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Search for "cross-section" in Full Text gives 506 result(s) in Beilstein Journal of Nanotechnology. Showing first 200.

CuInSe2 quantum dots grown by molecular beam epitaxy on amorphous SiO2 surfaces

  • Henrique Limborço,
  • Pedro M.P. Salomé,
  • Rodrigo Ribeiro-Andrade,
  • Jennifer P. Teixeira,
  • Nicoleta Nicoara,
  • Kamal Abderrafi,
  • Joaquim P. Leitão,
  • Juan C. Gonzalez and
  • Sascha Sadewasser

Beilstein J. Nanotechnol. 2019, 10, 1103–1111, doi:10.3762/bjnano.10.110

Graphical Abstract
  • the 530 °C sample. Figure 2a shows a high-resolution cross-section high-angle annular dark-field (HAADF) image of a nanodot. Due to the large density of nanodots in the sample, a superposition of two other nanodots can be observed on the back (left and right sides of the image) of the nanodot under
  • amorphous layer as evidenced by the STEM analysis. Energy-dispersive X-ray spectroscopy (EDS) mapping was carried out in the 530 °C sample in order to determine the chemical composition of the nanodots. Figure 3a–f, shows a low-resolution cross-section HAADF image of the sample, as well as the EDS chemical
  • ) and Si substrate (red). Chemical analysis of the sample grown at 530 °C. (a) Low-resolution cross-section STEM HAADF image of a region of the 530 °C sample studied by EDS. (b–f) EDS mapping of Se, Cu, In, Si, and O. (g) EDS line profile across a nanodot (blue rectangle in (a)). (h) EDS line profile
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Published 22 May 2019

Influence of dielectric layer thickness and roughness on topographic effects in magnetic force microscopy

  • Alexander Krivcov,
  • Jasmin Ehrler,
  • Marc Fuhrmann,
  • Tanja Junkers and
  • Hildegard Möbius

Beilstein J. Nanotechnol. 2019, 10, 1056–1064, doi:10.3762/bjnano.10.106

Graphical Abstract
  • . The position of the tip dipole is assumed to be at the half radius of the tip [17]. Cross section simulation of MFM phase The first scan of MFM measurements provides a topographic image displaying a convolution of the tip and the nanoparticle [24]. The topographic cross section is simulated by using a
  • be calculated as a function of the horizontal position of the tip corresponding to a cross section of the MFM image. The vertical distance changes in the second scan (interleave scan with a certain lift height following the topography of the first scan) lead to a positive phase shift due to
  • observed directly above the nanoparticles indicating a remaining weak capacitive coupling. Figure 10 shows a cross section of the topography image as well as of the phase image for a single SPION on a silicon substrate. For the single SPION lying directly on the silicon surface a strong repulsion indicated
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Published 17 May 2019
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  • scattering (SERS), the Raman scattering cross-section of molecules adsorbed on the surface of plasmonic nanostructures is enormously increased compared to the same isolated molecules [1][2][3][4][5]. In particular, the SERS enhancement factor can reach values as high as 1012, which can be attributed to two
  • deviation of the counts per second from a single AuNT in the experimental conditions used (reported in Figure 3B), which is indicative of the average Raman scattering cross-section for a single label. The signal from all of the three label types exceeds the noise level for 1 s of acquisition, meaning that
  • phenomena, the local electric field enhancement due to the surface plasmon resonance of the metal nanostructure (electromagnetic enhancement) and the charge transfer between the molecule and the metal substrate (chemical enhancement) [6][7][8]. In addition, given the generally low Raman scattering cross
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Published 10 May 2019

Direct growth of few-layer graphene on AlN-based resonators for high-sensitivity gravimetric biosensors

  • Jimena Olivares,
  • Teona Mirea,
  • Lorena Gordillo-Dagallier,
  • Bruno Marco,
  • José Miguel Escolano,
  • Marta Clement and
  • Enrique Iborra

Beilstein J. Nanotechnol. 2019, 10, 975–984, doi:10.3762/bjnano.10.98

Graphical Abstract
  • antibody detection process. The arrows indicate the moments at what the liquids are changed. Resonant frequency evolution of a resonator during the non-covalent functionalization with anti-IgG antibody. The arrows indicate the moments at what the liquids are changed. a) Schematic cross section of a typical
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Published 29 Apr 2019

