Magnetism between 0.90 and 300 k and complete ligand field theory for chromocene and cobaltoceneE. König; R. Schnakig; S. Kremer; B. Kanellakopulos; R. Klenze · 1978

Matrix elements for configuratuin d5 in weak octahedral field using Bacah methods—A correctionE. König; S. Kremer; R. Schnakig · 1974

Magnetism down to 0.90 K, zero-field splitting, and the ligand field in chromoceneE. König; R. Schnakig; B. Kanellakopulos; R. Klenze · 1977

Zero-field splitting of Mn2+ ions in tetragonal and rhombic symmetry. The effect of excited state contributionsE. König; R. Schnakig · 1975

Thermally induced incomplete high-spin (5T2) ⇌ low-spin (1AJ) transition in dithiocy anatobis (n-phenyl-2-pyridinaldimine) iron (II)E. König; G. Ritter; R. Schnakig · 1974

Theory of spin triplet ground states in d6 transition metal compounds of D4h and D3d symmetries. I. Ground state boundary delineationE. König; R. Schnakig · 1973

The high-spin(5T2) ⇌ low-spin(1A1) transition in oxalatobis(1,10-phenanthroline)iron(II) pentahydrate and the significance of lattice waterE. König; R. Schnakig; G. Ritter; W. Irler; B. Kanellakopulos; B. Powietzka · 1979

Theory of spin triplet ground states ind6transition metal compounds and the effect of high-energy states on the nature of the ground stateE. König; R. Schnakig · 1973