Numerical investigation of depth profiling capabilities of helium and neon ions in ion microscopy

• Patrick Philipp,
• Lukasz Rzeznik and
• Tom Wirtz

Beilstein J. Nanotechnol. 2016, 7, 1749–1760, doi:10.3762/bjnano.7.168

• damage formation. The emission of H2, CH4, C2H2, C3H5, etc. has been observed for 100 keV He+ and 200 keV Ar+ bombardment of polyethylene (PE) and polystyrene (PS) [14]. Similarly, H2, C2H2, CO and CO2 are typically emitted from implanted PI [15]. The degassing leads to an increase of the carbon

• polytetrafluoroethylene (PTFE), polystyrene (PS) or poly(methyl methacrylate) (PMMA). For samples 1 to 3, layers 1 and 5 have a thickness of 20 nm while the remaining layers have a thickness of 10 nm. For samples 4 and 6, layers 1, 3 and 6 are 20 nm thick, layers 2 and 4 are 10 nm thick and layer 5 is 40 nm thick. The

Graphene-enhanced plasmonic nanohole arrays for environmental sensing in aqueous samples

• Christa Genslein,
• Peter Hausler,
• Eva-Maria Kirchner,
• Rudolf Bierl,
• Antje J. Baeumner and
• Thomas Hirsch

Beilstein J. Nanotechnol. 2016, 7, 1564–1573, doi:10.3762/bjnano.7.150

• that this type of plasticizers adsorbs on polystyrene resins by multiple adsorbent–adsorbate interactions such as hydrogen bonding and π-stacking [38], which makes them an ideal analyte for the evaluation of the graphene-modified gold surfaces in SPR. Nanostructured surfaces are promising in enhancing

• method described by Masson et al. [39][40]. Drop casting of the polystyrene particles on a clean glass slide leads to a densely packed monolayer on the substrate (Figure 2). The sphere mask consists of ordered areas of several square millimetres covering more than the optical spot size of the SPR device

• polystyrene particles on a clean and dry glass slide. The polystyrene particles have a diameter of 1.04 μm (SD = 0.04 μm, microparticles GmbH). Covering with a Petri dish allows a slow evaporation rate, resulting in a close-packed monolayer. The sphere masks were dried overnight. In order to create a nanohole

Polystyrene-block-poly(ethylene oxide) copolymers as templates for stacked, spherical large-mesopore silica coatings: dependence of silica pore size on the PS/PEO ratio

• Roberto Nisticò,
• Giuliana Magnacca,
• Sushilkumar A. Jadhav and
• Dominique Scalarone

Beilstein J. Nanotechnol. 2016, 7, 1454–1460, doi:10.3762/bjnano.7.137

• narrow pore size distribution and high porosity have been obtained by a sol–gel reaction of a silicon oxide precursor (TEOS) and using polystyrene-block-poly(ethylene oxide) (PS-b-PEO) copolymers as templates in an acidic environment. PS-b-PEO copolymers with different molecular weight and composition

• block copolymers, such as polystyrene-block-poly(ethylene oxide) (PS-b-PEO), have been successfully employed to synthetize mesoporous oxides [19][25]. Starting from these previous works, we decided to develop a systematic study to gain better control on the morphological features of templated silica

Three-gradient regular solution model for simple liquids wetting complex surface topologies

• Sabine Akerboom,
• Marleen Kamperman and
• Frans A. M. Leermakers

Beilstein J. Nanotechnol. 2016, 7, 1377–1396, doi:10.3762/bjnano.7.129

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

• , end-to-end (via the polystyrene-capped (111) facet) assembly was noticed for more hydrophilic solvent combinations [42]. This helps to understand the role of water in the growth of the AgNPs–cysteamine assemblies under study. The poorer affinity of “heavy” cysteamine to the solvent (light water

Reasons and remedies for the agglomeration of multilayered graphene and carbon nanotubes in polymers