Nanoscale optical and structural characterisation of silk

  • Meguya Ryu,
  • Reo Honda,
  • Adrian Cernescu,
  • Arturas Vailionis,
  • Armandas Balčytis,
  • Jitraporn Vongsvivut,
  • Jing-Liang Li,
  • Denver P. Linklater,
  • Elena P. Ivanova,
  • Vygantas Mizeikis,
  • Mark J. Tobin,
  • Junko Morikawa and
  • Saulius Juodkazis

Beilstein J. Nanotechnol. 2019, 10, 922–929, doi:10.3762/bjnano.10.93

Graphical Abstract
  • features [10]. Whilst the first two modalities probe micrometer-sized volumes of silk, the AFM-based nano-IR technique acquires structural information at the nanoscale (i.e., the area under the AFM tip from a volume with a lateral cross section of ca. 20 nm). Differences in absorbance and spectral line
  • ]. The most pronounced peak corresponds to the separation between the equatorial (200) planes d(200) = 4.69 nm and crystal cross section of L ≈ 2.15 nm, while for the meridional (002) planes d(002) = 3.46 nm and crystal size of L ≈ 10.76 nm [18]. These are the dimensions of the β-sheets, which are
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Published 23 Apr 2019

Trapping polysulfide on two-dimensional molybdenum disulfide for Li–S batteries through phase selection with optimized binding

  • Sha Dong,
  • Xiaoli Sun and
  • Zhiguo Wang

Beilstein J. Nanotechnol. 2019, 10, 774–780, doi:10.3762/bjnano.10.77

Graphical Abstract
  • × 1 k-grid for the geometry optimization. All atomic positions and cell parameters were relaxed until the force on each atom is less than 0.02 eV/Å. Cross-section and side views of (a) 2H-MoS2 and (b) 1T'-MoS2 monolayers. Orbital-decomposed band structures along high-symmetry points of (c) 2H-MoS2 and
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Published 26 Mar 2019

Renewable energy conversion using nano- and microstructured materials

  • Harry Mönig and
  • Martina Schmid

Beilstein J. Nanotechnol. 2019, 10, 771–773, doi:10.3762/bjnano.10.76

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  • together with the related scientific discussions. In this sense, the present thematic issue provides a platform for a contemporary cross-section of topics in this broad field of research. The Beilstein Journal of Nanotechnology is a unique medium for scientific exchange across the traditional disciplines
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Published 26 Mar 2019

Features and advantages of flexible silicon nanowires for SERS applications

  • Hrvoje Gebavi,
  • Vlatko Gašparić,
  • Dubravko Risović,
  • Nikola Baran,
  • Paweł Henryk Albrycht and
  • Mile Ivanda

Beilstein J. Nanotechnol. 2019, 10, 725–734, doi:10.3762/bjnano.10.72

Graphical Abstract
  • , preferably with clusters of metal nanoparticles, sharp edges and tips, are the key to strong electromagnetic enhancement ranging from 1010 to 1014 [3]. If the values of Raman cross section of the analyte and of SERS enhancement are appropriate, even single-molecule detection is possible. For example, under
  • resonant laser excitation of analyte molecules with differential cross section of ca. 10−27 cm2/sr, a SERS enhancement factor (EF) of 108 would be adequate for single-molecule detection. Under non-resonant conditions and/or for lower cross sections (ca. 10−30 cm2/sr ) EF values above 1011 are required [4
  • -sensitive and has a relatively large Raman cross section (ca. 10−29 cm2/sr [28]). The boronic acid group binds to certain analytes, for example, peptidoglycans in bacterial cell walls [29]. Recently, the difficult detection of saccharides (glucose, fructose) due to a low Raman scattering cross-section and a
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Published 15 Mar 2019

Biomimetic synthesis of Ag-coated glasswing butterfly arrays as ultra-sensitive SERS substrates for efficient trace detection of pesticides

