Revalidation of the isobaric multiplet mass equation at A=53, T=3/2
暂无分享,去创建一个
Xiaoping Zhou | Z. Bai | B. Guo | L. Zhang | S. Zeng | Y. Lam | S. Jin | J. Hu | Z. Li | G. Audi | M. Maccormick | J. He | J. Su | N. Zhang | G. Lian | X. Du | L. Gan | Jian-song Wang | P. Ma | S. Ma | S. Z. Chen | B. Ding | Jian-ping Ma | X. X. Bai | S. W. Xu | Y. J. Li | Y. B. Wang | W. H. Ma | N. Smirnova | X. Tang | Weiping Liu | X. Bai | Y. P. Shen | Z. Gao | L. Jing | S. Q. Yan | Y. H. Zhang | Y. Yang | M. Huang | Ye-Ling Zhou | W. Ma | Mei Huang | S. W. Xu | S. Ma | J. Hu | J. He | S. W. Xu | S. Zeng | L. Zhang
[1] Xing Xu,et al. The AME2016 atomic mass evaluation (I). Evaluation of input data; and adjustment procedures , 2017 .
[2] B. A. Brown,et al. REACTION RATES OF 64Ge(p,γ)65As AND 65As(p,γ)66Se AND THE EXTENT OF NUCLEOSYNTHESIS IN TYPE I X-RAY BURSTS , 2015, 1505.02275.
[3] B. A. Brown,et al. Breakdown of the isobaric multiplet mass equation for the A = 20 and 21 multiplets. , 2014, Physical review letters.
[4] B. A. Brown,et al. The Shell-Model Code NuShellX@MSU , 2014 .
[5] A. Tamii,et al. Observation of the β-delayed γ-proton decay of (56)Zn and its impact on the Gamow-Teller strength evaluation. , 2014, Physical review letters.
[6] G. Audi,et al. Evaluated experimental isobaric analogue states from T=1/2 to T=3 and associated IMME coefficients , 2013, 1312.1521.
[7] A. Volya,et al. Split isobaric analog state in 55Ni: case of strong isospin mixing. , 2013, Physical review letters.
[8] A. Tamii,et al. Isospin mixing of the isobaric analog state studied in a high-resolution 56 Fe( 3 He , t ) 56 Co reaction , 2013 .
[9] Y. Lam,et al. The isobaric multiplet mass equation for A≤71A≤71 revisited , 2013, 2109.12956.
[10] M. Smith,et al. Reexamining the Beta Decay of 53,54Ni, 52,53Co, 51Fe, and 50Mn , 2013 .
[11] Mei Wang,et al. The NUBASE2016 evaluation of nuclear properties , 2012 .
[12] Xing Xu,et al. The AME2016 atomic mass evaluation (II). Tables, graphs and references , 2012 .
[13] Y. Lam,et al. Isospin Non-Conservation in $sd$-Shell Nuclei , 2012, 1210.0183.
[14] B. A. Brown,et al. Elucidation of the anomalous A=9 isospin quartet behavior. , 2012, Physical review letters.
[15] A. Saastamoinen,et al. Mass of Al 23 for testing the isobaric multiplet mass equation , 2009 .
[16] D. L. Lincoln,et al. Precision test of the isobaric multiplet mass equation for the A=32, T=2 quintet , 2008 .
[17] B. Blank,et al. Nuclear structure at the proton drip line: Advances with nuclear decay studies , 2008 .
[18] D. Karamanis,et al. The decay of proton-rich nuclei in the mass A=36–56 region , 2007 .
[19] K. Blaum,et al. Evidence for a breakdown of the isobaric multiplet mass equation: A study of the A = 35, T = 3/2 isospin quartet , 2007, 0707.3201.
[20] D. Morrissey,et al. High-precision Penning trap mass measurements of Ca37,38 and their contributions to conserved vector current and isobaric mass multiplet equation , 2007 .
[21] A. Sallaska,et al. Mass of the lowest T=2 state in {sup 32}S: A test of the isobaric multiplet mass equation , 2006 .
[22] B. A. Brown,et al. Shell-model description of neutron-rich pf-shell nuclei with a new effective interaction GXPF 1 , 2005 .
[23] Balraj Singh,et al. Nuclear Data Sheets for A=40☆ , 2004 .
[24] B. A. Brown,et al. New effective interaction for pf-shell nuclei and its implications for the stability of the N = Z = 28 closed core , 2004, nucl-th/0402079.
[25] E. Sauvan,et al. Masses of 32Ar and 33Ar for fundamental tests. , 2003, Physical review letters.
[26] P. Fallon,et al. Anomalous Coulomb matrix elements in the f 7 / 2 shell , 2003 .
[27] W. Zhan,et al. RIBLL, the radioactive ion beam line in Lanzhou , 2003 .
[28] L. D. Knutson,et al. Revalidation of the isobaric multiplet mass equation. , 2002, Physical review letters.
[29] A. Kellerbauer,et al. Breakdown of the isobaric multiplet mass equation at A = 33, T = 3/2. , 2001, Physical review letters.
[30] C. Donzaud,et al. Neutrino absorption efficiency of an 40 Ar detector from the β decay of 40 Ti , 1998 .
[31] Weiping Liu,et al. beta decay of Ti-40 and Ti-41 and implication for solar-neutrino detection , 1998 .
[32] J. Britz,et al. Coefficients of the isobaric mass equation and their correlations with various nuclear parameters , 1998 .
[33] G. Lhersonneau,et al. High-resolution study of the beta decay of 41Ti , 1997 .
[34] W. Ormand,et al. Empirical isospin-nonconserving hamiltonians for shell-model calculations , 1989 .
[35] M. Zisman,et al. Extension of the Tz = −32 beta-delayed proton precursor series to 57Zn☆ , 1976 .
[36] R. Sextro,et al. High-resolution measurements of beta-delayed protons from 37Ca and 41Ti , 1974 .
[37] G. Bertsch,et al. TZ3 term in the isobaric multiplet equation , 1970 .
[38] E. Henley,et al. Simple Model for Corrections to the Isobaric Multiplet Mass Equation , 1969 .
[39] J. Jänecke. The quartic isobaric multiplet mass equation , 1969 .
[40] J. B. French,et al. Stripping Reactions and the Structure of Light and Intermediate Nuclei , 1960 .
[41] S. Weinberg,et al. Electromagnetic Corrections to Isotopic Spin Conservation , 1959 .
[42] W. Heisenberg,et al. On the structure of atomic nuclei , 1932 .