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Search for "dielectric permittivity" in Full Text gives 37 result(s) in Beilstein Journal of Nanotechnology.

Photocurrent generation in carbon nanotube/cubic-phase HfO2 nanoparticle hybrid nanocomposites

  • Protima Rauwel,
  • Augustinas Galeckas,
  • Martin Salumaa,
  • Frédérique Ducroquet and
  • Erwan Rauwel

Beilstein J. Nanotechnol. 2016, 7, 1075–1085, doi:10.3762/bjnano.7.101

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  • its more interesting properties such as higher dielectric permittivity via doping [17] and substrate-induced strain. Many systems and processes were developed to reach this goal. One advantage of studying this material for other properties is that the microelectronic industry already produces and
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Published 26 Jul 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

Graphical Abstract
  • electric field (Figure 7a) because the LC molecules do not change their position, and there is not any change of their effective dielectric permittivity. The SWCNT-doped LC cell impedance is variable according to Figure 7b. In an initial unbiased state (0 V), the electrical behavior is close to that of a
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Published 08 Jun 2016

Characterisation of thin films of graphene–surfactant composites produced through a novel semi-automated method

  • Nik J. Walch,
  • Alexei Nabok,
  • Frank Davis and
  • Séamus P. J. Higson

Beilstein J. Nanotechnol. 2016, 7, 209–219, doi:10.3762/bjnano.7.19

Graphical Abstract
  • . A. Woollam data analysis software, which is given below as a dispersion function of a complex dielectric permittivity, ε(hν): where ε1∞ is the dielectric permittivity at infinite frequency, Ek, Ak and Bk are, respectively, the position, amplitude, and half-width of the k-th Lorentzian peak. There
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Published 08 Feb 2016

High photocatalytic activity of V-doped SrTiO3 porous nanofibers produced from a combined electrospinning and thermal diffusion process

  • Panpan Jing,
  • Wei Lan,
  • Qing Su and
  • Erqing Xie

Beilstein J. Nanotechnol. 2015, 6, 1281–1286, doi:10.3762/bjnano.6.132

Graphical Abstract
  • ]. Although a promising photocatalytic candidate, the catalytic activity of SrTiO3 is still heavily influenced by its considerably large band gap of ≈3.25 eV and high dielectric permittivity [14]. The calculated band structure of SrTiO3 shows that the top of the valence band (VB) and the bottom of the
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Published 09 Jun 2015

Entropy effects in the collective dynamic behavior of alkyl monolayers tethered to Si(111)

  • Christian Godet

Beilstein J. Nanotechnol. 2015, 6, 583–594, doi:10.3762/bjnano.6.60

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  • -dependent electric field. Dissipation (energy loss) mechanisms can be described by using equivalent representations of the complex admittance, including the dielectric permittivity ε* and electrical modulus M*. Dipole reorientation requires an activation of the system with energy barriers related either to
  • insulating OML with thickness dOML and dielectric permittivity εI: This electrostatic force leads to compressive and shear stress components, respectively, normal and parallel to the substrate. Furthermore, each molecule is considered as a rigid elastic rod, tilted at some angle with respect to the normal to
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Published 26 Feb 2015

Electrical response of liquid crystal cells doped with multi-walled carbon nanotubes

  • Amanda García-García,
  • Ricardo Vergaz,
  • José F. Algorri,
  • Xabier Quintana and
  • José M. Otón

Beilstein J. Nanotechnol. 2015, 6, 396–403, doi:10.3762/bjnano.6.39

Graphical Abstract
  • conditioning of the cell walls [12] and modified by application of external electric fields above a certain voltage called Freedericksz threshold. Depending on the applied voltage, the LC dielectric permittivity along the electric field varies since the LC director adopts a specific orientation in order to
  • . Remarkable conductivity differences between CNT-doped and undoped LC cells have been reported, and studies about variations in the dielectric permittivity [14][15], threshold voltage [16] and response time [17][18] have been published. Yet a more detailed description of the electrical behavior of CNT-doped
  • above mentioned operating frequency range, from 100 Hz to 10 kHz. As Cr is proportional to the dielectric permittivity, its value is expected to vary with the applied voltage upon reorientation of the material, due to the dielectric anisotropy of LC. For MWCNT-doped LC cells, one could also expect a
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Published 06 Feb 2015

Kelvin probe force microscopy in liquid using electrochemical force microscopy

  • Liam Collins,
  • Stephen Jesse,
  • Jason I. Kilpatrick,
  • Alexander Tselev,
  • M. Baris Okatan,
  • Sergei V. Kalinin and
  • Brian J. Rodriguez