  • Guochao Shi,
  • Mingli Wang,
  • Yanying Zhu,
  • Yuhong Wang,
  • Xiaoya Yan,
  • Xin Sun,
  • Haijun Xu and
  • Wanli Ma

Beilstein J. Nanotechnol. 2019, 10, 578–588, doi:10.3762/bjnano.10.59

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  • a dynamic electron transfer between probe molecules and nanostructures. In contact with the nanostructures, the adsorbed molecules exhibit a larger scattering cross section, thus enhancing the Raman signal intensity efficiently [5]. However, CE only contributes to the enhancement factor (EF) up to
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Published 28 Feb 2019

Choosing a substrate for the ion irradiation of two-dimensional materials

  • Egor A. Kolesov

Beilstein J. Nanotechnol. 2019, 10, 531–539, doi:10.3762/bjnano.10.54

Graphical Abstract
  • contribution of this mechanism to the total stopping cross section. At large incident ion energies, more than 99% of the ion energy loss can be attributed to the electronic stopping. As its role increases with the ion energy, massive atom ionization occurs, leading to the generation of hot electrons in the
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Published 22 Feb 2019

Mechanical and thermodynamic properties of Aβ42, Aβ40, and α-synuclein fibrils: a coarse-grained method to complement experimental studies

  • Adolfo B. Poma,
  • Horacio V. Guzman,
  • Mai Suan Li and
  • Panagiotis E. Theodorakis

Beilstein J. Nanotechnol. 2019, 10, 500–513, doi:10.3762/bjnano.10.51

Graphical Abstract
  • temperature. Results and Discussion Tensile deformation Our results for tensile deformation for all studied cases are illustrated in Figure 4. The initial length (L0) is measured after an equilibration of 100 τ. The cross-section area (A) for each system is monitored during the simulation and is shown as a
  • function of the strain in the insets of Figure 4. The deviations are small compared to the mean value, especially in the case of β-amyloid fibrils. Hence, we calculated the stress using the average value of A. The values of the cross-section areas and the initial length for each fibril are listed in Table
  • contrast, the interchain contacts, which keep together Aβ chains in the cross-section area, reduce their length. Moreover, in the case of α-syn there are no interchain contacts given that there is only one chain at the cross-section. In this case, only the intrachain contacts stretch during tensile
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Published 19 Feb 2019

Biological and biomimetic surfaces: adhesion, friction and wetting phenomena

  • Stanislav N. Gorb,
  • Kerstin Koch and
  • Lars Heepe

Beilstein J. Nanotechnol. 2019, 10, 481–482, doi:10.3762/bjnano.10.48

Graphical Abstract
  • cross section of recent developments in this highly diverse and interdisciplinary field of research. The articles highlight recent achievements in the understanding of animal and plant surfaces in the broadest context of adhesion, friction, and wetting phenomena on one hand. On the other hand, they
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Published 15 Feb 2019

Wearable, stable, highly sensitive hydrogel–graphene strain sensors

  • Jian Lv,
  • Chuncai Kong,
  • Chao Yang,
  • Lu Yin,
  • Itthipon Jeerapan,
  • Fangzhao Pu,
  • Xiaojing Zhang,
  • Sen Yang and
  • Zhimao Yang

Beilstein J. Nanotechnol. 2019, 10, 475–480, doi:10.3762/bjnano.10.47

Graphical Abstract
  • when the layer is stretched, which will enhance the resistance change of the hydrogel under strain. The SEM image of the cross section of the graphene/hydrogel composite is shown in Supporting Information File 1, Figure S2. A great contact between the graphene layer and the hydrogel layer can be seen
  • showing the real life application of the strain sensor to sense the movement of the proximal interphalangeal joint (c) and the metacarpophalangeal joint (d). Supporting Information Yield strain stress curve of the hydrogels; Cross-section SEM image of the graphene/hydrogel composite; Hysteresis curve for
  • the graphene/WG-hydrogel strain sensor; Optical cross-section images of the graphene/WG-hydrogel composite before and after stretching. Supporting Information File 54: Additional figures. Acknowledgements This work was supported by the National Natural Science Foundation of China (NSFC No.51501140
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Published 14 Feb 2019

