Pion transfer processes of pionic atoms in the gas mixtures containing hydrogen at various pressures

2001 ◽  
Vol 89 (11-12) ◽  
Author(s):  
Atsushi Shinohara ◽  
T. Miura ◽  
Akihiko Yokoyama ◽  
K. Takamiya ◽  
T. Kaneko ◽  
...  

The pion capture process in gas mixtures containing hydrogen was studied by measuring pionic X rays and π

1983 ◽  
Vol 217 (1-2) ◽  
pp. 282-284 ◽  
Author(s):  
Marja-Leena Järvinen ◽  
Heikki Sipilä

1993 ◽  
Vol 11 (1) ◽  
pp. 89-96 ◽  
Author(s):  
H. Nishimura ◽  
H. Shiraga ◽  
T. Endo ◽  
H. Takabe ◽  
M. Katayama ◽  
...  

In the last few years, systematic studies on radiation hydrodynamics in the X-ray confining cavity and a fuel capsule have attained remarkable progress. This makes it possible to analyze quantitatively the energy transfer processes from laser to the fusion capsule and find uniform irradiation conditions of the fusion capsule driven by thermal X rays. As a result, reproducible and stable implosions were achieved. Throughout implosion experiments with the Gekko XII blue laser system (351 nm, kJ, 0.8 ns), good agreement of implosion has been obtained between the experiment and numerical simulations, assuming perfectly spherical symmetry, up to a radial convergence ratio of 15. Described are particularly the issues of (1) energy transfer processes from laser to a fuel capsule and conditions for uniform irradiation, (2) properties of the X-ray propagation through aluminum heated by X-ray radiation, and (3) dependence of the convergence ratio of Ri/Rf (where Ri and Rf are the initial and final radii) of the capsule on the initial fill pressure of D–T gas and its influence on the core parameters and fusion products to evaluate implosion sphericity.


2001 ◽  
Vol 89 (12) ◽  
pp. 8202-8213 ◽  
Author(s):  
F. P. Santos ◽  
T. H. V. T. Dias ◽  
P. J. B. M. Rachinhas ◽  
C. A. N. Conde ◽  
A. D. Stauffer

2021 ◽  
Vol 118 (26) ◽  
pp. e2103971118
Author(s):  
Alexander H. Bork ◽  
Margarita Rekhtina ◽  
Elena Willinger ◽  
Pedro Castro-Fernández ◽  
Jakub Drnec ◽  
...  

The addition of molten alkali metal salts drastically accelerates the kinetics of CO2 capture by MgO through the formation of MgCO3. However, the growth mechanism, the nature of MgCO3 formation, and the exact role of the molten alkali metal salts on the CO2 capture process remain elusive, holding back the development of more-effective MgO-based CO2 sorbents. Here, we unveil the growth mechanism of MgCO3 under practically relevant conditions using a well-defined, yet representative, model system that is a MgO(100) single crystal coated with NaNO3. The model system is interrogated by in situ X-ray reflectometry coupled with grazing incidence X-ray diffraction, scanning electron microscopy, and high-resolution transmission electron microscopy. When bare MgO(100) is exposed to a flow of CO2, a noncrystalline surface carbonate layer of ca. 7-Å thickness forms. In contrast, when MgO(100) is coated with NaNO3, MgCO3 crystals nucleate and grow. These crystals have a preferential orientation with respect to the MgO(100) substrate, and form at the interface between MgO(100) and the molten NaNO3. MgCO3 grows epitaxially with respect to MgO(100), and the lattice mismatch between MgCO3 and MgO is relaxed through lattice misfit dislocations. Pyramid-shaped pits on the surface of MgO, in proximity to and below the MgCO3 crystals, point to the etching of surface MgO, providing dissolved [Mg2+…O2–] ionic pairs for MgCO3 growth. Our studies highlight the importance of combining X-rays and electron microscopy techniques to provide atomic to micrometer scale insight into the changes occurring at complex interfaces under reactive conditions.


2020 ◽  
Vol 135 (10) ◽  
Author(s):  
A. Knecht ◽  
A. Skawran ◽  
S. M. Vogiatzi

AbstractMuons are a fascinating probe to study nuclear properties. Muonic atoms can easily be formed by stopping negative muons inside a material. The muon is subsequently captured by the nucleus and, due to its much higher mass compared to the electron, orbits the nucleus at very small distances. During this atomic capture process, the muon emits characteristic X-rays during its cascade down to the ground state. The energies of these X-rays reveal the muonic energy level scheme, from which properties like the nuclear charge radius or its quadrupole moment can be extracted. While almost all stable elements have been examined using muons, probing highly radioactive atoms has so far not been possible. The muX experiment has developed a technique based on transfer reaction inside a high-pressure hydrogen/deuterium gas cell to examine targets available only in microgram quantities.


Author(s):  
Nobutsugu Imanishi ◽  
Yuka Takeuchi ◽  
Katsuya Toyoda ◽  
Atsushi Shinohara ◽  
Yoshio Yoshimura
Keyword(s):  

2005 ◽  
Vol 93 (9-10) ◽  
Author(s):  
Kazuhiko Ninomiya ◽  
Hironori Sugiura ◽  
Yoshitaka Kasamatsu ◽  
Hidetoshi Kikunaga ◽  
Koichi Takamiya ◽  
...  
Keyword(s):  
X Rays ◽  

SummaryThe electronic


2021 ◽  
Author(s):  
Alexander Hansen Bork ◽  
Margarita Rekhtina ◽  
Elena Willinger ◽  
Pedro Castro-Fernández ◽  
Jakub Drnec ◽  
...  

<p>The addition of molten alkali metal salts drastically accelerates the kinetics of CO<sub>2</sub> capture by MgO through the formation of MgCO<sub>3</sub>. However, the growth mechanism, the nature of MgCO<sub>3</sub> formation and the exact role of the molten alkali metal salts on the CO2 capture process remains elusive, holding back the development of more effective MgO-based CO<sub>2</sub> sorbents. Here, we unveil the growth mechanism of MgCO<sub>3</sub> under practically relevant conditions using a well-defined, yet representative, model system that is a MgO(100) single crystal coated with NaNO<sub>3</sub>. The model system is interrogated by in situ X-ray reflectometry coupled with grazing incidence X-ray diffraction, scanning electron microscopy and high-resolution transmission electron microscopy. When bare MgO(100) is exposed to a flow of CO<sub>2</sub>, a non-crystalline surface carbonate layer of ca. 7 Å thickness forms. In contrast, when MgO(100) is coated with NaNO<sub>3</sub> MgCO<sub>3</sub> crystals nucleate and growth. These crystals have a preferential orientation with respect to the MgO(100) substrate, and form at the interface between MgO(100) and the molten NaNO<sub>3</sub>. MgCO<sub>3</sub> grows epitaxially with respect to MgO(100) and the lattice mismatch between MgCO<sub>3</sub> and MgO is relaxed through lattice misfit dislocations. Pyramid shaped pits on the surface of MgO, in the proximity and below the MgCO<sub>3</sub> crystals, point to the etching of surface MgO, providing dissolved [Mg<sup>2+</sup>…O<sup>2–</sup>] ionic pairs for MgCO<sub>3</sub> growth. Our studies highlight the importance of combining X-rays and electron microscopy techniques to provide atomic to micrometer scale insight into the changes occurring at complex interfaces under reactive conditions.</p>


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