2014
DOI: 10.1103/physrevlett.113.042501
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First Direct Measurement of theH2(α,γ)Li

Abstract: Recent observations of (6)Li in metal poor stars suggest a large production of this isotope during big bang nucleosynthesis (BBN). In standard BBN calculations, the (2)H(α,γ)(6)Li reaction dominates (6)Li production. This reaction has never been measured inside the BBN energy region because its cross section drops exponentially at low energy and because the electric dipole transition is strongly suppressed for the isoscalar particles (2)H and α at energies below the Coulomb barrier. Indirect measurements using… Show more

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Cited by 105 publications
(122 citation statements)
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References 33 publications
(85 reference statements)
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“…The 2 H( α, γ ) 6 Li cross section has never been directly measured in the BBN region of interest (30 ࣠ E ࣠ 300 keV), before the LUNA data first reported in [5] . It is worth nothing, only one attempt to directly measure the 2 H( α, γ ) 6 Li cross section at low energy is reported in literature, providing only an upper limit [17] .…”
Section: The Nuclear Physics Of Primordial 6 LImentioning
confidence: 99%
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“…The 2 H( α, γ ) 6 Li cross section has never been directly measured in the BBN region of interest (30 ࣠ E ࣠ 300 keV), before the LUNA data first reported in [5] . It is worth nothing, only one attempt to directly measure the 2 H( α, γ ) 6 Li cross section at low energy is reported in literature, providing only an upper limit [17] .…”
Section: The Nuclear Physics Of Primordial 6 LImentioning
confidence: 99%
“…(4) is below the calorimeter. The pressure is kept constant by means of a feedback system controlled by a pressure gauge (5). The γ -rays produced by the 2 H( α, γ ) 6 Li reaction are detected by a HPGe detector (6).…”
Section: The Nuclear Physics Of Primordial 6 LImentioning
confidence: 99%
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“…A few years ago, observations [40] of 6 Li in a few metal poor stars had suggested the presence of a plateau, at typically 6 Li/H ≈ 10 −11 , orders of magnitude higher than the BBN predictions of 6 Li/H ≈ 1.3×10 −14 [41]. The uncertainties on the D(α, γ) 6 Li cross section have been experimentally constraint by a LUNA measurement [42] and by theory [43] confirming the BBN value. However, later, the observational 6 Li plateau has been questioned due to line asymmetries which were neglected in previous abundance analyses.…”
Section: Discussionmentioning
confidence: 72%
“…The accelerated deuterium particles, after Rutherford scattering with the α-beam, interact with the gas itself producing the two reactions: 2 H(d,n) 3 He and 2 H(d,p) 3 H. In particular, the neutrons emitted by the 2 H(d,n) 3 He were responsible for a high beam induced background in the γ-spectrum. A long and detailed study of this background was required in order to perform the analysis of the data [58][59][60].…”
Section: Big Bang Nucleosynthesismentioning
confidence: 99%