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

• forces in KPFM is generally expressed as the minimum detectable CPD [53], and is directly limited by the geometry of the interaction, thermal noise of the cantilever, and the detection noise limits of the AFM [36][54]. Cantilevers have a number of eigenmodes, ωn, where there is a mechanical enhancement

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

• interaction [9]. Generally, integrin-mediated interactions involve a complex series of events including activation, ligand binding, reorganization of the cytoskeleton, and adhesion [13]. In this context, integrin activation is regulated in response to signal cascades inside the cell known as an “inside-out

• ” process initiated by other cell surface receptors, such as chemokine receptors and selectins. The subsequent interaction with cytoplasmic factors leads to a conformational switch in the extracellular integrin binding region from a non-adhesive (inactive) to an adhesive state [19]. Moreover, adhesive

• interaction partners for the cellular receptors mentioned above and contain binding sites for further biologically active molecules, including growth factors, which stimulate several subsequent cellular responses, such as growth or differentiation [20][21][22][23]. Prominent examples of ECM proteins are

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

• “systematic evolution of ligands by exponential enrichment” (SELEX), first introduced in 1990 [13]. This methodology includes the exposure of the target molecule to a chemically synthesized random-sequence library (1014–1015 sequences) to allow for the interaction of all binding oligonucleotides to the target

• support this electron transfer from pyrene-modified molecules to graphene as the binding mechanism in π–π interactions between such compounds [35][36][37]. The association of pyrene-modified ZIKV60 aptamers with graphene may also be mediated by charge transfer that assists the interaction between the

Self-assembly of C₆₀ on a ZnTPP/Fe(001)–p(1 × 1)O substrate: observation of a quasi-freestanding C₆₀ monolayer

• Guglielmo Albani,
• Michele Capra,
• Alessandro Lodesani,
• Alberto Calloni,
• Gianlorenzo Bussetti,
• Marco Finazzi,
• Franco Ciccacci,
• Alberto Brambilla,
• Lamberto Duò and
• Andrea Picone

Beilstein J. Nanotechnol. 2022, 13, 857–864, doi:10.3762/bjnano.13.76

• materials possessing antithetic electronic and structural properties. In this frame, the molecule–metal interaction arising at the interface plays a crucial role in determining the morphology and the electronic properties of the hybrid organic/inorganic system. With regard to the structural aspects, a

• relevant charge transfer between the overlayer and the substrate occurs. In contrast, a low Ea is characteristic of physisorbed molecules, for which the adsorption is mediated by the weak van der Waals interaction with the substrate. Chemisorption is the typical scenario for molecules stabilized on

• surfaces for the investigation of their intrinsic properties, the minimization of the molecule–substrate interaction is desirable [20]. Furthermore, a weak molecule/metal electronic coupling is required in organic solar cells, because metallic states promote the relaxation of photo-excitations, lowering

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

• , it was found that their flexibility can increase their mean lift coefficient [21]. In rhinoceros beetles, the elytra is also involved in aerodynamics during takeoff, producing an interaction force between the elytra and the hind wings [22]. To avoid damage or hinder the movement on the ground, the

Ultrafast signatures of magnetic inhomogeneity in Pd_1−xFe_x (x ≤ 0.08) epitaxial thin films

• Andrey V. Petrov,
• Sergey I. Nikitin,
• Lenar R. Tagirov,
• Amir I. Gumarov,
• Igor V. Yanilkin and
• Roman V. Yusupov

Beilstein J. Nanotechnol. 2022, 13, 836–844, doi:10.3762/bjnano.13.74

• fractions by highly mobile s and p electrons (which occurs due to the s–d interaction [40]) should only increase the rate of photoinduced demagnetization on a subpicosecond scale. This mechanism was justified to explain the ultrafast (subpicosecond) transfer of the angular momentum in F/N heterostructures

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

• in Ga. According to the manufacturer, the interaction depth of the XPS was approx. 10 nm. We detected metallic bonded Ga, In, and Sn; thus, we infer that the oxide layer was less than 10 nm thick. Thickness and composition of the surface oxide of a similar newly developed Ga–In–Sn-Zn liquid alloy

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

• weak interaction between these chains [3][4]. Therefore, those 1D materials have defect-free surfaces, high anisotropy, and carrier mobility. For example, TiS3 nanowires obtained by mechanical stripping have a large carrier mobility of about 10000 cm2·V−1·s−1 [5][6][7]. Fibrous phosphorus is also a new

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

• system is usually tested intensively in vitro using cell culture-based assays before application in in vivo studies. Depending on the particle material, the mechanical properties will be influenced, also modulating potentially the particle–cell interaction. For polymeric particles, a higher uptake for

