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

• stabilizes the favorable orientation of histidine. Then a nucleophilic attack by serine on the Si–O bond of the precursor molecule results in a Ser–O–Si(OR)3 transitory complex. The hydrolysis is completed by the addition of water, separating the protein and the hydrolyzed precursor molecule, and the release

Cyclodextrins as eminent constituents in nanoarchitectonics for drug delivery systems

• Makoto Komiyama

Beilstein J. Nanotechnol. 2023, 14, 218–232, doi:10.3762/bjnano.14.21

• resultant well-organized orientation of functional groups in CyD-based nanoarchitectures, should be very appropriate to yield both stable encapsulation of nucleic acid drugs and their prompt release when needed. 3.1 CyD-based nanoarchitectures for delivery of siRNA The therapeutic nucleic acid siRNA is

• CyD molecules are arranged in a predetermined position (and orientation) by molecular imprinting. Thus, their assembly as a whole binds the large drug strongly and selectively. Many CyD-based carriers of drugs were prepared by means of this methodology and used for DDSs [111]. For example, ʟ-DOPA was

The influence of structure and local structural defects on the magnetic properties of cobalt nanofilms

• Alexander Vakhrushev,
• Aleksey Fedotov,
• Olesya Severyukhina and
• Anatolie Sidorenko

Beilstein J. Nanotechnol. 2023, 14, 23–33, doi:10.3762/bjnano.14.3

• estimate the influence of the disturbances in the atomic arrangement inside the crystal lattice, in the destruction and fragmentation zones of spin orientation inside the material, and overall magnetization of the sample. Description and Conditions of the Numerical Experiment The structure and magnetic

• the crystal lattice of magnets largely determine the type and shape of the resulting magnetic anisotropy. In ferromagnets, magnetic anisotropy is characterized by the magnitude and orientation of the magnetization, as well as by the change in the magnetic energy of the material. The main causes of

• clarity, so that the orientation of individual atom spins could be easily traced. Subsequently, the two selected systems were exposed to an external magnetic field with induction Bext = 1.0 T in the ox axis direction (along the nanofilm surface for the real structure variant) for 100 ps. The result of the

Electrical and optical enhancement of ITO/Mo bilayer thin films via laser annealing

• Abdelbaki Hacini,
• Ahmad Hadi Ali,
• Nurul Nadia Adnan and
• Nafarizal Nayan

Beilstein J. Nanotechnol. 2022, 13, 1589–1595, doi:10.3762/bjnano.13.133

• seen that the predominant peaks are (222) and (400), which are the preferred orientations before and after laser annealing. The intensities of the crystallite peaks orientation increased and attained a maximum at 200 mJ. The crystallite size (D) and the dislocation density (δ) were determined from the

• size obtained by XRD analysis. Figure 4 shows the correlation between the grain size evolution and crystallite size corresponding to the (400) orientation. This variation is due to the rearrangement of the crystallites during the laser annealing of the IM bilayer thin film structure. Moreover, both

• analyses show that the ITO/Mo has a polycrystalline structure. As well, it can be seen from the grain size analysis that the energy of 120 mJ gives the highest grain size and good crystallinity because most of the orientation of the crystallites appears in the XRD results. Figure 5 shows the optical

From a free electron gas to confined states: A mixed island of PTCDA and copper phthalocyanine on Ag(111)

• Alfred J. Weymouth,
• Emily Roche and
• Franz J. Giessibl

Beilstein J. Nanotechnol. 2022, 13, 1572–1577, doi:10.3762/bjnano.13.131

• from SPA-LEED and STM experiments [25]. As reported previously [16], the PTCDA molecules within a given phase all have the same orientation. The lower lobes of the CuPc molecules appear brighter, which might be an indication that the CuPc molecules do not lie flat in this configuration. This would be

• orientation of the PTCDA molecules can be verified by acquiring dI/dV spectra at −0.39 V, which is an energy level corresponding to the localized LUMO level [27], which we refer to as the F-LUMO. The F-LUMO state (although not obviously present in Figure 2b as a local maximum in the spectrum) can be clearly

Single-step extraction of small-diameter single-walled carbon nanotubes in the presence of riboflavin

