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Fig. 1: UCL Nanotechnology Centre. The schematic shows the role that the Centre will play as a focus for interdisciplinary nanoscale materials and device research at UCL. By acting as bridge between biomedical, physical and electrical sciences, the Centre will cross the chip-to-cell interface: an essential step if the UK is to remain internationally competitive in biotechnology. |
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Fig. 2: Laboratories on chip fabricated as part of UCL research program. An array of microcalorimeters deposited on Si. Each comprises a heater and two thermometers, allowing the heat capacity of milligram size samples to be measured. This technology is in its infancy but is proliferating rapidly. The new Centre will allow UCL to maintain its leadership role in this area. |
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| Fig. 3: Temperature-dependent magnetic force imaging. Data show magnetic contrast near artificial (straight vertical line) and natural (clustered around oblique line) grain boundaries in a manganite film, deposited by pulsed laser deposition, exhibiting colossal magnetoresistance. Above the nominal Curie point (350 K) for the film (far left), the grain boundaries still display a magnetic moment whose magnitude and spatial decay length into the grains shrink as the temperature is raised above 360 K (far right). |
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| Fig. 4: UCL theory and modelling of atomic and electronic motion at the nanoscale. An atomic force microscope tip leaves self-forming 'nanostrings' of atoms as it is pulled away from a surface (left), while an electron moving coherently through a nanowire is predicted to couple to the atomic vibrations, lowering the band gap locally as it moves along (right). |
| Fig. 5: UV fabrication methods at UCL. Copper microstructures formed directly on AlN via direct VUV irradiation of palladium acetate with an excimer lamp system constructed at UCL. The irradiated zones result in the creation of Pd clusters which act as nucleation sites during subsequent Cu deposition. The figure indicates the ability to readily process conventional chip-sized area. No fundamental limits are foreseen for the larger areas and finer linewidths to be explored in the new Centre. | ![]() |
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Fig. 6: Diamond electronics. AFM image (left) of a 2mm x 2mm section of highly oriented diamond nuclei grown by microwave plasma-assisted CVD. The (100) grains are oriented with respect to the Si(100) substrate and mis-aligned to each other by less than 4%. Diamond optoelectronic devices (right) produced at UCL are now commercially produced by UK industry under licence. |
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Fig. 7: Strongly correlated Fermi system. Phase diagram for (Mn,Fe,Co)Si. Colours in top frame represent electrical conductivity, those in bottom frame correspond to low field magnetisation. While MnSi is a classic metallic ferromagnet and CoSi a diamagnetic metal, FeSi is a non-magnetic small gap insulator, which, when doped, becomes a low carrier density heavy fermion metal. Depending on the sign of the carriers (holes or electrons), the metal can remain a Pauli paramagnet or what seems to be a fully polarised, ferromagnetic electron gas. A curious fact is that even though FeSi and CoSi are both non-magnetic, most intermediate mixtures of the two isostructural compounds are magnetic. Quantum interference effects appear to account for the entire magnetotransport to temperatures above 50 K. At the new Centre such effects will be followed into the mesoscopic regime. |
| Fig. 8: Nanomagnetism. AFM image of an aminosilane coated iron oxide magnetic fluid deposited on a glass slide (350 x 350 x 10 nm3). These biocompatible fluids could be the basis of a new magnetic separation based technology for protein purification, and a means of enzyme immobilisation and assaying. | ![]() |
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Fig. 9: Nanofluids: A snapshot of a hydrated vermiculite clay, in which the clay layer spacing is 4nm. The colour coding is: blue-O, white-H, black-Si/Mg, green-N, red-C. Our neutron diffraction studies of this system have provided a uniquely detailed picture of aqueous structure at a charged solid surface, in the so-called electrical double layer. The data reveal two layers of highly structured water molecules at each clay surface. More surprisingly, the distribution of propyl-ammonium counter-ions reaches a maximum at the centre of the interlayer region. The combined X-ray reflectometer/uniaxial stress cell in the new Centre will allow interfacial structure to be directly related to forces between surfaces. The new understanding of confined liquids and solid-liquid interfaces will form the basis for our research into 'chip-cell-probe' systems. |
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| Fig. 10: Development of AFM systems for biology. The results are images of surface and intracellular structures of living cells (at left, live cells on glass with prominent cytoskeletal fibres) and maps of physical properties - e.g. receptor binding forces - of cell materials. We have also integrated a confocal microscope with the AFM to accomplish simultaneous fluorescence analysis (at right, a 3D isosurface reconstruction of bone cells on a mineralised substrate (blue) labelled in two colours (red, green) to independently demonstrate the distribution of two membrane proteins). The future lies in developing the bio-AFM further and introducing a range of more sophisticated physical techniques, electrophysiological applications and micromanipulation methods. Each image measures 50 x 50 μm2. |