Beilstein J. Nanotechnol. 2015, 6, 201–214, doi:10.3762/bjnano.6.19

Graphical Abstract
  • be expressed as where D is the diffusivity of the ions in solution, L is the separation of the electrodes and λ is the Debye screening length, given by where k is Boltzmann’s constant, Cb is the molar concentration, ε is the dielectric permittivity of the solvent, T is the temperature, e is the
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Published 19 Jan 2015

Tunable light filtering by a Bragg mirror/heavily doped semiconducting nanocrystal composite

  • Ilka Kriegel and
  • Francesco Scotognella

Beilstein J. Nanotechnol. 2015, 6, 193–200, doi:10.3762/bjnano.6.18

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  • * the effective mass and ε0 the vacuum dielectric permittivity. The absorption of the ITO NC film has been described by applying the effective medium theory or Maxwell–Garnett effective medium approximation (MG-EMA) [40][41][42]. This theory has been developed to describe the macroscopic properties of a
  • properties [28]. The refractive index of the film is 1.5 (same as that of the glass). For the NCs we consider a free carrier damping Γ = 0.31 eV and a high frequency dielectric permittivity of ε∞ = 4 [28][29][30]. The volume fraction of ITO in the film is chosen to be 0.01 [35]. In Figure 2b the absorption
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Published 16 Jan 2015

Hole-mask colloidal nanolithography combined with tilted-angle-rotation evaporation: A versatile method for fabrication of low-cost and large-area complex plasmonic nanostructures and metamaterials

  • Jun Zhao,
  • Bettina Frank,
  • Frank Neubrech,
  • Chunjie Zhang,
  • Paul V. Braun and
  • Harald Giessen

Beilstein J. Nanotechnol. 2014, 5, 577–586, doi:10.3762/bjnano.5.68

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  • based on metallic split-ring resonators (SRRs) were able to simultaneously demonstrate negative dielectric permittivity as well as magnetic permeability, which leads to a negative refractive index [11]. In hybrid solar cells and organic light emitting diodes, plasmonic nanostructures enhanced the
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Published 06 May 2014

Dye-doped spheres with plasmonic semi-shells: Lasing modes and scattering at realistic gain levels

  • Nikita Arnold,
  • Boyang Ding,
  • Calin Hrelescu and
  • Thomas A. Klar

Beilstein J. Nanotechnol. 2013, 4, 974–987, doi:10.3762/bjnano.4.110

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  • is somewhat similar to the scattering by weakly dissipating plasmonic spheres, in which very narrow higher order resonances can dominate [52]. These effects are even more pronounced for the anisotropic dielectric permittivity with transverse or longitudinal gain [53]. Computational details are
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Published 30 Dec 2013

3D nano-structures for laser nano-manipulation

  • Gediminas Seniutinas,
  • Lorenzo Rosa,
  • Gediminas Gervinskas,
  • Etienne Brasselet and
  • Saulius Juodkazis

Beilstein J. Nanotechnol. 2013, 4, 534–541, doi:10.3762/bjnano.4.62

Graphical Abstract
  • , hence · D = 0 with D = ε0εrE = ε0E + P where P is the material polarization due to the bound charges and εr is complex if the medium is not transparent. On the other hand, we have jf = 0, jb = ∂t P, which leads to: For materials whose dielectric permittivity accounts for conduction electrons, i.e
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Published 17 Sep 2013

Single-pass Kelvin force microscopy and dC/dZ measurements in the intermittent contact: applications to polymer materials

  • Sergei Magonov and
  • John Alexander

Beilstein J. Nanotechnol. 2011, 2, 15–27, doi:10.3762/bjnano.2.2

Graphical Abstract
  • enable measurements of electrical properties (surface potential, dielectric permittivity, capacitance, etc.) at a tip–sample junction. Here we will demonstrate that single-pass Kelvin force microscopy (KFM) studies based on sensing of an electrostatic force gradient can be performed in the intermittent
  • to dC/dZ. Both the dC/dZ and d2C/dZ2 signals are related to the local dielectric permittivity and we used these for compositional mapping. The interplay between the experimental measurements and theoretical studies is needed for a better understanding of the sensitivity of dC/dZ and d2C/dZ2 based
  • contaminating particles, which are marked with the red stars, are seen in the topography and dC/dZ images but not in surface potential image. The dC/dZ contrast correlates with variations of dielectric permittivity and the latter is related to averaged dipole values. A quantification of dC/dZ and permittivity
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Published 06 Jan 2011
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