• Polina M. Kalachikova,
• Anastasia E. Goldt,
• Eldar M. Khabushev,
• Timofei V. Eremin,
• Timofei S. Zatsepin,
• Elena D. Obraztsova,
• Konstantin V. Larionov,
• Liubov Yu. Antipina,
• Pavel B. Sorokin and
• Albert G. Nasibulin

Beilstein J. Nanotechnol. 2022, 13, 1564–1571, doi:10.3762/bjnano.13.130

• riboflavin assembly (Figure 5b), different bonding patterns are observed depending on the mutual orientation of the adjacent isoalloxazine moieties. The strength of bonding between neighboring riboflavin molecules is proportional to the type of riboflavin helix around a particular SWCNT. The yield 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

• forms a porous structure. There is a disparity in the particle sizes measured with SEM and XRD, because the particle sizes detected using these two techniques are not in the same orientation, and the terms "particle size" and "crystal size" refer to different concepts (a particle may contain several or

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

• -continuum (QC) method. Four variables (i.e., crystal orientation, workpiece thickness, clearance between the punch and the substrate, and the taper angle of punch) are used to explore their effect during the nano-punching process. The shear stress distribution is used to express the punching effect on the

• punch and on both sides of the substrates. Besides, fracture strength, residual flash, and the atomic displacement vector are observed and discussed regarding the behaviors of the nano-punching process under various conditions. Based on the results, the Al workpiece with the X[111]Y[−110] orientation

• strength at a specific structural orientation [51]. Besides, Tran et al. studied the friction and scratch characteristics of pure aluminum by the QC method. The bump width to the bump pitch (W/P) value, scratch depth, surface roughness, and indenter radius were set as variables in order to explore the

Enhanced electronic transport properties of Te roll-like nanostructures

• E. R. Viana,
• N. Cifuentes and
• J. C. González

Beilstein J. Nanotechnol. 2022, 13, 1284–1291, doi:10.3762/bjnano.13.106

• ). Detailed analysis of the SAED patterns, acquired along the [−1−20] zone axis, using CrysTBox software [22][23] demonstrates that the roll-like nanostructure is crystalline. The one-dimensional nanostructure has the trigonal crystal structure of bulk Te, growing in the [001] orientation (indicated by a

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

• too low. Scanning electron micrograph of electrospun nanofibers. One can see the random orientation of the individual fibers forming a kind of mesh. Peel-off force measurement of polished (a) and LIPSS-covered (b) steel samples. The applied weights and hence the normal forces are equal in panels (a

Role of titanium and organic precursors in molecular layer deposition of “titanicone” hybrid materials

• Arbresha Muriqi and
• Michael Nolan

Beilstein J. Nanotechnol. 2022, 13, 1240–1255, doi:10.3762/bjnano.13.103

• the origin of the different thicknesses of EG–titanicone and GL–titanicone films observed in experimental work. We find that EG and GL coupled with TiCl4 can orient in a flat lying configuration on anatase while on rutile, the preferred orientation is upright. When combined with Ti(DMA)4, EG and GL

• orientation of GL when deposited on Si surfaces, DFT shows that the desired upright orientation of GL could be energetically favourable on a rutile TiO2 surface and this provides motivation to develop a lower temperature rutile TiO2/TiCl4–GL process where higher growth per cycle could be achieved. We note

• important role on the orientation of the organic species. The Ti–O distances to the EG and GL in the upright and flat lying configurations are presented in Table S3 (Supporting Information File 1). The computed distances show that the Ti–O bond to the molecules does not change significantly when EG and GL

A super-oscillatory step-zoom metalens for visible light

• Yi Zhou,
• Chao Yan,
• Peng Tian,
• Zhu Li,
• Yu He,
• Bin Fan,
• Zhiyong Wang,
• Yao Deng and
• Dongliang Tang

Beilstein J. Nanotechnol. 2022, 13, 1220–1227, doi:10.3762/bjnano.13.101

• designed a unit cell structure based on the geometric phase (i.e., Pancharatnam–Berry phase) principle [30][31]. Generally, metasurfaces based on geometric phases are easier to process, and the phase modulation in the whole 2π range can be achieved by simply changing the orientation of the unit cell. Also

