Rational Chemical Multifunctionalization of Graphene Interface Enhances Targeted Cancer Therapy

The synthesis of a drug delivery platform based on graphene was achieved through a step‐by‐step strategy of selective amine deprotection and functionalization. The multifunctional graphene platform, functionalized with indocyanine green, folic acid, and doxorubicin showed an enhanced anticancer activity. The remarkable targeting capacity for cancer cells in combination with the synergistic effect of drug release and photothermal properties prove the great advantage of a combined chemo‐ and phototherapy based on graphene against cancer, opening the doors to future therapeutic applications of this type of material.     

Photofunctional Nanomodulators for Bioexcitation

A single organism comprises diverse types of cells. To acquire a detailed understanding of the biological functions of each cell, comprehensive control and analysis of homeostatic processes at the single‐cell level are required. In this study, we develop a new type of light‐driven nanomodulator comprising dye‐functionalized carbon nanohorns (CNHs) that generate heat and reactive oxygen species under biologically transparent near‐infrared (NIR) laser irradiation. By exploiting the physicochemical properties of the nanohorns, cellular calcium ion flux and membrane currents were successfully controlled at the single‐cell level. In addition, the nanomodulator allows a remote bioexcitation of tissues during NIR laser exposure making this system a powerful tool for single‐cell analyses and innovative cell therapies.     

Elastic Scattering of 6He + p at 82.3MeV/nucleon

Differential cross sections for the elastic scattering of halo nucleus 6He on proton target were measured at 82.3 MeV/u. The experimental results axe well reproduced by optical model calculations using global potential KD02 with a reduction of the depth of real volume part by a factor of 0.7. A systematic analysis shows that this behavior might be related to the weakly bound property of unstable nuclei.     

Study of N=20 shell gap with 1H(28Ne,27,28Ne) reactions

This paper reports on the ¹H(²⁸Ne,²⁸Ne) and ¹H(²⁸Ne,²⁷Ne) reactions studied at intermediate energy using a liquid hydrogen target. From the cross section populating the first 2⁺ excited state of ²⁸Ne, and using the previously determined B(E2) value, the neutron quadrupole transition matrix element has been calculated to be M_n=13.8 ±3.7 fm². In the neutron knock-out reaction, two low-lying excited states were populated in ²⁷Ne. Only one of them can be interpreted by the sd shell model while the additional state may intrude from the fp shell. These experimental observations are consistent with the presence of fp shell configurations at low excitation energy in ^27,28Ne nuclei caused by a vanishing N=20 shell gap at Z=10.     

Photodynamic release of fullerenes from within carbon nanohorn

We have found that oxidized single-wall carbon nanohorns (SWNHox) can exhibit a near-infrared (NIR) laser-triggered accelerated release of encapsulated fullerenes (C₆₀) from within their inner nanospaces. After the NIR laser irradiation of an aqueous SWNHox encapsulating C₆₀ solution/toluene biphasic system, C₆₀ molecules are enriched in the toluene phase. NIR laser-driven SWNHs encapsulating substrates could initiate the development of a new range of drug-delivery systems.     

In Vivo Remote Control of Reactions in Caenorhabditis elegans by Using Supramolecular Nanohybrids of Carbon Nanotubes and Liposomes

A supramolecular nanohybrid based on carbon nanotubes and liposomes that is highly biocompatible and capable of permeation through cells is described. The nanohybrid can be loaded with a variety of functional molecules and is structurally controlled by near‐infrared laser irradiation for the release of molecules from the nanohybrids in a targeted manner via microscopy. We implemented the controlled release of molecules from the nanohybrids and demonstrated remote regulation of the photoinduced nanohybrid functions. As a proof of principle, nanohybrids loaded with amiloride were successfully used in the spatiotemporally targeted blocking of amiloride‐sensitive mechanosensory neurons in living Caenorhabditis elegans. Our prototype could inspire new designs for biomimetic parasitism and symbiosis, and biologically active nanorobots for the higher‐level manipulation of organisms.     

Photoemission results of intermetallic superconductors: Nb3Al and MgB2

We study the superconducting electronic structures of Nb₃Al and MgB₂ using high-resolution spectroscopy. The obtained spectrum of Nb₃Al measured below T_c shows clear opening of the superconducting gap with a sharp pile up in the density of states and a shift of the leading edge. In addition, the spectrum shows a peak-dip-hump line shape expected from the strong-coupling theory. On the other hand, for MgB₂, the superconducting-state spectrum measured at 5.4 K shows a coherent peak with a shoulder structure, in sharp contrast to that expected from a single isotropic gap. The superconducting spectral shape of MgB₂ can be explained in terms of a multicomponent gap.     

Spectroscopic study of neutron shell closures via nucleon transfer in the near-dripline nucleus 23O

Neutron single particle energies have been measured in 23O using the 22O(d,p)23O*-->22O+n process. The energies of the resonant states have been deduced to be 4.00(2) MeV and 5.30(4) MeV. The first excited state can be assigned to the nu d3/2 single particle state from a comparison with shell model calculations. The measured 4.0 MeV energy difference between the nu s1/2 and nu d3/2 states gives the size of the N=16 shell gap which is in agreement with the recent USD05 ("universal" sd from 2005) shell model calculation, and is large enough to explain the unbound nature of the oxygen isotopes heavier than A=24. The resonance detected at 5.3 MeV can be assigned to a state out of the sd shell model space. Its energy corresponds to a approximately 1.3 MeV sized N=20 shell gap, therefore, the N=20 shell closure disappears at Z=8 in agreement with Monte Carlo shell model calculations using SDPF-M interaction.