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Mathematical modelling of the structure and function of the lymphatic system

Crystal field simulation and NMR study of 19F in a EuF3 Van Vleck paramagnet of 19F nuclei is measured for a powder sample of a EuF3 Van Vleck paramagnet, in a broad temperature

Observation of magnetic coupling between the nuclei of liquid 3He and the 141Pr nuclei of PrF3 crystalline powderThe resonance magnetic coupling between the nuclei of liquid 3He and the 141Pr nuclei of a fine

Crystal field simulation and NMR study of 19F in a EuF3 Van Vleck paramagnet of 19F nuclei is measured for a powder sample of a EuF3 Van Vleck paramagnet, in a broad temperature

Phase diagram of YBa2Cu3O7-y at T < Tc according to transverse nuclear relaxation data for Cu(2)2Cu3O7-y. A comparison of the relaxation rates for isotopes 63Cu(2) and 65Cu(2) at T= 47 K indicates

Temperature dependence of the Cu(2) NQR line width in YBa2Cu3O7 - y behavior of the superconducting gap. The observed dependence is explained by the fact that the energy of a

Dynamics and distribution of doped holes in the CuO2 plane of slightly doped Y1-y CayBa2Cu3O 6 studied by Cu(1) NQR) and longitudinal (1/ T1) relaxation rates of the NQR are found at low temperature, which allows us to determine a

NMR, high frequency EPR and magnetization studies of YF 3:Tm 3+ and TmF 3-frequency EPR and dc-magnetometry. It is shown that TmF 3 is a Van Vleck paramagnet. Zero field splitting

Magnetic properties of powders LiTbF4 and TbF3

Magnetic properties of Dy 3+ ions and crystal field characterization in YF 3:Dy 3+and DyF 3 single crystals

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