Thorium-229 is a unique case in nuclear physics: it presents a metastable first excited state 229m Th, just a few electronvolts above the nuclear ground state. This so-called isomer is accessible by VUV lasers, which allows transferring the amazing precision of atomic laser spectroscopy to nuclear physics. Being able to manipulate the 229 Th nuclear states at will opens up a multitude of prospects, from studies of the fundamental interactions in physics to applications as a compact and robust nuclear clock. However, direct optical excitation of the isomer or its radiative decay back to the ground state has not yet been observed, and a series of key nuclear structure parameters such as the exact energies and half-lives of the low-lying nuclear levels of 229 Th are yet unknown. Here we present the first active optical pumping into 229m Th. Our scheme employs narrow-band 29 keV synchrotron radiation to resonantly excite the second excited state, which then predominantly decays into the isomer. We determine the resonance energy with 0.07 eV accuracy, measure a half-life of 82.2 ps, an excitation linewidth of 1.70 neV, and extract the branching ratio of the second excited state into the ground and isomeric state respectively. These measurements allow us to re-evaluate gamma spectroscopy data that have been collected over 40 years.
The 12 C excitation energy spectra populated in both proton and α-particle inelastic scattering measurements are examined. The data indicate the existence of a 2 + state at Ex=9.75(0.15) MeV with a width of 750(150) keV. It is believed that this state corresponds to the 2 + excitation of the 7.65 MeV, 0 + , Hoyle-state, which acts as the main path by which carbon is synthesised in stars. A simultaneous R-matrix analysis of the two sets of data indicates that the 2 + state possesses a very large α-reduced width, approaching the Wigner limit. This would indicate that the state is associated with a highly clustered structure. The potential geometric arrangements of the clusters is discussed.
We investigated the effect of polymer composition on nifedipine (NIF) dissolution through molecular-level characterization of NIF/hypromellose (HPMC)/Eudragit S (EUD-S) ternary solid dispersions. The dissolution rates and molecular states of NIF and polymers were evaluated in NIF/HPMC/EUD-S spray-dried samples (SPDs) with different polymer compositions. Blending of HPMC and EUD-S improved the dissolution property of each polymer. Moreover, polymer blending enhanced NIF dissolution from the NIF/polymer SPD with EUD-S/polymer wt % of 50-75%. NIF dissolved simultaneously with polymers from the NIF/polymer SPDs with high EUD-S/polymer wt %. In contrast, NIF and polymers separately dissolved from the NIF/polymer SPDs with EUD-S/polymer wt % of 10-25%, exhibiting a significantly reduced NIF dissolution rate. Fourier transform-infrared and solid-state NMR measurements revealed that HPMC and EUD-S formed molecular interactions with NIF via different interaction modes. Comprehensive analysis by spectroscopic measurements and modulated differential scanning calorimetry showed that the molecular interaction between NIF and EUD-S was stronger than that between NIF and HPMC. Furthermore, the C-spin-lattice relaxation time measurements revealed that EUD-S effectively restricted the molecular mobility of NIF compared with HPMC. The molecular interaction between NIF and EUD-S led to the simultaneous and fast dissolution of NIF with EUD-S from the NIF/polymer SPD with high EUD-S loading. Thus, enhanced NIF dissolution was ascribed to the fast dissolution properties of the blended polymer and to polymer-controlled NIF dissolution through the strong molecular interaction between NIF and EUD-S. To achieve efficient optimization of the formulation of polymer-blended solid dispersion with desired drug dissolution, it is necessary to consider both polymer-polymer and drug-polymer intermolecular interactions.
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