 2022, 13, 745–762, doi:10.3762/bjnano.13.66

Graphical Abstract
  • of pure TiO2-NT and Bi2WO6 powder samples, except for the 90%−Bi2WO6/TiO2-NT nanocomposite, which is ascribed to the higher specific surface area as well as to close contact and uniform formation of the heterostructures in between the TiO2 and Bi2WO6 phases of the Bi2WO6/TiO2-NT nanocomposites. When
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Published 04 Aug 2022
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