2005
DOI: 10.1016/j.jpcs.2005.09.089
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Magnetic behavior of a spin-1 dimer: model system for homodinuclear nickel(II) complexes

Abstract: Magnetic behavior of a spin-1 Heisenberg dimer is analysed in dependence on both uniaxial single-ion anisotropy and XXZ exchange anisotropy in a zero-as well as non-zero longitudinal magnetic field. A complete set of eigenfunctions and eigenvalues of the total Hamiltonian is presented together with an exact analytical expression for the Gibbs free energy, longitudinal magnetization, longitudinal and transverse susceptibility. The obtained theoretical results are compared with the relevant experimental data of … Show more

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Cited by 23 publications
(32 citation statements)
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References 75 publications
(23 reference statements)
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“…Intermediate magnetization plateaux were predicted for the Ising spin clusters with the shape of Platonic solids [9], 'star of David' [10] or tetrahedra-based Ising clusters [11], while the magnetization curve of Heisenberg spin clusters was studied with the shape of triangle [12], tetrahedron [13], truncated tetrahedron [14,15], cuboctahedron [16,17], icosidodecahedron [16] and many more [18][19][20][21][22][23]. It is noteworthy that besides the theoretical predictions, the magnetization plateaux were indeed observed in experimental representatives of molecular magnets, for example for linear trimer compound A 3 Cu(PO 4 ) 4 [24], cubane-based compounds [25], or homodinuclear nickel complexes [26,27].…”
Section: Introductionmentioning
confidence: 90%
“…Intermediate magnetization plateaux were predicted for the Ising spin clusters with the shape of Platonic solids [9], 'star of David' [10] or tetrahedra-based Ising clusters [11], while the magnetization curve of Heisenberg spin clusters was studied with the shape of triangle [12], tetrahedron [13], truncated tetrahedron [14,15], cuboctahedron [16,17], icosidodecahedron [16] and many more [18][19][20][21][22][23]. It is noteworthy that besides the theoretical predictions, the magnetization plateaux were indeed observed in experimental representatives of molecular magnets, for example for linear trimer compound A 3 Cu(PO 4 ) 4 [24], cubane-based compounds [25], or homodinuclear nickel complexes [26,27].…”
Section: Introductionmentioning
confidence: 90%
“…Finally, the Zeeman’s term accounts for the effect of the external magnetic field B ( is the Bohr magneton and g is the Landé g -factor). The energy eigenvalues, eigenvectors and basic magnetic properties of the spin-1 Heisenberg dimer given by the Hamiltonian ( 1 ) were exactly calculated and comprehensively discussed in reference [ 51 ], to which readers interested in further details are referred to. For completeness, the eigenvalues and eigenvectors of the Hamiltonian ( 1 ) are listed in Appendix A together with the explicit form of the relevant partition function.…”
Section: Model and Methodsmentioning
confidence: 99%
“…It is noteworthy that the homodinuclear nickel complex [Ni (Medpt) (µ-ox)(H O) ](ClO ) ·2H O (NAOC) [ 48 ] serves as an experimental realization of the investigated spin-1 Heisenberg dimer. We will also take advantage of the available magnetic data reported previously for the NAOC complex [ 49 , 50 ] and theoretical analysis of the respective coupling constants [ 51 , 52 ] in order to quantify a strength of the bipartite entanglement within this molecular-based magnetic material. In particular, we will clarify on this specific molecular magnetic material robustness of the thermal entanglement of the NAOC complex against temperature and magnetic field.…”
Section: Introductionmentioning
confidence: 99%
“…(9) for the sake of compactness. It is quite evident that the Hamiltonians H (0) 2i of the vertical dimers (8) are already diagonal in the dimer representation, while the Hamiltonians H (0) 2i+1 of the horizontal dimers (9) can be diagonalized by a unitary transformation:…”
Section: -51mentioning
confidence: 99%
“…(C2)). Using this procedure, the total Hamiltonian (2) of the spin-1/2 Ising-Heisenberg orthogonal-dimer chain has been put into a fully diagonal form and the ground state of the model can be easily found by minimizing a sum of its local diagonal parts (8) and (12) (see also Ref. 42).…”
Section: -51mentioning
confidence: 99%