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Search for "polarity" in Full Text gives 141 result(s) in Beilstein Journal of Nanotechnology.

BTEX detection with composites of ethylenevinyl acetate and nanostructured carbon

  • Santa Stepina,
  • Astrida Berzina,
  • Gita Sakale and
  • Maris Knite

Beilstein J. Nanotechnol. 2017, 8, 982–988, doi:10.3762/bjnano.8.100

Graphical Abstract
  • measurement depends on the polarity of the polymer and is different for polar and non-polar solvents. Sensors for VOC and various gases have been widely researched around the world [10][11][12][13][14][15][16][17][18]. Mondal et al. [19] in their study about VOC sensing materials used hybrid composites. The
  • chosen because of its dual polarity. EVA has a polar part (vinyl acetate) and a non-polar part (ethylene). This allows one to detect polar as well as non-polar VOC vapours. Carbon nanoparticles (CB; PRINTEX XE-2) with average particle size of 30 nm were used as electroconductive filler. The composite EVA
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Published 04 May 2017

Recombinant DNA technology and click chemistry: a powerful combination for generating a hybrid elastin-like-statherin hydrogel to control calcium phosphate mineralization

  • Mohamed Hamed Misbah,
  • Mercedes Santos,
  • Luis Quintanilla,
  • Christina Günter,
  • Matilde Alonso,
  • Andreas Taubert and
  • José Carlos Rodríguez-Cabello

Beilstein J. Nanotechnol. 2017, 8, 772–783, doi:10.3762/bjnano.8.80

Graphical Abstract
  • polymers in a random coil conformation, whereas above Tt, the ELR chains self-assemble into β-turns, which are organized into a fibrillar morphology [27][30]. Changes to the guest residue X modulate Tt, with the key influence being the polarity of the amino acid side-chain in X. As such, ELRs can be
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Published 04 Apr 2017

Multimodal cantilevers with novel piezoelectric layer topology for sensitivity enhancement

  • Steven Ian Moore,
  • Michael G. Ruppert and
  • Yuen Kuan Yong

Beilstein J. Nanotechnol. 2017, 8, 358–371, doi:10.3762/bjnano.8.38

Graphical Abstract
  • polarity of the transducers response for a given mode shape. Using this result, the piezoelectric layer is split into isolated regions whose individual responses constructively combine in order to maximize the actuator gain/sensor output. The remainder of the paper is organized as follows. Section ’Modal
  • as an optimization problem. For the i-th finite element in the cantilever mesh, the associated Be is denoted The piezoelectric material on each finite element is observed in either a positive polarity or negative polarity. A design parameter is introduced indicating this polarity. If χi = 1 the
  • polarity to constructively combine the two responses. For displacement measurement, a vibrometer (Polytec MSA-400) is used to detect the motion of the cantilever. The actuator gains (Vi→d) are measured in two locations which are shown in Figure 2m. Measurements are made at location 1 for flexural modes M1
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Published 06 Feb 2017

Tailoring bifunctional hybrid organic–inorganic nanoadsorbents by the choice of functional layer composition probed by adsorption of Cu2+ ions

  • Veronika V. Tomina,
  • Inna V. Melnyk,
  • Yuriy L. Zub,
  • Aivaras Kareiva,
  • Miroslava Vaclavikova,
  • Gulaim A. Seisenbaeva and
  • Vadim G. Kessler

Beilstein J. Nanotechnol. 2017, 8, 334–347, doi:10.3762/bjnano.8.36

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  • structure and especially different polarity. The molecules of n-hexane are capable of adsorption interactions due to dispersion forces, whereas interaction of acetonitrile with the surface is dominated by the basic properties of the nitrogen atom. Obviously, acetonitrile (as well as n-hexane) interacts with
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Published 02 Feb 2017

Nanoscale isoindigo-carriers: self-assembly and tunable properties

  • Tatiana N. Pashirova,
  • Andrei V. Bogdanov,
  • Lenar I. Musin,
  • Julia K. Voronina,
  • Irek R. Nizameev,
  • Marsil K. Kadirov,
  • Vladimir F. Mironov,
  • Lucia Ya. Zakharova,
  • Shamil K. Latypov and
  • Oleg G. Sinyashin

