Nucleonic versus nuclear spin-isospin polarization: A study of the 48Ca and 88Sr M1 form factors
暂无分享,去创建一个
[1] W. Knüpfer,et al. Proton correlations and the missing M1 strength in 48Ca: A two-state model☆ , 1983 .
[2] A. Faessler,et al. The screening of the particle-hole interaction to all orders , 1983 .
[3] A. Richter,et al. Form factor of the M1 transition to the 10.23 MeV state in 48Ca and the role of the Δ(1232) , 1983 .
[4] R. Lawson. The effect of the Δ(1236) on the g-factor of nucleons , 1983 .
[5] F. Khanna,et al. Corrections to the single-particle M1 and Gamow-Teller matrix elements , 1983 .
[6] B. Frois,et al. Radial distribution of nucleons in the isotopes 48,40ca , 1983 .
[7] W. Weaise. Role of the Δ(1232) in nuclear isovector-spin transitions☆ , 1983 .
[8] T. Cheon,et al. Comments on the effect of Δ (1232 MeV)-hole excitation in quenching the gamow-teller matrix element , 1983 .
[9] W. Weise. Chiral bag models and the Lorentz-Lorenz correction , 1982 .
[10] R. Frey,et al. Quenching of the electron scattering form factor of the 1+ state at 3.48 MeV in88Sr and the influence of theΔ(1232)-isobar , 1982 .
[11] H. Toki,et al. Pionic modes of excitation in nuclei , 1982 .
[12] C. Goodman. Gamow-Teller resonances , 1982 .
[13] A. Richter. Inelastic electron scattering at low energy: Magnetic transitions and the magnetic polarizability of nuclei , 1982 .
[14] J. Delorme. MESON DEGREES OF FREEDOM IN NUCLEI , 1982 .
[15] J. Speth,et al. Theory of Giant Resonances , 1982 .
[16] G. Brown,et al. The giant Gamow-Teller resonance , 1981 .
[17] J. Speth,et al. Experimental signatures of the Δ(1236)-hole quenching mechanism in pionic states , 1981 .
[18] E. Sugarbaker,et al. Excitation of giant spin-isospin multipole vibrations , 1981 .
[19] J. Meyer-ter-Vehn,et al. The Quasiparticle Interaction, a Shield of Nuclear Matter Against Pion Condensation , 1981 .
[20] H. Toki,et al. Quenching of magnetic transitions and Δ(1232) degrees of freedom in nuclei: the 48Ca case , 1981 .
[21] J. B. McGrory,et al. Shell-model calculation of M1 scattering strengths in 42,44,48Ca , 1981 .
[22] J. Speth,et al. Critical analysis of a precritical phenomenon in connection with pion condensation , 1981 .
[23] A. Bohr,et al. On the role of the Δ resonance in the effective spin-dependent moments of nuclei , 1981 .
[24] H. Toki,et al. On the mass dependent quenching of magnetic transitions in nuclei , 1980 .
[25] W. Knüpfer,et al. Quenching of the magnetic multipole strength distribution and of the anomalous magnetic moment in complex nuclei and mesonic renormalization of the nuclear spin current , 1980 .
[26] W. Knüpfer,et al. Backward-angle high-resolution inelastic electron scattering on 40, 42, 44, 48Ca and observation of a very strong magnetic dipole ground-state transition in 48Ca , 1980 .
[27] H. Toki,et al. Pionic modes of excitation in nuclei: Inelastic electron and proton scattering to the (1+, T=1; 15.1 MeV) state in 12C , 1980 .
[28] N. Giraud,et al. Critical opalescence of the nuclear pion field: A possible evidence in the M1 (15.11 MeV) form factor of 12C , 1980 .
[29] S.-O. Bäckman,et al. The role of tensor forces in Fermi liquid theory , 1979 .
[30] E. Oset,et al. Axial currents in nuclei: The Gamow-Teller matrix element , 1979 .
[31] F. Khanna,et al. Quenching of Allowed Gamow-Teller β Transitions in Mirror Nuclei , 1979 .
[32] M. Anastasio,et al. Meson exchange and the theory of finite fermi systems , 1977 .
[33] W. Weise. Δ-isobar dynamics in finite nuclei: Pion elastic scattering , 1977 .
[34] M. Wakamatsu,et al. Renormalization of the axial current form factors in nuclei , 1974 .
[35] M. Rho. Quenching of axial-vector coupling constant in β-decay and pion-nucleus optical potential☆ , 1974 .
[36] M. Ericson,et al. Pionic field and renormalization of the axial coupling constant in nuclei , 1973 .
[37] E. Boeker,et al. FBCS for odd nuclei and the inverse gap equations: Application to N = 50 isotones , 1972 .