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Beilstein J. Nanotechnol. 2021, 12, 304–318, doi:10.3762/bjnano.12.25
Figure 1: FIB-o-mat overview. (a) For patterning the beam spot follows a rasterized beam path with a defined ...
Figure 2: Geometric primitives and rasterization styles available for high-level pattern generation. (a) Sing...
Figure 3: Geometric entities and rasterization styles available for low-level pattern generation. (a) Pre-ras...
Figure 4: Geometry-optimized patterning. (a) Beam path generation by curve off-setting around arbitrary disco...
Figure 5: Magnetic nanopatterning of a Co/Pt multilayer. Fourier-transform holography (FTH) images (a–f) with...
Figure 6: Single-layer graphene resonator. (a) Secondary electron He ion microscopy image of the graphene res...
Figure 7: Coupled plasmonic antennas. (a–c) Scanning electron micrographs of gold tetramers on glass with a t...
Figure 8: Optimized tetramer. Secondary electron He ion microscopy images of gold tetramers on glass with min...
Beilstein J. Nanotechnol. 2017, 8, 28–37, doi:10.3762/bjnano.8.4
Figure 1: MFM imaging of a HDD featuring PMR with magnetic domains being aligned parallel or antiparallel to ...
Figure 2: Magnetic recording medium: (a) TEM cross-section image with indication of the stack setup used for ...
Figure 3: Polarization dependence of absorptivity (λ = 785 nm): p-polarized light is 3.5–4 times better absor...
Figure 4: Influence of the DC bias field during laser illumination (λ = 532 nm, CW, P = 8 mW) on an as-is HDD...
Figure 5: (a) Free-hand writing of magnetic features at CW illumination (p-polarized, 785 nm, 12 mW), yieldin...
Figure 6: MFM phase scans and intensity profiles of “dots” laser-written at 785 nm. The laser power was kept ...
Figure 7: Power absorption per volume within the magnetic stack. (a) Cross-sectional absorption per layer of ...
Figure 8: Comsol thermal modelling of a Gaussian laser pulse (P = 40 mW; λ = 785 nm; τ = 50 ns, γ = 70°) bein...