• Rasheed Atif and
• Fawad Inam

Beilstein J. Nanotechnol. 2016, 7, 1174–1196, doi:10.3762/bjnano.7.109

• properties using TEM in polystyrene–1 wt % MWNT. They have reported a 42% increase in breaking strength, which is an indication of strong interfacial adhesion [144]. The trend for strength and modulus with varying content of CSCNT loading is shown in Figure 15 [141]. It can be seen that mechanical properties

Experimental and simulation-based investigation of He, Ne and Ar irradiation of polymers for ion microscopy

• Lukasz Rzeznik,
• Yves Fleming,
• Tom Wirtz and
• Patrick Philipp

Beilstein J. Nanotechnol. 2016, 7, 1113–1128, doi:10.3762/bjnano.7.104

• studies on monatomic bombardment on polymers report on 5 keV and 500 eV Ar atom bombardment of polystyrene oligomers [21] and polystyrene molecules containing 61 repeat units [22] adsorbed on Ag(111), respectively. In the first study, the excited volume in the substrate induces collective motion which

• composition can be found. Methods Experimental setup For this study, different polymer samples were spin-coated on silicon (111). The homopolymers of polystyrene (PS) with molecular mass Mw = 1 900 (Mw/Mn = 1.10) and poly(methyl methacrylate) (PMMA) with molecular mass Mn = 22 200 (Mw/Mn = 1.07) were obtained

• evolution of the He, Ne and Ar positions in the system at atomic level. Four different polymers have been selected: polyethylene (PE), polytetrafluoroethylene (PTFE), atactic polystyrene (PS) and poly(methyl methacrylate) (PMMA). Different polymer samples have been created, each sample containing 10

Multiwalled carbon nanotube hybrids as MRI contrast agents

• Nikodem Kuźnik and
• Mateusz M. Tomczyk

Beilstein J. Nanotechnol. 2016, 7, 1086–1103, doi:10.3762/bjnano.7.102

• conditions [34]. The so-obtained hybrids were further wrapped with anionic polyelectrolyte polystyrene sulfonate (PSS) and then with cationic polyethylenimine (PEI). A modification of this hybrid, PEI/PSS/SPIO/oMWCNT#Yin, was additionally synthesized by covalent carboxylic-amine crosslinking with folic acid

Generalized Hertz model for bimodal nanomechanical mapping

• Aleksander Labuda,
• Marta Kocuń,
• Waiman Meinhold,
• Deron Walters and
• Roger Proksch

Beilstein J. Nanotechnol. 2016, 7, 970–982, doi:10.3762/bjnano.7.89

• experimental data and extract a shape and size of the tip interacting with a polystyrene surface. Keywords: bimodal atomic force microscopy; bimodal spectroscopy; contact mechanics; multifrequency; nanomechanical mapping; nanomechanics; Introduction Over the decades since its invention [1] the atomic force

• amplitude modulation (AM) [1][18][19], phase modulation (PM) [43][44][45][46] and frequency modulation (FM) [23][36][47]. Finally, a method for extracting the tip size and tip shape from bimodal AFM approach curves is presented and demonstrated on a polystyrene sample. Figure 1 provides a diagram of the

• measurements [39][55]. Here, the AM-AM, AM-PM and AM-FM configurations are explored in detail. Practical considerations for these choices will be discussed later. Results A polystyrene surface was probed with bimodal approach curves (also known as “force–distance” curves), where the bimodally oscillating

Large-scale fabrication of achiral plasmonic metamaterials with giant chiroptical response

• Morten Slyngborg,
• Yao-Chung Tsao and
• Peter Fojan

Beilstein J. Nanotechnol. 2016, 7, 914–925, doi:10.3762/bjnano.7.83

• been investigated. These have been thoroughly studied [17][18][19][20] and other structures including theoretical suggestions are limited to plasma sphere arrays [21], gold dot arrays [22], gold square arrays [23], metal disk arrays [24], two layer hole arrays [25], polystyrene sphere templates for

