Plasmonic nanostructures fabricated using nanosphere-lithography, soft-lithography and plasma etching

• Manuel R. Gonçalves,
• Taron Makaryan,
• Fabian Enderle,
• Stefan Wiedemann,
• Alfred Plettl,
• Othmar Marti and
• Paul Ziemann

Beilstein J. Nanotechnol. 2011, 2, 448–458, doi:10.3762/bjnano.2.49

• low Young’s modulus of PDMS used in the fabrication of the stamp, deformed hemispheres may occur for very small PS beads. The zeroth-order reflectance and transmittance of gold films evaporated onto the hemispheres was measured. The low reflectance bands found on coated hemispheres, when compared to

Infrared receptors in pyrophilous (“fire loving”) insects as model for new un-cooled infrared sensors

• David Klocke,
• Anke Schmitz,
• Helmut Soltner,
• Herbert Bousack and
• Helmut Schmitz

Beilstein J. Nanotechnol. 2011, 2, 186–197, doi:10.3762/bjnano.2.22

• deflection y of this membrane caused by a pressure difference can be calculated as a function of the radial distance r with the shell theory [26] with R: radius of the membrane, D: flexural stiffness of the membrane, E: Young’s modulus, tP: thickness of the membrane, ν: Poisson’s ratio. Equation 2 is a good

Capillary origami: superhydrophobic ribbon surfaces and liquid marbles

• Glen McHale,
• Michael I. Newton,
• Neil J. Shirtcliffe and
• Nicasio R. Geraldi

Beilstein J. Nanotechnol. 2011, 2, 145–151, doi:10.3762/bjnano.2.18

• stretching a thin membrane substrate is related to the principal radii of curvatures of the substrate, where κb is the elastic bending rigidity and κG is the Gaussian bending modulus [20]. For a film of thickness h, the bending rigidity is given by κb = Eh3/12(1−ν2), where E is Young’s modulus and ν is