Beilstein J. Nanotechnol. 2017, 8, 313–324, doi:10.3762/bjnano.8.34

Graphical Abstract
  • ). The change in pyrene fluorescence intensity is likely due to the decrease in the polarity of the pyrene microenvironment. Based on these spectra, the CAC of amphiphilic compounds was calculated from the I1/I3 values in the pyrene fluorescence spectrum as a function of the concentration of amphiphilic
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Published 01 Feb 2017

Functionalized TiO2 nanoparticles by single-step hydrothermal synthesis: the role of the silane coupling agents

  • Antoine R. M. Dalod,
  • Lars Henriksen,
  • Tor Grande and
  • Mari-Ann Einarsrud

Beilstein J. Nanotechnol. 2017, 8, 304–312, doi:10.3762/bjnano.8.33

Graphical Abstract
  • functionalization agent (DTES). Ahmad et al. [33] reported that different crystallographic faces of anatase exhibit different polarity and Kassir et al. [18] demonstrated that aminosilanes do not react homogeneously on the different faces of TiO2 nanoparticles. Thus, we propose that as the nanoparticles growth and
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Published 31 Jan 2017

Template-controlled piezoactivity of ZnO thin films grown via a bioinspired approach

  • Nina J. Blumenstein,
  • Fabian Streb,
  • Stefan Walheim,
  • Thomas Schimmel,
  • Zaklina Burghard and
  • Joachim Bill

Beilstein J. Nanotechnol. 2017, 8, 296–303, doi:10.3762/bjnano.8.32

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  • depends on the conformation of the polyion molecules and the roughness increases with every polyion layer. WCA measurements on the PEL give a value of 29°, which is lower than the WCA of the COOH-SAM (35°). This can be attributed to a difference in polarity of the two templates. Shyue et al. measured the
  • ions as can be seen from the pKa values reported by Rived et al. [43]. Therefore, it is probable that the surface charge of the used templates is lower in methanol than it could be expected from zeta potential measurements in water. Nevertheless, the polarity of the two templates is high enough to
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Published 30 Jan 2017

Colorimetric gas detection by the varying thickness of a thin film of ultrasmall PTSA-coated TiO2 nanoparticles on a Si substrate

  • Urmas Joost,
  • Andris Šutka,
  • Meeri Visnapuu,
  • Aile Tamm,
  • Meeri Lembinen,
  • Mikk Antsov,
  • Kathriin Utt,
  • Krisjanis Smits,
  • Ergo Nõmmiste and
  • Vambola Kisand

Beilstein J. Nanotechnol. 2017, 8, 229–236, doi:10.3762/bjnano.8.25

Graphical Abstract
  • 2p photoemission line in the overview spectrum (168.2 eV, Figure 3c) is consistent with the sulfonic acid group [30]. This demonstrates that the nanoparticles are covered with PTSA molecules, yielding specific surface properties such as polarity and affinity towards the specific compounds. The vapor
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Published 24 Jan 2017

Structural and tribometric characterization of biomimetically inspired synthetic "insect adhesives"

  • Matthias W. Speidel,
  • Malte Kleemeier,
  • Andreas Hartwig,
  • Klaus Rischka,
  • Angelika Ellermann,
  • Rolf Daniels and
  • Oliver Betz

Beilstein J. Nanotechnol. 2017, 8, 45–63, doi:10.3762/bjnano.8.6

Graphical Abstract
  • increased flexibility towards substrates of different surface energy and polarity, (ii) their possible non-Newtonian viscosity shifts implying adjustable viscosities [24][25] and (iii) the formation of lipoid shields that prevent the aqueous fraction of an adhesive from desiccation and its sticking to the
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Published 06 Jan 2017

Monolayer graphene/SiC Schottky barrier diodes with improved barrier height uniformity as a sensing platform for the detection of heavy metals

  • Ivan Shtepliuk,
  • Jens Eriksson,
  • Volodymyr Khranovskyy,
  • Tihomir Iakimov,
  • Anita Lloyd Spetz and
  • Rositsa Yakimova