Recent advances in nanoarchitectures of monocrystalline coordination polymers through confined assembly

• Lingling Xia,
• Qinyue Wang and
• Ming Hu

Beilstein J. Nanotechnol. 2022, 13, 763–777, doi:10.3762/bjnano.13.67

• particles were squeezed by ice in a 2D space, forming nanosheets. 2D monocrystalline coordination polymers are anisotropic and, thus, very suitable to enhance inter-crystal interaction by forming laminar stacking superstructures. This concept was earlier demonstrated by applying a solution-based layer-by

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

• presence of the hierarchical TiO2 nanotubes influences and inhibits the crystallinity of Bi2WO6 in between the interface of the two phases, revealing the strong interaction between TiO2 and Bi2WO6 phases [35][36]. Figure 2b displays the FTIR spectra of the hierarchical Bi2WO6/TiO2-NT nanocomposites, pure

• the spectra of pure TiO2-NT and pure Bi2WO6 powder samples, the absorption bands in the Bi2WO6/TiO2-NT nanocomposites all exhibit slight red shifts, demonstrating the close connection, strong interaction, and formation of heterostructures in between Bi2WO6 and TiO2 phases. It is deduced from the XRD

• and 8.1 times higher than those of the Bi2WO6/TiO2 (0.18 h−1) and Bi2WO6-TiO2 (0.08 h−1) samples. This result reveals that the cellulose-derived three-dimensional network structure promotes the homogeneous dispersion of Bi2WO6 nanoparticles on TiO2 nanotubes, as well as an intense interaction and

A nonenzymatic reduced graphene oxide-based nanosensor for parathion

• Sarani Sen,
• Anurag Roy,
• Ambarish Sanyal and
• Parukuttyamma Sujatha Devi

Beilstein J. Nanotechnol. 2022, 13, 730–744, doi:10.3762/bjnano.13.65

• absorption of PT through π stacking interaction between aromatic moieties of GO and the benzene ring of PT. In comparison, the highest cathodic/anodic peak was obtained at −0.58 and −0.05 V, respectively, for the electro-reduction/oxidation of PT on ERGO/GCE. The oxidation/reduction potentials of PT on ERGO

Design and selection of peptides to block the SARS-CoV-2 receptor binding domain by molecular docking

• Kendra Ramirez-Acosta,
• Ivan A. Rosales-Fuerte,
• J. Eduardo Perez-Sanchez,
• Alfredo Nuñez-Rivera,
• Josue Juarez and
• Ruben D. Cadena-Nava

Beilstein J. Nanotechnol. 2022, 13, 699–711, doi:10.3762/bjnano.13.62

• variants of SARS-CoV-2. This research work will be focused on the molecular docking of peptides by molecular dynamics, in addition to an analysis of the possible interaction of these peptides with physiological proteins. This methodology could be extended to design peptides that are active against other

• entry of SARS-CoV-2 into cells is mediated by the interaction of the RBD with the host cell ACE2 receptor [2][3][5]. Figure 1 shows the RBD–ACE2 complex formed at the first stage of the cellular infection by SARS-CoV-2. The formation of the RBD–ACE2 complex is mediated by the amino acid residues F486

• , and their interaction with the RDB is discussed in the following section. Physicochemical parameters and peptide–RBD interaction Solubility, net charge, and size are important physical parameters that need to be considered in the design of novel drugs since these play a role in the distribution in the

Tunable high-quality-factor absorption in a graphene monolayer based on quasi-bound states in the continuum

• Jun Wu,
• Yasong Sun,
• Feng Wu,
• Biyuan Wu and
• Xiaohu Wu

Beilstein J. Nanotechnol. 2022, 13, 675–681, doi:10.3762/bjnano.13.59

• interaction between graphene and incident light plays a key role in these applications. Unfortunately, it is extremely weak owing to the single-atom thickness of graphene monolayers, which severely limits the performance of graphene devices. Various approaches based on different physical mechanisms have been

A superconducting adiabatic neuron in a quantum regime

• Marina V. Bastrakova,
• Dmitrii S. Pashin,
• Dmitriy A. Rybin,
• Andrey E. Schegolev,
• Nikolay V. Klenov,
• Igor I. Soloviev,
• Anastasiya A. Gorchavkina and
• Arkady M. Satanin

Beilstein J. Nanotechnol. 2022, 13, 653–665, doi:10.3762/bjnano.13.57

• bosonic bath. For further analysis, we use a linear model of the interaction between the quantum neuron and the bath: where and are creation and annihilation operators of the i-th bosonic mode, and k is the coupling constant. With an adiabatic change of the input flux, the SQ state can be described in