• [31], preassembled nanoparticles [32][33][34] and a variety of colloidal nanolithography techniques [35][36][37]. Compared to the above mentioned PCMs, the experimentally proven ECMs only comprise structures from polystyrene sphere templates for gold deposition [26], structures formed by carbon

Magnetic switching of nanoscale antidot lattices

• Ulf Wiedwald,
• Joachim Gräfe,
• Kristof M. Lebecki,
• Maxim Skripnik,
• Felix Haering,
• Gisela Schütz,
• Paul Ziemann,
• Eberhard Goering and
• Ulrich Nowak

Beilstein J. Nanotechnol. 2016, 7, 733–750, doi:10.3762/bjnano.7.65

• , nanosphere lithography offers the preparation of a self-assembled monolayer on the time scale of minutes even on a centimetre length scale. In this work, polystyrene(PS)-based nanosphere lithography was chosen, since monodisperse PS nanosphere suspensions are nowadays commercially available with a wide range

Tight junction between endothelial cells: the interaction between nanoparticles and blood vessels

• Yue Zhang and
• Wan-Xi Yang

Beilstein J. Nanotechnol. 2016, 7, 675–684, doi:10.3762/bjnano.7.60

• exposure to NPs (polystyrene nanoparticles, quantum dots, single-wall carbon nanotubes) results in the disruption of the alveolar epithelial barrier, the extent of which also depends on the composition, shape and surface charge of the NPs [31]. Carbon nanotubes also show their capacity to penetrate the

Correlative infrared nanospectroscopic and nanomechanical imaging of block copolymer microdomains

• Benjamin Pollard and
• Markus B. Raschke

Beilstein J. Nanotechnol. 2016, 7, 605–612, doi:10.3762/bjnano.7.53

• properties between and within polymer microdomains. Methods We study a high molecular weight block copolymer of polystyrene-block-poly(methyl methacrylate) (PS-b-PMMA), with a relative chain length of 270.0-b-289.0 Mn × 103 (P4443-SMMA, Polymer Source), spin-coated from a 1% w/v solution in toluene onto

Characterization of spherical domains at the polystyrene thin film–water interface

• Khurshid Ahmad,
• Xuezeng Zhao,
• Yunlu Pan and
• Danish Hussain

Beilstein J. Nanotechnol. 2016, 7, 581–590, doi:10.3762/bjnano.7.51

• , University of Engineering and Technology, Peshawar, Pakistan State Key Laboratory of Robotics and Systems and School of Mechatronics Engineering, Harbin Institute of Technology, Harbin 150001, P.R. China 10.3762/bjnano.7.51 Abstract Spherical domains that readily form at the polystyrene (PS)–water interface

• have been used to produce such films. Polystyrene (PS) is one of the most widely used materials for the preparation of thin films. Thin PS films have been prepared by spin coating [11][12][13][14][15]. So far, these films have been used in different studies related to surface and interface science, for

• , China), polystyrene beads (average MW ≈350,000; Aldrich, USA), AFM cantilevers (RTESPA, DNP, SNL; Bruker, USA), AFM (Innova; Bruker, USA), digital microscope (KH1300; Hirox, Japan), spin coater (KW-4A; SETCAS Electronics Co. Ltd., Beijing, China), and drop meter (MAIST, Vision, China). Sample

Active multi-point microrheology of cytoskeletal networks

• Tobias Paust,
• Tobias Neckernuss,
• Lina Katinka Mertens,
• Ines Martin,
• Michael Beil,
• Paul Walther,
• Thomas Schimmel and
• Othmar Marti

Beilstein J. Nanotechnol. 2016, 7, 484–491, doi:10.3762/bjnano.7.42

• viscoelastic media. Experimental Human keratins 8 and 18 were isolated and purified according to [28][29]. They were assembled into networks in 10 mM Tris-HCl buffer with a protein concentration of 0.5 g/L. Polystyrene beads with 1 µm diameter were incorporated in the network as measuring probes for