Beilstein J. Nanotechnol. 2016, 7, 1800–1814, doi:10.3762/bjnano.7.173

Graphical Abstract
  • ideality parameter for graphene/SiC structures are the homogeneity of the graphene thickness, the quality of the grown interface (defects, pits, dislocations, surface roughness), the type of the grown interface (SiC polytypism, face polarity) and the growth conditions. Indeed, we noticed that the Schottky
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Published 22 Nov 2016

Properties of Ni and Ni–Fe nanowires electrochemically deposited into a porous alumina template

  • Alla I. Vorobjova,
  • Dmitry L. Shimanovich,
  • Kazimir I. Yanushkevich,
  • Sergej L. Prischepa and
  • Elena A. Outkina

Beilstein J. Nanotechnol. 2016, 7, 1709–1717, doi:10.3762/bjnano.7.163

Graphical Abstract
  • high aspect ratio) [19]. During deposition in the alternating current mode (ac-deposition) [2][19][20] and pulsed electro-deposition with pauses between the opposite polarity pulses [21][22][23] etching of the pore walls during the cathodic polarity stage and during pauses occurs. It changes and
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Published 14 Nov 2016

Analysis of self-heating of thermally assisted spin-transfer torque magnetic random access memory

  • Austin Deschenes,
  • Sadid Muneer,
  • Mustafa Akbulut,
  • Ali Gokirmak and
  • Helena Silva

Beilstein J. Nanotechnol. 2016, 7, 1676–1683, doi:10.3762/bjnano.7.160

Graphical Abstract
  • tunneling junction. We compare self-heating for different common passivation materials, positive and negative electrical current polarity, and different device thermal anchoring and boundaries resistance configurations. The variations considered are found to result in significant differences in maximum
  • temperatures reached. Average increases of 3 K, 10 K, and 100 K for different passivation materials, positive and negative polarity, and different thermal anchoring configurations, respectively, are observed. The highest temperatures, up to 424 K, are obtained for silicon dioxide as the passivation material
  • , positive polarity, and low thermal anchoring with thermal boundary resistance configurations. Interestingly it is also found that due to the tunneling heat, Peltier effect, device geometry, and numerous interfacial layers around the magnetic tunnel junction (MTJ), most of the heat is dissipated on the
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Published 11 Nov 2016

Photothermal effect of gold nanostar patterns inkjet-printed on coated paper substrates with different permeability

  • Mykola Borzenkov,
  • Anni Määttänen,
  • Petri Ihalainen,
  • Maddalena Collini,
  • Elisa Cabrini,
  • Giacomo Dacarro,
  • Piersandro Pallavicini and
  • Giuseppe Chirico

Beilstein J. Nanotechnol. 2016, 7, 1480–1485, doi:10.3762/bjnano.7.140

Graphical Abstract
  • commonly employed material that combines low-cost and excellent environmental compatibility [20]. Furthermore, the physical and chemical properties of this superb printing substrate (e.g., topography, roughness, stiffness, surface energy, polarity, porosity and pore geometry) can be easily tailored by
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Published 19 Oct 2016

Influence of ambient humidity on the attachment ability of ladybird beetles (Coccinella septempunctata)

  • Lars Heepe,
  • Jonas O. Wolff and
  • Stanislav N. Gorb

Beilstein J. Nanotechnol. 2016, 7, 1322–1329, doi:10.3762/bjnano.7.123

Graphical Abstract
  • by ambient humidity [16][17]. Due to its polarity it can work as a bonding agent between two surfaces, and therefore have a substantial effect on adhesion [18][19][20][21]. In insects the terminal contact elements of tenent setae are not dry, but rather wetted by a fluid secretion that is usually a
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Published 22 Sep 2016

Tunable longitudinal modes in extended silver nanoparticle assemblies

  • Serene S. Bayram,
  • Klas Lindfors and
  • Amy Szuchmacher Blum

Beilstein J. Nanotechnol. 2016, 7, 1219–1228, doi:10.3762/bjnano.7.113

Graphical Abstract
  • File 1). Different pH values were used to test how H-bonding modulates the self-assembly and contributes to the stability of the assemblies. Protonating H-bonding moieties should reduce the ligand polarity and hence prevent nanoparticle assembly. Figure 5A clearly demonstrates this for AgNPs–cysteamine
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Published 26 Aug 2016