Improving control of carbide-derived carbon microstructure by immobilization of a transition-metal catalyst within the shell of carbide/carbon core–shell structures

  • Teguh Ariyanto,
  • Jan Glaesel,
  • Andreas Kern,
  • Gui-Rong Zhang and
  • Bastian J. M. Etzold

Beilstein J. Nanotechnol. 2019, 10, 419–427, doi:10.3762/bjnano.10.41

Graphical Abstract
  • 5 s per step. The XRD diffractograms were deconvoluted to evaluate the properties of graphitic reflexes (see exemplary deconvolution in Figure 7). The graphite dimension (La of the in-plane and Lc of the cross section size) was evaluated by the Scherrer equation shown in Equation 2 [34]. where λ is
  • crystallite dimension for the in-plane (La) and cross section of multi-layer carbons (Lc) of final CDCs. (a) Temperature-programmed oxidation profile of final CDC; (b) the calculated fraction of Area II representing content of more graphitic carbon. TEM images of CDC-Ni0 (a) and CDC-Ni60 (b,c). (a) N2
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Published 11 Feb 2019

Integration of LaMnO3+δ films on platinized silicon substrates for resistive switching applications by PI-MOCVD

  • Raquel Rodriguez-Lamas,
  • Dolors Pla,
  • Odette Chaix-Pluchery,
  • Benjamin Meunier,
  • Fabrice Wilhelm,
  • Andrei Rogalev,
  • Laetitia Rapenne,
  • Xavier Mescot,
  • Quentin Rafhay,
  • Hervé Roussel,
  • Michel Boudard,
  • Carmen Jiménez and
  • Mónica Burriel

Beilstein J. Nanotechnol. 2019, 10, 389–398, doi:10.3762/bjnano.10.38

Graphical Abstract
  • ). Structural and electrical characterization Scanning electron microscopy (SEM) was performed in a Quanta250 environmental SEM FEG from FEI, and SEM FEG ZEISS GeminiSEM 500 to study the surface morphology and determine the LMO thickness using the cross section of the films. The cationic film composition was
  • nanostructure growth was further analyzed in cross section by transmission electron microscopy (TEM), a JEOL 2011 equipment operating at 200 kV with a 0.19 nm point-to-point resolution. X-ray absorption near-edge spectroscopy (XANES) spectra at the Mn K-edge of LMO thin films were collected at the ESRF ID12
  • substrate surface. The main issues were Pt dewetting, the formation of pinholes at the LMO film, and/or LMO film cracking due to Pt grain evolution. The surface and the cross section of the heterostructures showing cracking of the sample, holes and Pt percolating to the surface are presented in Figure S1
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Published 07 Feb 2019

Geometrical optimisation of core–shell nanowire arrays for enhanced absorption in thin crystalline silicon heterojunction solar cells

  • Robin Vismara,
  • Olindo Isabella,
  • Andrea Ingenito,
  • Fai Tong Si and
  • Miro Zeman

Beilstein J. Nanotechnol. 2019, 10, 322–331, doi:10.3762/bjnano.10.31

Graphical Abstract
  • dependence of absorption on the nanowire cross section, a weaker effect of the nanowire height and good resilience for angles of incidence of light up to 60°. Conclusion: The presence of a nanowire array increases the optical performance of ultra-thin crystalline silicon solar cells in a wide range of
  • = 800 nm, the height is h = 2 μm and the cross section is d = 200 nm. A depiction of one unit cell of the device model is presented in Figure 3. Appropriately defined periodic boundary conditions ensure the creation of a complete solar cell endowed with an hexagonal nanowire array. The crystalline
  • absorber of the NW device () is significantly higher then the value computed for the FLAT reference (), but can be further increased by careful optimisation of the nanowire geometry. To this purpose, the height (h) and cross section (d) of the nanowires were varied in the ranges of 0–5 μm and 0–700 nm
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Published 31 Jan 2019

Electromagnetic analysis of the lasing thresholds of hybrid plasmon modes of a silver tube nanolaser with active core and active shell

