Because of their mechanical strength, chemical stability, and low molecular weight, carbon nanotubes (CNTs) are attractive biological implant materials. Biomaterials are typically implanted into subcutaneous tissue or bone; however, the long-term biopersistence of CNTs in these tissues is unknown. Here, tangled oxidized multi-walled CNTs (t-ox-MWCNTs) were implanted into rat subcutaneous tissues and structural changes in the t-ox-MWCNTs located inside and outside of macrophages were studied for 2 years post-implantation. The majority of the large agglomerates were present in the intercellular space, maintained a layered structure, and did not undergo degradation. By contrast, small agglomerates were found inside macrophages, where they were gradually degraded in lysosomes. None of the rats displayed symptoms of cancer or severe inflammatory reactions such as necrosis. These results indicate that t-ox-MWCNTs have high biopersistence and do not evoke adverse events in rat subcutaneous tissue in vivo, demonstrating their potential utility as implantable biomaterials.

The light-harvesting 1 reaction center (LH1-RC) complex from Thermochromatium (Tch.) tepidum exhibits unusual Q(y) absorption by LH1 bacteriochlorophyll-a (BChl-a) molecules at 915nm, and the transition energy is finely modulated by the binding of metal cations to the LH1 polypeptides. Here, we demonstrate the metal-dependent interactions between BChl-a and the polypeptides within the intact LH1-RC complexes by near-infrared Raman spectroscopy. The wild-type LH1-RC (B915) exhibited Raman bands for the C3-acetyl and C13-keto CO stretching modes at 1637 and 1675cm(-1), respectively. The corresponding bands appeared at 1643 and 1673cm(-1) when Ca(2+) was biosynthetically replaced with Sr(2+) (B888) or at 1647 and 1669cm(-1) in the mesophilic counterpart, Allochromatium vinosum. These results indicate the significant difference in the BChl-polypeptide interactions between B915 and B888 and between B915 and the mesophilic counterpart. The removal of the original metal cations from B915 and B888 resulted in marked band shifts of the C3-acetyl/C13-carbonyl νCO modes to ~1645/~1670cm(-1), supporting a model in which the metal cations are involved in the fine-tuning of the hydrogen bonding between the BChl-a and LH1-polypeptides. Interestingly, the interaction modes were almost identical between the Ca(2+)-depleted B915 and Sr(2+)-depleted B888 and between B915 and Ca(2+)-substituted B888, despite the significant differences in their LH1 Q(y) peak positions and the denaturing temperatures, as revealed by differential scanning calorimetry. These results suggest that not only the BChl-polypeptide interactions but some structural origin may be involved in the unusual Q(y) red-shift and the enhanced thermal stability of the LH1-RC complexes from Tch. tepidum.

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Raman scattering and infrared (IR) absorption spectra of enantiopure (R)-propylene carbonate ((R)PC) and racemic propylene carbonate (PC) were recorded at room temperature, 25 °C, in benzene (Bz) solution and in the pure liquid state to investigate the presence of dimers and other higher order intermolecular associations. (R)PC and PC both demonstrated a strong C=O stretching vibrational band. The band exhibited changes in its shape and resonance wavenumber highly dependent on the concentrations of PCs, whereas a difference between the chirality of (R)PC and PC had little influence. In an extremely dilute condition, doubly split bands were observed at 1807 and 1820 cm-1 in both Raman and IR spectra, which are assigned to the characteristic bands of isolated monomeric PCs. An additional band appeared at 1795 cm-1 in a dilute to concentrated regime, and its magnitude strengthened with increasing concentrations accompanied with slight increasing in the magnitude of 1807 cm-1 band in Raman spectra, while an increase in the magnitude of 1807 cm-1 band was clearly greater than that of 1795 cm-1 band in IR spectra. The spectrum changes at 1795 and 1807 cm-1 were attributed to characteristics of anti-parallel dimer formation of PCs caused by strong dipole-dipole interactions between C=O groups. Moreover, another additional signal was clearly observed at 1780-1790 cm-1 in a concentrated regime, and became the primary signal in the pure liquid state with slight increasing in the intensity of 1795 cm-1 band in Raman spectra. On the other hand, in IR spectra the observed increasing of 1780-1790 cm-1 band was much less than that of 1795 cm-1 band. These newly found spectrum changes in the concentrated regime are attributed to the formation of anti-parallel tetramers of PCs based on the characteristics of band selection rule found in Raman and IR spectra. Equilibrium constants for the anti-parallel dimer (KD) and tetramer formation (KT) of PCs in Bz solution and in the pure liquid state were also determined using the Raman and IR data assuming chemical processes: 4PC ↔ 2(PC)2 ↔ (PC)4.

The effect of stress stimulation on gold (Au) induced lateral crystallization (GILC) of amorphous Ge on insulating substrates is investigated. As a result, the GILC is significantly enhanced by using compressive residual stresses of up to 200 MPa in TEOS-SiO2. In addition, it is found that the annealing temperature necessary to cause the GILC for a short annealing time (60 min) can be decreased to 130 °C. We have demonstrated that the GILC enhancement was caused by the stress stimulation contributed to bond rearrangement and Au easily diffused into Ge. This study proposes a unique low temperature crystallization technique that introduces a residual film stress on metal induced lateral crystallization, paving the way for the low-cost fabrication of flexible electronic devices on low-softening temperature plastic substrates.