High antiviral effect of TiO2·PL–DNA nanocomposites targeted to conservative regions of (−)RNA and (+)RNA of influenza A virus in cell culture

  • Asya S. Levina,
  • Marina N. Repkova,
  • Elena V. Bessudnova,
  • Ekaterina I. Filippova,
  • Natalia A. Mazurkova and
  • Valentina F. Zarytova

Beilstein J. Nanotechnol. 2016, 7, 1166–1173, doi:10.3762/bjnano.7.108

Graphical Abstract
  • -based drugs to affect IAV replication may contribute to the creation of therapeutic preparations, the activity of which would be less dependent on mutations. The IAV genome contains eight single-stranded RNA segments of negative polarity and belongs to the Ortomyxoviridae family. All eight segments are
  • fragments with phosphodiester internucleotide bonds can be used without any additional modification. We investigated the antiviral action of eight nanocomposites of this type bearing DNA fragments complementary to eight conservative regions of RNA segment 5 of negative and positive polarity (Figure 1, Table
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Published 10 Aug 2016

Reorientation of single-wall carbon nanotubes in negative anisotropy liquid crystals by an electric field

  • Amanda García-García,
  • Ricardo Vergaz,
  • José F. Algorri,
  • Gianluigi Zito,
  • Teresa Cacace,
  • Antigone Marino,
  • José M. Otón and
  • Morten A. Geday

Beilstein J. Nanotechnol. 2016, 7, 825–833, doi:10.3762/bjnano.7.74

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  • according to the driving voltage under study. The LC reorientation is minimally affected by polarity changes by the use of a square signal. The low amplitude AC impedance probe signal (0.1Vrms) is added. The details about the results sampling have been described in [15]. The Raman measurements are made
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Published 08 Jun 2016

Rigid multipodal platforms for metal surfaces

  • Michal Valášek,
  • Marcin Lindner and
  • Marcel Mayor

Beilstein J. Nanotechnol. 2016, 7, 374–405, doi:10.3762/bjnano.7.34

Graphical Abstract
  • tunneling. Electroluminescence from the excited molecules is a strongly unipolar process and depends on the polarity of the applied bias as revealed by STML spectra, which displayed electroluminescence exclusively at positive bias polarity (ca. 1.9 V). They attributed this unipolar behavior to both, the
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Published 08 Mar 2016

Chemical bath deposition of textured and compact zinc oxide thin films on vinyl-terminated polystyrene brushes

  • Nina J. Blumenstein,
  • Caroline G. Hofmeister,
  • Peter Lindemann,
  • Cheng Huang,
  • Johannes Baier,
  • Andreas Leineweber,
  • Stefan Walheim,
  • Christof Wöll,
  • Thomas Schimmel and
  • Joachim Bill

Beilstein J. Nanotechnol. 2016, 7, 102–110, doi:10.3762/bjnano.7.12

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  • the molecules. Since we measured a thickness of 1–2 nm for our PS films, we can calculate a nominal grafting density of 20–40% (0.164–0.329 molecules per nm2) for our brush system. The polarity of the different surfaces was investigated by ζ-potential and contact angle measurements. The isoelectric
  • spectra (see Supporting Information File 1) show a decrease in intensity for the aromatic bands after the modification reaction, confirming the ATR results. Here it also seems that the transesterification process is incomplete and a PS Brush with modified properties (increased polarity and charge) is the
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Published 25 Jan 2016

Blue and white light emission from zinc oxide nanoforests

  • Nafisa Noor,
  • Luca Lucera,
  • Thomas Capuano,
  • Venkata Manthina,
  • Alexander G. Agrios,
  • Helena Silva and
  • Ali Gokirmak

