Spin singlet and spin triplet pairing correlations on shape evolution in s d -shell N = Z Nuclei
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[1] M. Cheoun,et al. A study of Gamow-Teller transitions for N = Z nuclei, 24Mg, 28Si, and 32S, by a deformed QRPA , 2017 .
[2] M. Cheoun,et al. Effects of deformation and neutron-proton pairing on the Gamow-Teller transitions for Mg-24,Mg-26 in a deformed quasiparticle random-phase approximation , 2016 .
[3] H. Sagawa,et al. Effect of isoscalar spin-triplet pairings on spin-isospin responses in s d -shell nuclei , 2016, 1607.05881.
[4] Kenichi Yoshida,et al. Effect of ground-state deformation on isoscalar giant resonances in Si 28 , 2016 .
[5] A. Gezerlis,et al. Probing mixed-spin pairing in heavy nuclei , 2015, 1509.04295.
[6] H. Sagawa,et al. Isovector spin-singlet (T = 1, S = 0) and isoscalar spin-triplet (T = 0, S = 1) pairing interactions and spin-isospin response , 2015, 1512.07589.
[7] F. Šimkovic,et al. Brueckner G -matrix approach for neutron-proton pairing correlations in the deformed BCS approach , 2015 .
[8] Y. Yamada,et al. Nonquenched Isoscalar Spin-M1 Excitations in sd-Shell Nuclei. , 2015, Physical review letters.
[9] H. Sagawa,et al. Nuclear ground-state masses and deformations: FRDM(2012) , 2015, 1508.06294.
[10] M. Cheoun,et al. Gamow–Teller strength distributions in 76Ge, 76,82Se, and 90,92Zr by the deformed proton–neutron QRPA , 2015 .
[11] D. Lacroix,et al. Deformation effects on the coexistence between neutron-proton and particle like pairing in N=Z medium mass nuclei , 2014, 1411.1891.
[12] Kenichi Yoshida. Proton-neutron pairing vibrations in N = Z nuclei: Precursory soft mode of isoscalar pairing condensation , 2014, 1409.4884.
[13] A. Macchiavelli,et al. Overview of neutron-proton pairing , 2014, 1405.1652.
[14] Balraj Singh,et al. Tables of E2 transition probabilities from the first 2+ states in even–even nuclei , 2013, 1312.5975.
[15] M. Cheoun,et al. Shell evolution of N=20 nuclei and Gamow-Teller strengths of 30,32,34 Mg with deformed quasiparticle random-phase approximation , 2013 .
[16] H. Sagawa,et al. Role of T=0 pairing in Gamow–Teller states in N=Z nuclei , 2012, 1211.4920.
[17] G. Bertsch,et al. Mixed-spin pairing condensates in heavy nuclei. , 2011, Physical review letters.
[18] B. Pritychenko,et al. An update of the B(E2) evaluation for 01+→21+ transitions in even–even nuclei near N∼Z∼28 , 2011, 1102.3365.
[19] K. Hagino,et al. Shape of {Lambda} hypernuclei in the ({beta},{gamma}) deformation plane , 2010, 1010.5561.
[20] K. Hagino,et al. Deformation of Λ hypernuclei , 2008, 0808.3303.
[21] H. Sagawa,et al. Evolution of deformations in medium-mass nuclei , 2005, nucl-th/0510086.
[22] N. Stone. Table of Nuclear Magnetic Dipole and Electric Quadrupole Moments , 2005 .
[23] F. Šimkovic,et al. Proton-neutron pairing in the deformed BCS approach , 2003, nucl-th/0308046.
[24] P. Reinhard,et al. Pairing gaps from nuclear mean-fieldmo dels , 2000, nucl-th/0005028.
[25] P. Ring,et al. GROUND-STATE PROPERTIES OF EVEN–EVEN NUCLEI IN THE RELATIVISTIC MEAN-FIELD THEORY☆ , 1999 .
[26] A. Goodman. T=0 and T=1 pair correlations in N=Z medium-mass nuclei , 1998 .
[27] Y. K. Gambhir,et al. Computer program for the relativistic mean field description of the ground state properties of even-even axially deformed nuclei , 1997, nucl-th/9710052.
[28] P. Vogel,et al. Neutron-proton pairing in the BCS approach , 1997, nucl-th/9702047.
[29] M. Stoitsov,et al. Neutron-proton correlations in an exactly solvable model , 1996, nucl-th/9610045.
[30] R. Wyss,et al. Competition between T = 0 and T = 1 pairing in proton-rich nuclei , 1996, nucl-th/9608041.
[31] N. Teruya,et al. BCS self-energy term and the 11Li , 1996 .
[32] P. Vogel,et al. Pairing and isospin symmetry in proton-rich nuclei , 1996, nucl-th/9605019.
[33] Faessler,et al. Neutrinoless double beta decay within the quasiparticle random-phase approximation with proton-neutron pairing. , 1996, Physical review. C, Nuclear physics.
[34] F. Šimkovic,et al. Total Gamow-Teller strength, ground-state correlations and sum rules in QRPA with neutron-proton pairing , 1995 .
[35] F. Šimkovic,et al. Two-neutrino double-beta decay in coupled QRPA with neutron-proton pairing , 1993 .
[36] F. Šimkovic,et al. Neutron-proton pairing in light nuclei and two-neutrino double-beta decay , 1993 .
[37] P. Tikkanen,et al. TRANSITION PROBABILITY FROM THE GROUND TO THE FIRST-EXCITED 2+ STATE OF EVEN–EVEN NUCLIDES , 2001 .
[38] I. Towner. Quenching of spin matrix elements in nuclei , 1987 .
[39] Witold Nazarewicz,et al. Single-particle energies, wave functions, quadrupole moments and g-factors in an axially deformed woods-saxon potential with applications to the two-centre-type nuclear problems , 1987 .
[40] R. Nojarov. Parameters of a cylindrical Woods-Saxon potential for the rare-earth region , 1984 .
[41] A. Arima. Nuclear magnetic properties and gamow-teller transitions , 1984 .
[42] R. Spear. Static quadrupole moments of first 2 + states in the 2s1d shell: A review of experiment and theory , 1981 .
[43] A. Faessler,et al. T = 0 proton-neutron pairing correlation in N ≠ Z light nuclei , 1970 .
[44] V. Strutinsky,et al. A method for solving the independent-particle Schrödinger equation with a deformed average field , 1969 .
[45] A. Goswami,et al. Generalized treatment of neutron-proton pairing in N = Z nuclei , 1967 .