High-bandwidth multimode self-sensing in bimodal atomic force microscopy

• Michael G. Ruppert and
• S. O. Reza Moheimani

Beilstein J. Nanotechnol. 2016, 7, 284–295, doi:10.3762/bjnano.7.26

• calibration grating available from NT-MDT with periodic rectangular features of heights h = 21.6 ± 1.5 nm and a blend of polystyrene (PS) and polyolefin elastomer (ethylene-octene copolymer) (LDPE) available from Bruker (PS-LDPE-12M). The PS regions of the sample have elastic modulus numbers around 2 GPa

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

• ]. Multi layered films of graphene were deposited onto gold-coated glass microscope slides by alternating layers of graphene–surfactant with oppositely charged polyelectrolytes, e.g., graphene(+)CTAB layers alternated with polyanionic layers of sodium polystyrene sulfonate (PSS), while graphene(−)SDS was

Single-molecule mechanics of protein-labelled DNA handles

• Vivek S. Jadhav,
• Dorothea Brüggemann,
• Florian Wruck and
• Martin Hegner

Beilstein J. Nanotechnol. 2016, 7, 138–148, doi:10.3762/bjnano.7.16

• ) were conjugated with streptavidin or neutravidin proteins. The DIG-modified ends of these hybrids were bound to surface-modified polystyrene (anti-DIG) beads. Using different physiological buffers, optical force measurements showed consistent mechanical characteristics with long dissociation times

• ) in high-resolution measurements [10]. We previously presented optical force rupture measurements of the nascent polypeptide chain from biotinylated ribosomes, which were specifically bound to surface-modified polystyrene beads [11]. While the ribosome was translating, the biotinylated lysine residue

• and coupling to polystyrene beads PCR amplification of plasmid pTYB1 (7477 bp, New England Biolabs, Ireland (NEB)) with 5’-biotin (5’-AAT TCT TGA AGA CGA AAG GGC GGC-3’ for 4056 bp DNA and 5’-GGA TAC GAC GAT ACC GAA GAC AGC-3’ for 3034 bp DNA) and 5’-thiol or 5’-DIG end-modified primers (both have the

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

• polystyrene brush on the deposition of ZnO thin films under moderate conditions. On a non-modified SiOx surface, island growth is observed, whereas the polymer brush induces homogeneous film growth. A chemical modification of the polystyrene brushes during the mineralization process occurs, which enables

• measurements as well as scanning electron microscopy (SEM), atomic force microscopy (AFM) and X-ray diffraction (XRD). Infrared spectroscopy (IR) measurements were used to investigate the polystyrene brushes before and after modification. Keywords: bioinspired synthesis; polymer brush; template activation

• [36] as organic templates are known, which can modify the surface charge on the substrates for ZnO precipitation under moderate conditions. Based on these studies, we investigated the ZnO film formation on silicon wafers modified with vinyl-terminated polystyrene (PS) brushes. Those brushes consist of

Ultrastructural changes in methicillin-resistant Staphylococcus aureus induced by positively charged silver nanoparticles

• Dulce G. Romero-Urbina,
• Humberto H. Lara,
• J. Jesús Velázquez-Salazar,
• M. Josefina Arellano-Jiménez,
• Eduardo Larios,
• Anand Srinivasan,
• Jose L. Lopez-Ribot and
• Miguel José Yacamán

Beilstein J. Nanotechnol. 2015, 6, 2396–2405, doi:10.3762/bjnano.6.246

• diluted in Mueller–Hinton broth (Difco, Detroit, Mich.) and plated in flat-bottom polystyrene 96-well tissue culture plates at a final density of 5.0 × 105 CFU/well. Two-fold serial dilutions of AgNPs were prepared at a final volume of 100 µL per well. The final concentration of the AgNPs ranged from 0.4

