TY - JOUR
T1 - 155Gd-Mössbauer studies of the T′-, T*- and T-phases of La2-x-yGdxSryCuO4
AU - Müther, Markus
AU - Wortmann, Gerhard
AU - Felner, Israel
AU - Nowik, Israel
PY - 1993/5/1
Y1 - 1993/5/1
N2 - 155Gd-Mössbauer studies determining the electric and magnetic hyperfine interactions reveal the location and magnetic properties of the Gd ions in the three possible phases of La2-x-yGdxSryCuO4. In T′ -phase Gd2CuO4, the Gd ions are located in lower local point symmetry than expected from the tetragonal structure, order at TN = 6.65 K and interact with the weak ferromagnetic component of the Cu sublattice. The Gd magnetic moments are oriented at an angle of 45° relative to the crystallographic c-axis. The analysis of the temperature dependence of the observed hyperfine fields reveals a zero-field splitting of the Gd S 7 2 ground state. In the superconducting T-phase of La1.775Gd0.075Sr0.15CuO4, Gd is paramagnetic and the Mössbauer spectra exhibit a large quadrupole splitting of 4.2 mm/s, reflecting the different oxygen surrounding in comparison to the T′-phase (1.39 mm/s). The T*-phase, LaGd0.85Sr0.15CuO4, exhibits below 4 K a dominant subspectrum of magnetically ordered Gd ions at M′ sites (eight-fold oxygen coordination) with hyperfine parameters similar to the T′-phase and minority sites with larger quadrupole splittings and paramagnetic behaviour.
AB - 155Gd-Mössbauer studies determining the electric and magnetic hyperfine interactions reveal the location and magnetic properties of the Gd ions in the three possible phases of La2-x-yGdxSryCuO4. In T′ -phase Gd2CuO4, the Gd ions are located in lower local point symmetry than expected from the tetragonal structure, order at TN = 6.65 K and interact with the weak ferromagnetic component of the Cu sublattice. The Gd magnetic moments are oriented at an angle of 45° relative to the crystallographic c-axis. The analysis of the temperature dependence of the observed hyperfine fields reveals a zero-field splitting of the Gd S 7 2 ground state. In the superconducting T-phase of La1.775Gd0.075Sr0.15CuO4, Gd is paramagnetic and the Mössbauer spectra exhibit a large quadrupole splitting of 4.2 mm/s, reflecting the different oxygen surrounding in comparison to the T′-phase (1.39 mm/s). The T*-phase, LaGd0.85Sr0.15CuO4, exhibits below 4 K a dominant subspectrum of magnetically ordered Gd ions at M′ sites (eight-fold oxygen coordination) with hyperfine parameters similar to the T′-phase and minority sites with larger quadrupole splittings and paramagnetic behaviour.
UR - http://www.scopus.com/inward/record.url?scp=0027595164&partnerID=8YFLogxK
U2 - 10.1016/0921-4534(93)90556-6
DO - 10.1016/0921-4534(93)90556-6
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AN - SCOPUS:0027595164
SN - 0921-4534
VL - 209
SP - 428
EP - 436
JO - Physica C: Superconductivity and its Applications
JF - Physica C: Superconductivity and its Applications
IS - 4
ER -