2019
DOI: 10.1103/physreva.100.042509
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Application of the Hylleraas- B -spline basis set: Nonrelativistic Bethe logarithm of helium

Abstract: In this work, we report an application of Hylleraas-B-spline basis set to the nonrelativistic Bethe logarithm calculation of helium. The Bethe logarithm for n 1 S, n up to 10, states of helium are calculated with a precision of 7-9 significant digits in two gauges, which greatly improves the accuracy of the traditional B-spline basis set. In addition, to deal with the numerical linear correlation problem in Bethe logarithm calculation, we developed a multiple-precision generalized symmetric eigenvalue problem … Show more

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Cited by 7 publications
(9 citation statements)
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“…is for both the 2 3 S and 3 3 S states. Yang et al [25] have implemented the correlated B-splines to calculate the helium atomic energy level and their non-relativistic ground state energy is −2.903 724 377 1(2) a.u.. A knot distribution optimization was performed for any individual states and present values of energies for the 1 1 S, 2 1 S, 2 3 S and 3 3 S states are listed in Table II. The optimized result of −2.903 724 377 034 0(2) a.u.…”
Section: Resultsmentioning
confidence: 99%
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“…is for both the 2 3 S and 3 3 S states. Yang et al [25] have implemented the correlated B-splines to calculate the helium atomic energy level and their non-relativistic ground state energy is −2.903 724 377 1(2) a.u.. A knot distribution optimization was performed for any individual states and present values of energies for the 1 1 S, 2 1 S, 2 3 S and 3 3 S states are listed in Table II. The optimized result of −2.903 724 377 034 0(2) a.u.…”
Section: Resultsmentioning
confidence: 99%
“…Compared with the relativistic correction, the more difficult to calculate in the leading QED correction are Bethe logarithm and Araki-sucher correction. The Bethe logarithms for the 1 1 S, 2 1 S, 2 3 S and 3 3 S state of the helium atom are summarized in Table I calculated by Zhang et al [22] using traditional Bspline function and Yang et al [26] using the C-BSBF, respectively, which based on the Drake-Goldman's method. The Korobov's results listed in the last column of Table I based on the integral representation method of Schwartz are the benchmarks.…”
Section: B Leading Relativistic and Qed Correctionsmentioning
confidence: 99%
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“…在文献 [108]中, Kor-obov还给出了一个新的计算氦原子里德堡态Bethe logarithm值的近似公式. 近几年, 国内的一些研究者, 如Tang等人 [109] 、Yang等人 [110] 、Zhang等人 [111] [50,86] ; 严格的计算直到 2003年才由Yan和Drake [112] 完成, 他们用Hylleraas坐标 下的赝态方法, 计算了锂原子2S和3S态的Bethe logarithm. 在同一年, Pachucki和Komasa [113] 用ECG计算了 锂原子2S态的Bethe logarithm, 其精度与Yan和Drake的…”
Section: 氦、锂、铍和硼原子领头阶相对论效应的计算 由unclassified