  • Denys M. Natarov,
  • Trevor M. Benson and
  • Alexander I. Nosich

Beilstein J. Nanotechnol. 2019, 10, 294–304, doi:10.3762/bjnano.10.28

Graphical Abstract
  • they are apparently not interesting for applications. We believe that the new results presented will help in the design of nanotube lasers, which are essentially single-mode sources. Cross section of a nanolaser built on a silver nanotube with an active core and an active shell. Relief of the function
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Published 28 Jan 2019

A Ni(OH)2 nanopetals network for high-performance supercapacitors synthesized by immersing Ni nanofoam in water

  • Donghui Zheng,
  • Man Li,
  • Yongyan Li,
  • Chunling Qin,
  • Yichao Wang and
  • Zhifeng Wang

Beilstein J. Nanotechnol. 2019, 10, 281–293, doi:10.3762/bjnano.10.27

Graphical Abstract
  • synthesis of Ni(OH)2 nanopetals. It is worth noting that the sandwich-like Ni(OH)2/Ni-NF/MG composite electrode exhibits excellent flexibility. This can be explained by the fact that the Ni-NF/MG substrate was obtained by dealloying ductile Ni40Zr20Ti40 MG. The cross section (Figure 3a) shows that the Ni-NF
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Published 25 Jan 2019

Relation between thickness, crystallite size and magnetoresistance of nanostructured La1−xSrxMnyO3±δ films for magnetic field sensors

  • Rasuole Lukose,
  • Valentina Plausinaitiene,
  • Milita Vagner,
  • Nerija Zurauskiene,
  • Skirmantas Kersulis,
  • Virgaudas Kubilius,
  • Karolis Motiejuitis,
  • Birute Knasiene,
  • Voitech Stankevic,
  • Zita Saltyte,
  • Martynas Skapas,
  • Algirdas Selskis and
  • Evaldas Naujalis

Beilstein J. Nanotechnol. 2019, 10, 256–261, doi:10.3762/bjnano.10.24

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  • SU70). The structural analysis was performed in cross section geometry by TEM (FEI Tecnai G2 F20 X-TWIN). The elemental composition analysis was performed by inductively coupled plasma high-resolution mass spectrometry (ICP-MS) - Thermo Scientific Element2, where the films were totally dissolved in 2
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Published 23 Jan 2019

Nanoporous water oxidation electrodes with a low loading of laser-deposited Ru/C exhibit enhanced corrosion stability

  • Sandra Haschke,
  • Dmitrii Pankin,
  • Vladimir Mikhailovskii,
  • Maïssa K. S. Barr,
  • Adriana Both-Engel,
  • Alina Manshina and
  • Julien Bachmann

Beilstein J. Nanotechnol. 2019, 10, 157–167, doi:10.3762/bjnano.10.15

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  • Ru3(CO)12 solutions. SEM images of planar samples coated with laser-induced Ru/C films in cross-section (a) and top-view (b). Laser-irradiation of Ru3(CO)12 solutions results in continuous and rough thin films deposited on ITO. Preparation of nanostructured Ru/C electrodes. (a) Anodization of Al in 1
  • deposition areas of 2 mm diameter on an anodic alumina substrate of 16 mm diameter. (d) Sputter-coating of the ITO backside contact. Scanning electron micrographs of a nanostructured Ru/C sample after all preparation steps in top view (a) and cross-section (b). EDX spectrum recorded over the whole sample
  • length L = 24 μm (c). EDX profile taken along the cross-section (d). Laser-irradiation of Ru3(CO)12 solutions results in thin ruthenium containing coatings along the whole length of Al2O3 pores. Raman spectra of a nanostructured template coated with Ru/C films, without ITO contact (a) and of the solid
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Published 11 Jan 2019

Graphene–graphite hybrid epoxy composites with controllable workability for thermal management

  • Idan Levy,
  • Eyal Merary Wormser,
  • Maxim Varenik,
  • Matat Buzaglo,
  • Roey Nadiv and
  • Oren Regev