Antibacterial activity of a berberine nanoformulation

• Hue Thi Nguyen,
• Tuyet Nhung Pham,
• Anh-Tuan Le,
• Nguyen Thanh Thuy,
• Tran Quang Huy and
• Thuy Thi Thu Nguyen

Beilstein J. Nanotechnol. 2022, 13, 641–652, doi:10.3762/bjnano.13.56

• -negative (Escherichia coli O157:H7) bacteria causing hospital-acquired infections was achieved in comparison with the precursor BBR at the same concentration. In addition, the interaction of BBR NPs with bacteria was also investigated in this study. Results and Discussion Chemical characterization of the

• PdI value reached 0.555, indicating a good stability of these BBR NP solutions. This can be explained by the narrow distribution of particle sizes, indicated by the low PDI value, resulting in a sufficiently large repulsive interaction between particles to form a stable dispersion [40]. Glycerol is a

• ratio facilitate interaction and absorption onto the bacterial cell membrane given the benefit of nanoscale size. According to previous studies, BBR can penetrate the phospholipid bilayers and then accumulate in the MRSA cell membrane, in which unsaturated fatty acids are the target of BBR-induced

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

• enables the system to keep the pressure constant but the volume is varied). The temperature of the nanofluid during simulation was maintained at 303 K with 1 bar pressure. Electrostatic and van der Waals forces were imparted on the nonbonded interaction for dispersion. Charges on the system were

• regarding dimensionless velocity demonstrate that the molecular interaction rate is faster in the water/CuO system as compared to the hydrocarbon-based system. However, in Abid et al., the thermal conductivity of kerosene/CuO-based nanofluids was found to be higher than that of water-based nanofluids [53

Quantitative dynamic force microscopy with inclined tip oscillation

• Philipp Rahe,
• Daniel Heile,
• Reinhard Olbrich and
• Michael Reichling

Beilstein J. Nanotechnol. 2022, 13, 610–619, doi:10.3762/bjnano.13.53

• interaction force, the measurement observables, and the probe excitation parameters is defined by an average of the normal force along the sampling path over the oscillation cycle. Usually, it is tacitly assumed that tip oscillation and force data recording follows the same path perpendicular to the surface

• path perpendicular to the surface, provide quantitative information about the details of the tip–surface interaction when properly analysed [2]. Recently, a universal description of quantitative dynamic force microscopy based on the harmonic approximation has been developed [3], yielding three central

• equations that link the physical interaction parameters force and damping with the measurement observables static deflection qs, oscillation amplitude A, and phase φ as well as the excitation parameters frequency fexc and force Fexc. This theory specifically predicts the distant-dependent frequency shift

Revealing local structural properties of an atomically thin MoSe₂ surface using optical microscopy

• Lin Pan,
• Peng Miao,
• Anke Horneber,
• Alfred J. Meixner,
• Pierre-Michel Adam and
• Dai Zhang

Beilstein J. Nanotechnol. 2022, 13, 572–581, doi:10.3762/bjnano.13.49

• Technologie de Troyes & CNRS EMR 7004, 12 Rue Marie Curie, CS42060, 10004 Troyes Cedex, France Center for Light-Matter-Interaction, Sensors and Analytics (LISA+), Eberhard Karls University of Tübingen, Auf der Morgenstelle 15, 72076 Tübingen, Germany 10.3762/bjnano.13.49 Abstract Using a triangular

• -of-plane electric field component dominates. This phenomenon indicates that the face-on oriented CuPc molecules strongly interact with the MoSe2 flake via charge transfer and dipole–dipole interaction. Furthermore, the Raman scattering maps on the irregular MoSe2 surface show a distinct correlation

• the interaction with local dipoles in plasma-treated MoS2 [22]. Additionally, the electronic band structure of MoS2 can be significantly modified after oxygen incorporation into MoS2. The charge transfer from the valence band of partially oxidized MoS2 to the LUMO of R6G can be tuned in resonance with

Detection and imaging of Hg(II) in vivo using glutathione-functionalized gold nanoparticles

• Gufeng Li,
• Shaoqing Li,
• Rui Wang,
• Min Yang,
• Lizhu Zhang,
• Yanli Zhang,
• Wenrong Yang and
• Hongbin Wang

