Quantum effects and Haldane gap in magnetic chains with alternating anisotropy axes

Abstract The isotropic quantum Heisenberg model with alternating uniaxial anisotropy axes is analyzed numerically by the density-matrix renormalization-group (DMRG) method. In the classical version, the model is applied to describe the magnetic properties of the S = 2 zigzag chain containing Mn(III) acetate meso-tetraphenylporphyrin complexes coupled by the phenylphosphinate ligands which transmit antiferromagnetic interactions. Although the tensors representing the uniaxial magnetic anisotropy D and g factors are non-diagonal in the global coordination system, the DMRG approach has been successfully applied to this complex model in the entire temperature region studied. The predictions of our quantum approach are compared to those previously obtained from the classical one and the importance of quantum effects for analysis of the single-crystal susceptibility and magnetization is demonstrated. At low temperatures the magnetization in the field applied along the c direction increases much more slowly than the classical counterpart. The magnetization behavior is very sensitive to temperature. Moreover, the presence of a magnetization jump in the limit T → 0 at the field H = 3.8 Tesla can be an indication of the Haldane gap of the order of 10.2 K. The considerable differences are demonstrated for the temperature dependent single-crystal susceptibilities, but surprisingly they disappear after averaging over the three crystallographic directions which has not been reported before.

[1]  M. Suzuki,et al.  On the convergence of exponential operators—the Zassenhaus formula, BCH formula and systematic approximants , 1977 .

[2]  G. Musiał,et al.  Phenomenological modeling of molecular-based rings beyond the strong exchange limit: Bond alternation and single-ion anisotropy effects , 2008 .

[3]  Density Matrix Renormalization Group Method for 2D Classical Models , 1995, cond-mat/9508111.

[4]  G. G. Stokes "J." , 1890, The New Yale Book of Quotations.

[5]  White,et al.  Density matrix formulation for quantum renormalization groups. , 1992, Physical review letters.

[6]  A. Vindigni,et al.  The canted antiferromagnetic approach to single-chain magnets. , 2008, Journal of the American Chemical Society.

[7]  T. Xiang,et al.  TRANSFER-MATRIX DENSITY-MATRIX RENORMALIZATION-GROUP THEORY FOR THERMODYNAMICS OF ONE-DIMENSIONAL QUANTUM SYSTEMS , 1997 .

[8]  A. Yamaguchi,et al.  Molecular Nanomagnets , 2002 .

[9]  A. Bieńko,et al.  Anisotropy and magnetic properties of the bimetallic thiocyanate-bridged chains: Density-matrix renormalization approach , 2010 .

[10]  White,et al.  Density-matrix algorithms for quantum renormalization groups. , 1993, Physical review. B, Condensed matter.

[11]  M. Suzuki,et al.  Generalized Trotter's formula and systematic approximants of exponential operators and inner derivations with applications to many-body problems , 1976 .

[12]  G. Kamieniarz,et al.  Simulations of the low-dimensional magnetic systems by the quantum transfer-matrix technique , 2003 .

[13]  A. Bieńko,et al.  Magnetic properties and DMRG modeling of the 1D bimetallic thiocyanate bridged compound {(CuL1)[Co(NCS)4]} (L1 = N-rac-5,12-Me2-[14]-4,11-dieneN4) , 2009 .

[14]  U. Schollwoeck The density-matrix renormalization group , 2004, cond-mat/0409292.

[15]  A. Maciołek,et al.  Interplay of complete wetting, critical adsorption, and capillary condensation. , 2008, Physical review. E, Statistical, nonlinear, and soft matter physics.