23 research outputs found
Quantum fluctuations in the effective pseudospin-1/2 model for magnetic pyrochlore oxides
The effective quantum pseudospin-1/2 model for interacting rare-earth
magnetic moments, which are locally described with atomic doublets, is studied
theoretically for magnetic pyrochlore oxides. It is derived microscopically for
localized Pr^{3+} 4f moments in Pr_2TM_2O_7 (TM = Zr, Sn, Hf, and Ir) by
starting from the atomic non-Kramers magnetic doublets and performing the
strong-coupling perturbation expansion of the virtual electron transfer between
the Pr 4f and O 2p electrons. The most generic form of the nearest-neighbor
anisotropic superexchange pseudospin-1/2 Hamiltonian is also constructed from
the symmetry properties, which is applicable to Kramers ions Nd^{3+}, Sm^{3+},
and Yb^{3+} potentially showing large quantum effects. The effective model is
then studied by means of a classical mean-field theory and the exact
diagonalization on a single tetrahedron and on a 16-site cluster. These
calculations reveal appreciable quantum fluctuations leading to quantum phase
transitions to a quadrupolar state as a melting of spin ice for the Pr^{3+}
case. The model also shows a formation of cooperative quadrupole moment and
pseudospin chirality on tetrahedrons. A sign of a singlet quantum spin ice is
also found in a finite region in the space of coupling constants. The relevance
to the experiments is discussed.Comment: 18 pages including 14 figures; Comparison with the magnetization
curve on Pr2Ir2O7 included; to appear in Phys. Rev.
Characterization of two-dimensional fermionic insulating states
Inspired by the duality picture between superconductivity and insulator in
two spatial dimension, we conjecture that the order parameter, suitable for
characterizing 2D fermionic insulating state, is the disorder operator, usually
known in the context of statistical transformation. Namely, the change of the
phase of the disorder operator along a closed loop measures the particle
density accommodating inside this loop. Thus, identifying this (doped) particle
density with the dual counterpart of the magnetic induction in 2D SC, we can
naturally introduce the disorder operator as the dual order parameter of 2D
insulators. The disorder operator has a branch cut emitting from this
``vortex'' to the single infinitely far point. To test this conjecture against
an arbitrary 2D lattice models, we have chosen this branch cut to be compatible
with the periodic boundary condition and obtain a general form of its
expectation value for non-interacting metal/insulator wavefunction, including
gapped mean-field order wavefunction. Based on this expression, we observed
analytically that it indeed vanishes for a wide class of band metals in the
thermodynamic limit. In insulating states, on the other hand, it is quantified
by the localization length or the real-valued gauge invariant 2-from dubbed as
the quantum metric tensor
Fractional vortex lattice structures in spin triplet superconductors
Motivated by recent interest in spin triplet superconductors, we investigate
the vortex lattice structures for this class of unconventional superconductors.
We discuss how the order parameter symmetry can give rise to U(1)U(1)
symmetry in same sense as in spinor condensates, making half-quantum vortices
(HQV) topologically stable. We then calculate the vortex lattice structure of
HQV's, with particular attention on the roles of the crystalline lattice, the
Zeeman coupling, and Meissner screening, all absent in spinor condensates.
Finally, we consider how spin-orbit coupling leads to a breakdown of the
U(1)U(1) symmetry in free energy and whether the HQV lattice survives
this symmetry breaking. As examples, we examine simpler spin-triplet models
proposed in the context of NaxCoO2yH2O and Bechgaard salts, as well as
the better known and more complex model for Sr2RuO4.Comment: 13 pages, 6 figures. The version published in New Journal of Physics
focus issue on 'Superconductors with Exotic Symmetry' with added reference
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