Nanoscale rippling on polymer surfaces induced by AFM manipulation

• Mario D’Acunto,
• Franco Dinelli and
• Pasqualantonio Pingue

Beilstein J. Nanotechnol. 2015, 6, 2278–2289, doi:10.3762/bjnano.6.234

• wide spectrum of polymers has been investigated including polystyrene (PS) [13][20], poly(methyl methacrylate) (PMMA) [25], poly(ethylene terephthalate) (PET) [23], poly(vinyl acetate) (PVAc) [26] and poly(ε-caprolactone) (PCL) [23]. Recently, we have reviewed wear occurring on polymeric surfaces and

• rippling for the thin lamellar microphases forming in polystyrene/poly(ethylene oxide) block copolymer (PS-b-PEO) films [48]. In particular via an analysis of the ripple patterns, they have deduced local thermochemical parameters such as the melting temperature of PEO, the Tg of PS, the specific heat of PS

• one to several hundreds of nanometers can be reproduced on the surface of polycarbonate (PC), poly(methyl methacrylate) (PMMA), and polystyrene (PS) films. Authors have clearly shown that the ripple formation varies with T and polymer type (Figure 8a). The dependence on T has been characterized and

Selective porous gates made from colloidal silica nanoparticles

• Roberto Nisticò,
• Paola Avetta,
• Paola Calza,
• Debora Fabbri,
• Giuliana Magnacca and
• Dominique Scalarone

Beilstein J. Nanotechnol. 2015, 6, 2105–2112, doi:10.3762/bjnano.6.215

• were prepared by spin-coating deposition of colloidal silica nanoparticles on an appropriate macroporous substrate. Silica nanoparticles very homogenous in size were obtained by sol–gel reaction of a metal oxide silica precursor, tetraethyl orthosilicate (TEOS), and using polystyrene-block-poly

Temperature-dependent breakdown of hydrogen peroxide-treated ZnO and TiO₂ nanoparticle agglomerates

• Sinan Sabuncu and
• Mustafa Çulha

Beilstein J. Nanotechnol. 2015, 6, 1897–1903, doi:10.3762/bjnano.6.193

• common ways of increasing the NP dispersion in aqueous media. Polymers such as polystyrene, poly(methyl methacrylate) (PMMA), and poly(acrylic acid) are also widely used to obtain dispersed NPs in aqueous environments [7][8][9]. Although the use of surfactants can provide better dispersion, they

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

• a templating substrate – properties which, in turn, are key properties for nanodevices. Experimental Template preparation by polymer-blend lithography Polymer solution: Polystyrene (PS, Mw = 96 kg/mol, PDI 1.04) and poly(methyl methacrylate) (PMMA, Mw = 9.59 kg/mol, PDI 1.05) were purchased from

Polymer blend lithography for metal films: large-area patterning with over 1 billion holes/inch²

• Cheng Huang,
• Alexander Förste,
• Stefan Walheim and
• Thomas Schimmel

Beilstein J. Nanotechnol. 2015, 6, 1205–1211, doi:10.3762/bjnano.6.123

• polystyrene (PS) and poly(methyl methacrylate) (PMMA), dissolved in methyl ethyl ketone (MEK) is used. This system forms a purely lateral structure on the substrate at controlled humidity, which means that PS droplets are formed in a PMMA matrix, whereby both phases have direct contact both to the substrate

• plasmonic resonance; metal islands; metal nanostructures; metal polymer blend lithography (metal PBL); nano-patterned template; nanoscale discs; optical transmission; perforated metal film; polymer phase separation; poly(methyl methacrylate) (PMMA); polystyrene (PS); self-assembly; spin-coating; surface

• polystyrene (PS)/poly(methyl methacrylate) (PMMA) blend film from a blend solution ends with a purely lateral phase separation between the two immiscible polymers under controlled spin-coating parameters (see Figure 1a). As reported in our earlier publication, the ambient atmosphere (humidity), the molar mass