Electron magnetic resonance (EMR) of the spin S≥1 systems: an overview of major intricacies awaiting unwary spectroscopists

[1]  C. Rudowicz,et al.  Can the electron magnetic resonance (EMR) techniques measure the crystal (ligand) field parameters , 2001 .

[2]  C. Rudowicz,et al.  On the non-standard rhombic spin Hamiltonian parameters derived from Mössbauer spectroscopy and magnetism-related measurements , 2001 .

[3]  C. Rudowicz.  Comment on “Analytical expressions for zero-field splittings of3d5ions in low-symmetry fields and their applications” , 2001 .

[4]  C. Rudowicz,et al.  SPIN-HAMILTONIAN FORMALISMS IN ELECTRON MAGNETIC RESONANCE (EMR) AND RELATED SPECTROSCOPIES , 2001 .

[5]  C. Rudowicz.  LETTER TO THE EDITOR: On the relations between the zero-field splitting parameters in the extended Stevens operator notation and the conventional ones used in EMR for orthorhombic and lower symmetry , 2000 .

[6]  C. Rudowicz,et al.  Monoclinic and orthorhombic standardization of spin-Hamiltonian parameters for rare-earth centers in various crystals , 2000 .

[7]  C. Rudowicz,et al.  Orthorhombic standardization of spin-Hamiltonian parameters for transition-metal centres in various crystals , 1999 .

[8]  R. Chatterjee,et al.  The analysis of EPR spectra using tesseral tensor angular momentum operators , 1998 .

[9]  J. Baker,et al.  Superposition model analysis of in sodium ammonium sulphate dihydrate , 1998 .

[10]  M. G. Zhao,et al.  g-factor formulas of 3d 5 ions in trigonal-symmetry fields and their applications , 1997 .

[11]  T. Yeom,et al.  Monoclinic Spin Hamiltonian Analysis of EPR Spectra of Mn2+ in BiVO4 Single Crystals , 1996 .

[12]  Zhao,et al.  Analytical expressions for zero-field splittings of 3d5 ions in low-symmetry fields and their applications. , 1995, Physical review. B, Condensed matter.

[13]  J. Baker,et al.  Studies of chromium-doped sodium ammonium sulphate dihydrate: I. Electron paramagnetic resonance of Cr3+ , 1995 .

[14]  C. Rudowicz,et al.  Zeeman and zero-field splitting of 3d4 and 3d6 ions with orbital singlet ground state at orthorhombic and tetragonal symmetry sites , 1994 .

[15]  R. Bartram,et al.  Structural Analysis of Point Defects in Solids , 1992 .

[16]  C. Rudowicz,et al.  Effect of Monoclinic Symmetry on the EPR Spectra of Gd3+‐Doped Hydrated Single Crystals of Rare‐Earth Trichlorides , 1988 .

[17]  D. McGavin.  Symmetry constraints on EPR spin-Hamiltonian parameters , 1987 .

[18]  C. Rudowicz,et al.  On the possible presence of odd-order terms in a magnetic resonance spin Hamiltonian for S-state ions , 1987 .

[19]  C. Rudowicz.  On standardization and algebraic symmetry of the ligand field Hamiltonian for rare earth ions at monoclinic symmetry sites , 1986 .

[20]  C. Rudowicz,et al.  On standardization of the spin Hamiltonian and the ligand field Hamiltonian for orthorhombic symmetry , 1985 .

[21]  R. Chatterjee,et al.  The derivation of a symmetry‐adapted generalized spin Hamiltonian , 1985 .

[22]  J. A. Tuszynski,et al.  Point-group discrimination using the c-axis angular variation of the EPR fine-structure spectra for S-state ions , 1985 .

[23]  C. Rudowicz,et al.  Transformation relations for the conventional Okq and normalised O'kq Stevens operator equivalents with k=1 to 6 and -k⩽q⩽k , 1985 .

[24]  K. Stevens.  Matrix Elements and Operator Equivalents Connected with the Magnetic Properties of Rare Earth Ions , 1952 .