Beilstein J. Nanotechnol. 2015, 6, 2463–2469, doi:10.3762/bjnano.6.255

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  • during DC tests with an approximate probe distance of 10–15 μm. The probe locations and applied voltage polarity are as indicated in yellow (multimedia view). Frames extracted from high-resolution videos showing light emission from the ZnO nanorods contacted by tungsten probes during AC excitation of 10
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Published 23 Dec 2015

Nanofibers for drug delivery – incorporation and release of model molecules, influence of molecular weight and polymer structure

  • Jakub Hrib,
  • Jakub Sirc,
  • Radka Hobzova,
  • Zuzana Hampejsova,
  • Zuzana Bosakova,
  • Marcela Munzarova and
  • Jiri Michalek

Beilstein J. Nanotechnol. 2015, 6, 1939–1945, doi:10.3762/bjnano.6.198

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  • PVA with water molecules during immersion – the PVA molecular structure contains hydroxy groups, which interact with water molecules at the expense of the interaction with PEG molecules, which are consequently released faster. The lower polarity of PCL and PLA and therefore weaker interaction with
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Published 25 Sep 2015

Predicting cytotoxicity of PAMAM dendrimers using molecular descriptors

  • David E. Jones,
  • Hamidreza Ghandehari and
  • Julio C. Facelli

Beilstein J. Nanotechnol. 2015, 6, 1886–1896, doi:10.3762/bjnano.6.192

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  • polarizability, rotatable bond count, atom count, logD, aliphatic bond count, chain bond count, chain atom count, aliphatic atom count, exact mass, molecular weight, Wiener index, Randic index, Szeged index, Wiener polarity, Platt index, H-bond donor count, hyper Wiener index, H-bond donor sites, and H-bond
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Published 11 Sep 2015

Template-controlled mineralization: Determining film granularity and structure by surface functionality patterns

  • Nina J. Blumenstein,
  • Jonathan Berson,
  • Stefan Walheim,
  • Petia Atanasova,
  • Johannes Baier,
  • Joachim Bill and
  • Thomas Schimmel

Beilstein J. Nanotechnol. 2015, 6, 1763–1768, doi:10.3762/bjnano.6.180

Graphical Abstract
  • controlling the properties of a self-assembling mineral film by means of the functionality and polarity of a substrate template. In the presented case, a zinc oxide film is deposited by chemical bath deposition on a nearly topography-free template structure composed of a pattern of two self-assembled
  • topographically flat (<1 nm roughness), but chemically patterned surface as a template, it was possible to guide the deposition – mainly by means of surface polarity. While deposition took place at sites with amino functionalization, no deposition was observed at locations with a fluorinated surface functionality
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Published 20 Aug 2015

Peptide-equipped tobacco mosaic virus templates for selective and controllable biomineral deposition

  • Klara Altintoprak,
  • Axel Seidenstücker,
  • Alexander Welle,
  • Sabine Eiben,
  • Petia Atanasova,
  • Nina Stitz,
  • Alfred Plettl,
  • Joachim Bill,
  • Hartmut Gliemann,
  • Holger Jeske,
  • Dirk Rothenstein,
  • Fania Geiger and
  • Christina Wege

Beilstein J. Nanotechnol. 2015, 6, 1399–1412, doi:10.3762/bjnano.6.145

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  • ). Analyzing SiOH+ and several fragments characteristic of silica in negative polarity spectra (SiO2−, SiO3−, SiO3H−) indicated the same trend. Since the sample preparation method did not yield fully TMV-covered samples, the recorded mass spectra averaged over a field of view of 500 × 500 µm2 show individual
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Published 25 Jun 2015

Closed-loop conductance scanning tunneling spectroscopy: demonstrating the equivalence to the open-loop alternative

  • Chris Hellenthal,
  • Kai Sotthewes,
  • Martin H. Siekman,
  • E. Stefan Kooij and
  • Harold J. W. Zandvliet

Beilstein J. Nanotechnol. 2015, 6, 1116–1124, doi:10.3762/bjnano.6.113

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  • voltage between the tip and sample causes the barrier to lower in an asymmetrical fashion: Any charge travelling between the tip and the sample will induce an image charge of equal magnitude but opposite polarity. In addition to lowering the barrier, the presence of an image charge effect will also narrow
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Published 06 May 2015
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