• used as unit cells of the two metasurfaces. The fused silica glass is used as substrate in the SSL. Theoretically, for the metasurface based on the geometric phase principle, the phase modulation of the transmitted RCP light is exactly twice of the orientation of the unit cell under the LCP incidence

• , height H = 600 nm, and period P = 250 nm × 250 nm. It is demonstrated in Figure 3b that the transmittance varies only little for different orientation angles and the modulated phase changes almost linearly with a factor of two, which also proves the geometric phase principle and the excellent performance

Design of surface nanostructures for chirality sensing based on quartz crystal microbalance

• Yinglin Ma,
• Xiangyun Xiao and
• Qingmin Ji

Beilstein J. Nanotechnol. 2022, 13, 1201–1219, doi:10.3762/bjnano.13.100

• significant difference in the binding with a certain group of CDs. For example, the hydroxy group of (+)-methyl ʟ-lactate interacts with the methoxy group of MP-β-CD through hydrogen bonding. However, (−)-methyl ʟ-lactate does not undergo similar interactions due to the orientation difference of the hydroxy

• odor molecules with 96% accuracy. Besides regulating the porous structure and functionalities of MOFs, it may also improve the chiral sensing performance by controlling the orientation growth of MOFs to the assembled composite films on the QCM surfaces. Wöll and Fischer et al. reported the construction

• substances [117]. Various metal or inorganic materials have been explored as chiral selectors in QCM systems based on different strategies and techniques. Sarkar et al. used tartaric acid as a chiral inducer to control the crystalline orientation of CuO films based on the electrodeposition method [118]. The

Influence of water contamination on the sputtering of silicon with low-energy argon ions investigated by molecular dynamics simulations

• Grégoire R. N. Defoort-Levkov,
• Alan Bahm and
• Patrick Philipp

Beilstein J. Nanotechnol. 2022, 13, 986–1003, doi:10.3762/bjnano.13.86

• sample. The water molecules were equilibrated using the ReaxFFOH(2017) [24] potential in a fully periodic space using the NPT ensemble. Since the adsorption of water molecules on a surface is a random process, the orientation of the molecules could freely evolve. Snapshots of water equilibration can be

• , and this orientation is maintained for the energy transfer to the target atoms. Interestingly, the partial sputtering yields of hydrogen and oxygen atoms are the highest at incidence angles between 70 and 80° (i.e., above angles where the silicon sputtering yields are the highest), leading to the

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

• proportions and orientation differed depending on the location on the mandible. The structures faded and eventually disappeared towards the apex and hairless edge of the mandible. It is possible that the scales in these areas are worn out by intensive use. However, it can be assumed that this is the normal

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

• fact that the proteins in the ECM (such as fibronectin, vitronectin, collagen, and laminin) are adsorbed in a denatured state, and their orientation becomes unsuitable for cell binding [66]. Cells (e.g., osteoblasts) are more likely to attach to more hydrophilic surfaces and exhibit the strongest

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

• transform (FFT) calculated from the image reported in Figure 2a. Four hexagonal domains can be identified, differing by their angular orientation with respect to the substrate. Interestingly, the domains do not possess a well-defined epitaxial relation with respect to the (5 × 5) lattice of ZnTPP

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

• . The surface energy of the eutectic Ga–In–Sn melt at the melting point has been reported to be 587 mN/m [21], while published values for SiOx, PtSi, and Au are = 53 mN/m [22], = 1150–1300 mN/m depending on its orientation [23], = 1710 mN/m [24]. These values lead to the following results for the

• ]. Depending on the surface orientation, a range of values between 0.6 N/m and 2.98 N/m has been reported. The values of and determined in this work are significantly lower than and Due to its chemical inertness, reactivity between PtSi and eutectic Ga–In–Sn melt can be ruled out. Also, reactions between

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

• structure or orientation of the monocrystalline coordination polymers are hardly affected. However, when solids have a similar lattice structure with the grown coordination polymers, epitaxy happens to guide the growth of the coordination polymers. The crystallographic orientation of the grown coordination