Beilstein J. Nanotechnol. 2022, 13, 549–559, doi:10.3762/bjnano.13.46

• through the interaction between covalent and non-covalent bonds due to the smaller steric hindrance [23][24][25]. The surface of GNPs can be modified by Au–S bonds with molecules containing thiol groups, such as cysteine [26][27][28], 3-mercaptopropionic acid [29], and homocysteine [30]. Also, they easily

Stimuli-responsive polypeptide nanogels for trypsin inhibition

• Petr Šálek,
• Jana Dvořáková,
• Sviatoslav Hladysh,
• Diana Oleshchuk,
• Ewa Pavlova,
• Jan Kučka and
• Vladimír Proks

Beilstein J. Nanotechnol. 2022, 13, 538–548, doi:10.3762/bjnano.13.45

• % (15 µg/mL), and 3.3% (17 µg/mL), respectively. This could be explained by the weak interaction between 125I-radiolabeled BSA and PHEG-Tyr nanogel at pH 4.7 and 25 °C and the low capturing ability of PHEG-Tyr nanogel [32]. As a next step, PHEG-Tyr nanogel loaded with 125I-radiolabeled BSA was incubated

• interaction [35][36]. Our observation indicates that the adsorption of 125I-radiolabeled BSA onto Nα-Lys-NG is mainly driven by hydrophobic interaction. At higher initial concentrations of 125I-radiolabeled BSA, both polypeptide nanogels, Nα-Lys-NG and PHEG-Tyr, are quickly saturated and unable to adsorb

Ciprofloxacin-loaded dissolving polymeric microneedles as a potential therapeutic for the treatment of S. aureus skin infections

• Sharif Abdelghany,
• Walhan Alshaer,
• Yazan Al Thaher,
• Maram Al Fawares,
• Amal G. Al-Bakri,
• Saja Zuriekat and
• Randa SH. Mansour

Beilstein J. Nanotechnol. 2022, 13, 517–527, doi:10.3762/bjnano.13.43

• results also showed that ciprofloxacin released from CIP_MN1 appeared to decrease with time in the upper layers and to increase in deeper layers, as shown by comparing the deposition of ciprofloxacin after 1 h and after 12 h. This was evidenced by p = 0.044 in a two-way ANOVA analysis for the interaction

Design and characterization of polymeric microneedles containing extracts of Brazilian green propolis

• Camila Felix Vecchi,
• Rafaela Said dos Santos,
• Jéssica Bassi da Silva and
• Marcos Luciano Bruschi

Beilstein J. Nanotechnol. 2022, 13, 503–516, doi:10.3762/bjnano.13.42

• show the interaction effects of the independent variables (P407 and EE or GE) on height and base measurements, strength, and printing area in the hard surface. To predict the optimal conditions, a polynomial equation was fitted correlating the relationship between the independent variables and the

• response: where Y is the response (the dependent variable) as function of X1 and X2, b0 is a constant term (the arithmetic mean response of nine batches), b1 and b2 are the estimated coefficients of linear terms, and b12 is the coefficient of the interaction effect. The polynomial terms X112 and X222

• consider the non-linearity, and the interaction term X1X2 shows the response changes when two factors are simultaneously changed. The experiments were randomized to minimize the influence of unexplained variability in the responses. Residual analysis was also conducted to validate the assumptions utilized

Ethosomal (−)-epigallocatechin-3-gallate as a novel approach to enhance antioxidant, anti-collagenase and anti-elastase effects

• Çiğdem Yücel,
• Gökçe Şeker Karatoprak,
• Sena Yalçıntaş and
• Tuğba Eren Böncü

Beilstein J. Nanotechnol. 2022, 13, 491–502, doi:10.3762/bjnano.13.41

• their interaction with skin cells is high. They are unique systems that can be easily shaped by the presence of ethanol in their structures, and their vesicle membranes become very flexible such that they can be transported through pores much smaller than their own diameters [20][21]. In addition, the

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

• chemical enhancement from the electronic interaction between the analyte and the nanosurface [59]. The electromagnetic enhancement factor (EF) can reach up to eleven orders of magnitude in the “hot spots” of the nanosubstrate [60][61], while the chemical EF usually has a value between 10 and 103. Since the

• chemical enhancement owing to the interaction between semiconductor and/or noble metals with the analytes [7][35]. The chemical enhancement is related to the photoinduced charge transfer effect that takes place under the light excitation when the highest occupied molecular orbital (HOMO) and lowest

• fluorophore and the surface plasmon field of the metallic nanostructure. This interaction leads to the enhancement of fluorophore emission, being an adequate method to improve the sensitivity of fluorescence detection of molecules. Based on the above, MEF is also referred to as plasmon-enhanced fluorescence