Abstract:The electron screening in the d(d, p)t reaction has been studied for the deuterated metal Pt at a sample temperature T = 20 • C-340 • C and for Co at T = 20 • C and 200 • 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 eleme… Show more
“…The issue of the possible dependence of β-decay and electron-capture (EC) rates of radioactive nuclei on the nature and temperature of the host matrix and environment is a long standing subject [1,2]. Numerous recent experiments have claimed that the half-life of radioactive nuclei embedded in metals would be significantly affected by screening of the electrons in the metal and this effect further be strengthened at low temperatures [3,4,5,6,7]. Several of the most recent articles cite a longer half-life for the EC of 7 Be (0.8 ± 0.2% [8]) and a shorter half-life for the β + -decay of 22 Na (1.2±0.2% [9]), where these nuclides were implanted in the metals Pd and In and cooled to T = 12 K. For the β − -decay of 198 Au in a Au metallic environment the half-life was observed to be longer by 0.4 ± 0.7% at room temperature and by 4.0 ± 0.7% when the metal was cooled to T = 12 K, both compared to the literature value of the half-life [10].…”
“…The issue of the possible dependence of β-decay and electron-capture (EC) rates of radioactive nuclei on the nature and temperature of the host matrix and environment is a long standing subject [1,2]. Numerous recent experiments have claimed that the half-life of radioactive nuclei embedded in metals would be significantly affected by screening of the electrons in the metal and this effect further be strengthened at low temperatures [3,4,5,6,7]. Several of the most recent articles cite a longer half-life for the EC of 7 Be (0.8 ± 0.2% [8]) and a shorter half-life for the β + -decay of 22 Na (1.2±0.2% [9]), where these nuclides were implanted in the metals Pd and In and cooled to T = 12 K. For the β − -decay of 198 Au in a Au metallic environment the half-life was observed to be longer by 0.4 ± 0.7% at room temperature and by 4.0 ± 0.7% when the metal was cooled to T = 12 K, both compared to the literature value of the half-life [10].…”
“…The effect is important in astrophysical scenarios, where almost all nuclear reactions happen at low energies and nuclei are not alone in the stellar plasma. The predicted effect was confirmed experimentally, but its measured magnitude was very often way above predictions [2][3][4][5][6][7][8][9][10][11]. Although the theory predicts an independence of electron screening on the nuclear surroundings, measurements of the same reactions in different environments gave different magnitudes of electron screening.…”
Abstract. Electron screening enhances nuclear reaction cross sections at low energies. We studied the nuclear reaction 1 H( 19 F,αγ) 16 O in inverse kinematics in different solid hydrogen targets. Measured resonance strengths differed by up to a factor of 10 in different targets. We also studied the 2 H(p,γ) 3 He fusion reaction and observed electrons emitted as reaction products instead of γ rays. In this case electron screening greatly enhances internal conversion probability.
Abstract. Nuclear fusion cross-sections considerably higher than corresponding theoretical predictions are observed in low-energy experiments with metal matrix targets and accelerated deuteron beams. The cross-section increment is significantly higher for liquid than for solid targets. We propose that the same two-body correlation entropy used in evaluating the metal melting entropy explains the large liquid-solid difference of the effective screening potential that parameterizes the cross-section increment. This approach is applied to the specific case of the 6 Li(d, α) 4 He reaction, whose measured screening potential liquid-solid difference is (235 ± 63) eV. Cross sections in the two metals with the highest two-body correlation entropy (In and Hg) has not been measured yet: increments of the cross sections in liquid relative to the ones in solid metals are estimated with the same procedure.
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