Beilstein J. Nanotechnol. 2019, 10, 95–104, doi:10.3762/bjnano.10.9

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  • difference in applicative TC performances caused by the different rheological behaviors of the two samples. A SEM micrograph of a cross-section of sample Y (the higher viscosity TIM, solid mixing) showed interfacial defects in the form of voids between the Cu plates and the composite (Figure 6b). These voids
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Published 08 Jan 2019

Pull-off and friction forces of micropatterned elastomers on soft substrates: the effects of pattern length scale and stiffness

  • Peter van Assenbergh,
  • Marike Fokker,
  • Julian Langowski,
  • Jan van Esch,
  • Marleen Kamperman and
  • Dimitra Dodou

Beilstein J. Nanotechnol. 2019, 10, 79–94, doi:10.3762/bjnano.10.8

Graphical Abstract
  • successfully expanded to fabricate adhesives with two geometries, namely dimples with and without a terminal layer. Dimples without a terminal layer were fabricated on two length scales, namely with sub-microscale and microscale dimple diameters. The cross section of samples with a terminal layer showed voids
  • = 100) (Figure 3, left). The depth of dimples from microscale particles could not be accurately determined from microscopic cross-section images, as it is unknown whether a dimple was sectioned through its center, where the diameter is largest. From the cross section shown at Figure 3 (left, inset), the
  • dimple depth was equal to half of the dimple diameter. The cross section of samples with a terminal layer showed voids with a spherical shape, separated by hourglass-shaped walls (Figure 3, right, inset). These voids penetrate the terminal layer, resulting in an array of holes at the surface (Figure 3
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Published 08 Jan 2019

Contact splitting in dry adhesion and friction: reducing the influence of roughness

  • Jae-Kang Kim and
  • Michael Varenberg

Beilstein J. Nanotechnol. 2019, 10, 1–8, doi:10.3762/bjnano.10.1

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  • the power of three in determination of the area moment of inertia for the flap cross-section). Assuming that flaps of 5 µm in thickness are not able to adapt to surface irregularities having a wavelength of less than 10 µm, we used this latter value as a cut-off length to filter out the waviness
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Published 02 Jan 2019

A new bioinspired method for pressure and flow sensing based on the underwater air-retaining surface of the backswimmer Notonecta

  • Matthias Mail,
  • Adrian Klein,
  • Horst Bleckmann,
  • Anke Schmitz,
  • Torsten Scherer,
  • Peter T. Rühr,
  • Goran Lovric,
  • Robin Fröhlingsdorf,
  • Stanislav N. Gorb and
  • Wilhelm Barthlott

Beilstein J. Nanotechnol. 2018, 9, 3039–3047, doi:10.3762/bjnano.9.282

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  • socket septum (ss) is attached to the tip of the dendrite where the tubular body is located. a) Three-dimensional reconstruction of a hemelytron µCT scan. The tomography data allowed an analysis of the outer and inner structures of the hemelytron. b) Digital cross section through a SR-µCT scan of a
  • hemelytron. c) Part of the cross section, where the dendritic canal below the setal base is visible, indicating an innervation of the seta. d–h) A stack of µCT-images used for tracking single seta and identifying the corresponding setal base and setal tip. Toluidine blue/borax stained semi-thin sections
  • ) Projection through a stack of images using confocal laser scanning microscopy. The picture shows the structure of the setae and the reflecting air layer in between the club-setae. d) Cross section through the image stack at the position of the blue line in (c) at ambient pressure. The shape of the air–water
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Published 14 Dec 2018

Femtosecond laser-assisted fabrication of chalcopyrite micro-concentrator photovoltaics

  • Franziska Ringleb,
  • Stefan Andree,
  • Berit Heidmann,
  • Jörn Bonse,
  • Katharina Eylers,
  • Owen Ernst,
  • Torsten Boeck,
  • Martina Schmid and
  • Jörg Krüger

Beilstein J. Nanotechnol. 2018, 9, 3025–3038, doi:10.3762/bjnano.9.281

Graphical Abstract
  • . Cross section of a CISe micro absorber island after processing to a micro cell imaged by tilted-view SEM. Note that the different materials were artificially post-colorized to enhance their visibility. The height of the CISe absorber is ca.1 µm. Electrical characterization with different light
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Published 12 Dec 2018
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