Enhanced d(d,p)t fusion reaction in metals

被引:0
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作者
F. Raiola
B. Burchard
Zs. Fülöp
Gy. Gyürky
S. Zeng
J. Cruz
A. Di Leva
B. Limata
M. Fonseca
H. Luis
M. Aliotta
H. W. Becker
C. Broggini
A. D'Onofrio
L. Gialanella
G. Imbriani
A. P. Jesus
M. Junker
J. P. Ribeiro
V. Roca
C. Rolfs
M. Romano
E. Somorjai
F. Strieder
F. Terrasi
机构
[1] Ruhr-Universität Bochum,Institut für Physik mit Ionenstrahlen
[2] Atomki,Centro de Fisica Nuclear
[3] China Institute of Atomic Energy,School of Physics
[4] Universidade de Lisboa,Dipartimento di Scienze Ambientali
[5] University of Edinburgh,Dipartimento di Scienze Fisiche
[6] Seconda Università di Napoli,Sezione di Padova
[7] Università Federico II and INFN,undefined
[8] Laboratori Nazionali del Gran Sasso dell'INFN,undefined
[9] INFN,undefined
关键词
25.10.+s Nuclear reactions involving few-nucleon systems; 95.30.-k Fundamental aspects of astrophysics; 25.45.-z ; H-induced reactions;
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摘要
The electron screening in the d(d,p)t reaction has been studied for the deuterated metal Pt at a target temperature \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath T = 20 ^{\circ}$\end{document}C to \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath 340 ^{\circ}$\end{document}C, and for Co at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath T = 20 ^{\circ}$\end{document}C and \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath 200 ^{\circ}$\end{document}C. The enhanced electron screening decreases with increasing temperature, where the data agree with the plasma model of Debye applied to the quasi-free metallic electrons. The data represent the first observation of a temperature dependence of a nuclear cross-section. We also measured the screening effect for the deuterated metal Ti (an element of group 4 of the periodic table) at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath T = -10 ^{\circ}$\end{document}C to \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath 200 ^{\circ}$\end{document}C: above \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath 50 ^{\circ}$\end{document}C the hydrogen solubility dropped to values far below unity and a large screening effect became observable. Similarly, all metals of groups 3 and 4 and the lanthanides showed a solubility of a few percent at \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath T = 200 ^{\circ}$\end{document}C (compared to \documentclass[12pt]{minimal} \usepackage{amsmath} \usepackage{wasysym} \usepackage{amsfonts} \usepackage{amssymb} \usepackage{amsbsy} \usepackage{mathrsfs} \usepackage{upgreek} \setlength{\oddsidemargin}{-69pt} \begin{document}$\ensuremath T = 20 ^{\circ}$\end{document}C) and a large screening became also observable. Within the Debye model the deduced number of valence electrons per metallic atom agrees with the corresponding number from the Hall coefficient, for all metals investigated.
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页码:79 / 82
页数:3
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