Abstract:In order to examine the possibility of (persistent) carrier doping to molecular crystals by light exposure, some different types of molecular crystals containing photoreactive species are synthesized and characterized. The [Ru(bpy) 3 ] 2+ cation (bpy = 2,2'-bipyridyl) yielded two different new complexes with [Ni(dmit) 2 ]radical species, both of which were structurally characterized and turned out to be band insulators. Methy viologen (MV) has been found to yield a new phase of the complex with [Ni(dmit) 2 ]-,… Show more
“…In addition to this apparent transition at 100 K, a slight and gradual increase in resistance at 260−290 K dependent on the duration of exposure to light in the ultraviolet−visible regime has also been reported . This feature was also observed in the present experiments, as indicated by arrows in Figure .…”
Multiprobe measurements were performed on tiny single crystals of DMe-DCNQI complexes prepared directly on SiO2/Si substrates. The differences in conduction properties between the micro- and nanocrystals and bulk crystals were observed.
“…In addition to this apparent transition at 100 K, a slight and gradual increase in resistance at 260−290 K dependent on the duration of exposure to light in the ultraviolet−visible regime has also been reported . This feature was also observed in the present experiments, as indicated by arrows in Figure .…”
Multiprobe measurements were performed on tiny single crystals of DMe-DCNQI complexes prepared directly on SiO2/Si substrates. The differences in conduction properties between the micro- and nanocrystals and bulk crystals were observed.
“…Thus a single crystal can be modified to have a junction structure ( Figure 4). 81,92,93 Junction structures are comprised of qualitatively different conduction parts, being a basic and necessary structure for all kinds of semiconductor devices. This treatment may correspond to the mixing of an insulator into the metal at a molecular level.…”
Section: Firstmentioning
confidence: 99%
“…Next, in order to distinguish artifacts from intrinsic and reproducible phenomena, the irradiation conditions were widely varied ( Figures 6 and 7), 98 and all the resultant changes and products were examined and characterized one by one. 80,81,92,93,98107 If we call the starting material α, the irradiated products from various conditions were classified into four different compounds called β, γ, δ and ε. The products are summarized in Figure 6 with their chemical formulae and typical irradiation conditions for production from α (Table 1).…”
Section: Development Of New Types Of Equipmentmentioning
This study concerns development of a non-destructive method to control conduction and magnetism of molecular solids such as single crystals of charge-transfer complexes. The method is named “optical doping”, where appropriate irradiation is utilized under ambient conditions. Owing to this feature, it can be applied to a wide range of substances while measuring the properties during the control. In addition, the method adds unique conduction and magnetic properties to common insulators. Unlike other doping methods, optical doping only affects the properties and/or structures of the irradiated part of a sample while leaving the rest of the sample unchanged. There are two patterns in the optical doping. Irreversible optical doping produces junction-structures on the single molecular crystals, which exhibit characteristic behavior of semiconductor devices such as diodes and varistors. Reversible optical doping produces “giant photoconductors” and “photomagnetic conductors” by realizing unprecedented metallic photoconduction. In the latter case, localized spins are also excited to produce a Kondo system, where carriers and localized spins interact with each other. Not only the control of conduction and magnetism, the optical doping has realized the observation of physical properties in molecular crystals hardly observed under any thermodynamic condition.
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