• find appropriate substrates with lattice similarity to the preferred crystallographic orientation of the targeted coordination polymer. Parallelly aligned Cu(OH)2 nanobelts were used to guide the epitaxial growth of Cu2(BDC)2 (BDC = benzenedicarboxylic acid). Centimeter-scale micropore alignment was

Modeling a multiple-chain emeraldine gas sensor for NH₃ and NO₂ detection

• Hana Sustkova and
• Jan Voves

Beilstein J. Nanotechnol. 2022, 13, 721–729, doi:10.3762/bjnano.13.64

• several chains were modeled, between two chains (Figure 3 and Figure 4). Also, the orientation of the gas molecule was varied. Apart from these variations, one position and one orientation of the gas molecule was determined utilizing energy minimizing optimization. For all these situations, computation of

• chosen fixed positions of ammonia and nitrogen dioxide molecules. We have computed the local energy minima through molecular dynamics, which results in the optimized position and orientation of the gas molecule. The spatial orientation of the gas molecules was estimated by these optimizations. Next, one

• as well. The I–V characteristics were computed for several molecule positions near the doped and near the undoped nitrogen atoms, see above. The molecule orientation was estimated through molecular dynamics optimization. The resistance from the linear part of the I–V characteristics was used to

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

• range from −2 (red) over 0 (white) to +2 (blue). The orientation of the molecule is rotated by about 90° along the z-axis of image (a) to show the RBD surface that binds to the ACE2 cell receptor. Image modified from PDB 6VYB [3]. Peptide candidates (blue) docked to the SARS-CoV-2 RBD (white). (a) ACE2

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

• orientations was tested [29]. Cooling properties of the CuO/water nanofluid were observed at each orientation. Moreover, efficient and accurate mathematical models were used to obtain readings that were precisely similar to experimental values. A maximum heat transfer rate was recorded in the right-oriented

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

• , three AFM equations were found that represent the general case for a probe oscillating in an arbitrary direction. A probe orientation different from the surface normal and its oscillation in the vector force field above the surface has important consequences on the measured force response and

• orientation of and violates a fundamental assumption of the commonly used inversion algorithms [4][5]: The tip sampling path segments are not overlapping when moving the tip along the data recording path for an inclined oscillation. The resulting error in the force recovery is shown in Figure 4c, where the

Sodium doping in brookite TiO₂ enhances its photocatalytic activity

• Boxiang Zhuang,
• Honglong Shi,
• Honglei Zhang and
• Zeqian Zhang

Beilstein J. Nanotechnol. 2022, 13, 599–609, doi:10.3762/bjnano.13.52

• , the brookite NaxTi1−xO2 transforms into Na2Ti6O13 by a twinning process with the orientation relationship of [1−2−3]Matrix//[1−23]Twins and (−2−10)Matrix//(1−1−1)Twins. The differences in the ionic radius and the electronegativity between Na and Ti destroy the local atomic arrangement of the brookite

• interplanar spacing values are 3.5092 and 3.4619 Å, respectively. Thus, the orientation relationship between the matrix and twins is // and // The twinning effect in the brookite structure may be the major driven force of the phase transformation from the brookite NaxTi1−xO2 to Na2Ti6O13. Such transformation

A new method for obtaining the magnetic shape anisotropy directly from electron tomography images

• Cristian Radu,
• Ioana D. Vlaicu and
• Andrei C. Kuncser

Beilstein J. Nanotechnol. 2022, 13, 590–598, doi:10.3762/bjnano.13.51

• maintaining the labeling at the contact between adjacent particles. Shape evaluation: The procedure consists of fitting each separated particle with an ellipsoid and recovering information about size, axis ratios, and orientation of the long axis from the fit. Both the direction and the magnitude of the semi

• rotation axes. This assumption is usually valid for the vast majority of MNPs used in practice. Output size, shape, and anisotropy distributions: A file containing MNP volume, position of its center of mass, magnitude and orientation of the three semi-axes under the ellipsoidal shape approximation for all

• software. Regarding this, a test data volume filled with ellipsoids has been generated (Figure 3). Again, size, shape, position, and orientation of the ellipsoids have a Gaussian distribution in space, this time without the constraint of no overlap. Experimentally obtained system A system of iron oxide