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Implication of the Proton-Deuteron Radiative Capture for Big Bang Nucleosynthesis

机译:质子-氘核辐射捕获对大爆炸核合成的影响

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The astrophysical S factor for the radiative capture d(p,gamma)He-3 in the energy range of interest for big bang nucleosynthesis (BBN) is calculated using an ab initio approach. The nuclear Hamiltonian retains both two-and three-nucleon interactions-the Argonne v(18) and the Urbana IX, respectively. Both one-and many-body contributions to the nuclear current operator are included. The former retain for the first time, besides the 1/m leading order contribution (m is the nucleon mass), also the next-to-leading order term, proportional to 1/m(3). The many-body currents are constructed in order to satisfy the current conservation relation with the adopted Hamiltonian model. The hyperspherical harmonics technique is applied to solve the A = 3 bound and scattering states. Particular attention is paid in this second case in order to obtain, in the energy range of BBN, an uncertainty on the astrophysical S factor of the order or below similar to 1%. Then, in this energy range, the S factor is found to be similar to 10% larger than the currently adopted values. Part of this increase (1%-3%) is due to the 1/m(3) one-body operator, while the remaining is due to the new more accurate scattering wave functions. We have studied the implication of this new determination for the d(p,gamma)He-3 S factor on the deuterium primordial abundance. We find that the predicted theoretical value for H-2/H is in excellent agreement with its experimental determination, using the most recent determination of the baryon density of the Planck experiment, and with a standard number of relativistic degrees of freedom N-eff = 3.046 during primordial nucleosynthesis. This calls for a more accurate measurement of the astrophysical S factor in order to confirm the present predictions.
机译:使用从头算方法计算大爆炸核合成(BBN)所需能量范围内辐射捕获d(p,γ)He-3的天体S因子。核哈密顿量保留了两个和三个核子相互作用,分别是Argonne v(18)和Urbana IX。包括对核电流运营者的单人和多人捐助。前者第一次保留,除了1 / m的前导贡献(m是核子质量),也是次要的前项,与1 / m成比例(3)。为了满足采用的哈密顿量模型的电流守恒关系,构造了多体电流。应用超球谐技术解决A = 3的束缚态和散射态。在第二种情况下要特别注意,以便在BBN的能量范围内获得天体物理学S因子的不确定度,该不确定度约为1%或更低。然后,在该能量范围内,发现S因子比当前采用的值大10%。这种增加的一部分(1%-3%)归因于1 / m(3)单体算子,而其余部分归因于新的更精确的散射波函数。我们已经研究了d(p,γ)He-3 S因子对氘原始丰度的这一新测定的含义。我们发现,H-2 / H的预测理论值与其实验确定值,使用普朗克实验的重子密度的最新确定值以及相对论自由度的标准数量N-eff =极为吻合。原始核合成期间为3.046。这就需要对天体S因子进行更精确的测量,以确认当前的预测。

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  • 来源
    《Physical review letters》 |2016年第10期|102501.1-102501.5|共5页
  • 作者单位

    Univ Pisa, Dept Phys, Largo B Pontecorvo 3, I-56127 Pisa, Italy|Ist Nazl Fis Nucl, Largo B Pontecorvo 3, I-56127 Pisa, Italy;

    Complesso Univ Monte S Angelo, INFN Napoli, Via Cintia, I-80126 Naples, Italy;

    Ist Nazl Fis Nucl, Largo B Pontecorvo 3, I-56127 Pisa, Italy;

    Ist Nazl Fis Nucl, Largo B Pontecorvo 3, I-56127 Pisa, Italy;

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