The X-ray phase tomography of biological samples is reported, which is based on X-ray Talbot interferometry. Its imaging principle is described in detail, and imaging results obtained for a cancerous rabbit liver and a mouse tail with synchrotron radiation are presented. Because an amplitude grating is needed to construct an X-ray Talbot interferometer, a high-aspectratio grating pattern was fabricated by X-ray lithography and gold electroplating. X-ray Talbot interferometry has an advantage that it functions with polychromatic cone-beam X-rays. Finally, the compatibility with a compact X-ray source is discussed.
We fabricated dye-adsorbed NiO solar cells (pDSCs) with six different metal-free organic dyes having various ground-state oxidation potentials. Under monochromatic light irradiation, all dyes showed cathodic current at wavelengths where the dyes absorb, suggesting hole injection occurred from the adsorbed dyes to the valence band of NiO. Absorbed photon-to-current conversion efficiency (APCE) tends to increase with the increase of energy difference (∆E) between the valence band edge of NiO and the ground state of the dyes. The maximum APCE of 30% was obtained with 0.6 eV of the ∆E. The apparent hole diffusion coefficient in the NiO electrode was nearly independent from light intensity, and the values were estimated to be 4 × 10 -8 cm 2 /s. On the other hand, hole lifetime depends on light intensity, ranging from 3 × 10 -2 to 1 × 10 0 s. Investigation of the anchoring site of the dyes and the results of molecular orbital calculations suggested that electron injection from the dye to the valence band of NiO, occurring just after the hole injection, is the major factor of the relatively low efficiency even with the case of large ∆E.
Colloidal gold nanoparticles with a broad size distribution were prepared by laser ablation of a gold metal plate in an aqueous solution of sodium dodecyl sulfate (SDS) and were fragmented under irradiation of a 532 nm laser at different SDS concentrations and laser fluences. Gold nanoparticles with a desired average size (1.7-5.5 nm in diameter) were prepared by tuning properly the surfactant concentration and the laser fluence. The concentration of SDS was found to be higher than a critical micelle concentration so as to gain a significant size reduction and to obtain stable final products. Laser ablation in combination with the laser-induced size control provides a versatile full physical preparation method of size-selected gold nanoparticles.
Platinum nanoparticles were produced by laser ablation of a platinum metal plate in an aqueous solution of sodium dodecyl sulfate (SDS). The absorption spectrum of the platinum nanoparticles was essentially the same as that of platinum nanoparticles chemically prepared in a solution. The size distribution of the nanoparticles thus produced was measured to be in the range of 1-7 nm in diameter by an electron microscope. The abundance of the nanoparticles changes with the concentration of SDS in the solution. Stable platinum nanoparticles were found to be produced by this method even in pure water.
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