Scalar order in PrFe_{4}P_{12} and PrRu_{4}P_{12}
We show by phenomenological Landau analysis that the properties of ordered phases in some skutterudites are consistently accounted for by a scalarorder parameter which preserves the cubic symmetry, even in the ordered phase. A universal value is found for the anisotropy ratio of the transition temperature in a magnetic field, homogeneous magnetization, and induced staggered magnetization. The difference in magnetic behavior between PrFe_{4}P_{12} and PrRu_{4}P_{12} near their phase transitions is explained within a single framework. For the lowfield phase of PrFe_{4}P_{12}, the scalar order with Γ_{1g} symmetry can explain (i) the absence of fieldinduced dipoles perpendicular to the magnetic field, (ii) isotropic magnetic susceptibility in the ordered phase, (iii) the fieldangle dependence of the transition temperature, and (iv) the splitting pattern of the ^{31}P nuclear magnetic resonance (NMR) spectra.
A. Kiss and Y. Kuramoto:
J. Phys. Soc. Jpn. 75, 103704 (2006).
Magnetic orders of NpTGa_{5} with T=Co, Ni, Rh, or Fe
We explain the characteristics of magnetic transitions in NpTGa_{5} with T=Co, Ni, Rh in a unified way with use of a crystalline electric field (CEF) model of localized 5f^{4} electrons of Np ion. The model takes a CEF doublet and a singlet as local states, and includes dipolar and quadrupolar intersite interactions in the meanfield theory. Diverse ordering phenomena are derived depending on the magnitude of interaction parameters, which qualitatively reproduce the experimentally observed magnetic behaviors in NpTGa_{5}. The quadrupole degrees of freedom are essential to the diverse magnetic orders. It is argued that NpRhGa_{5} is close to a multicritical point where quadrupoles and dipoles with different directions are competing to order.
In addition, we extended the CEF model by including the Fe moments as the source of anisotropy in order to explain the mechanism of successive magnetic transitions in NpFeGa_{5}. All possible dipolar and quadrupolar interactions are taken into account, which are allowed by the doublet–singlet subspace.
Phase diagrams are obtained which give either two or three successive transitions from the paramagnetic phase. In the latter case, Np moments first order along [110], then tilt around the c axis, and finally tilt out
of the abplane. The ensuing splitting pattern of ^{69}Ga and ^{71}Ga nuclear magnetic resonance (NMR) is analyzed theoretically, and compared with experimental results.
A. Kiss and Y. Kuramoto:
J. Phys. Soc. Jpn. 75, 034709 (2006).
A. Kiss and Y. Kuramoto:
J. Phys. Soc. Jpn. 77, 124708 (2008).
Ordering and crossover in SmRu_{4}P_{12}
We propose a crystalline electric field (CEF) model of localized 4f^{5} electrons of Sm ion for understanding intriguing ordering phenomena in SmRu_{4}P_{12}. We take the CEF quartet and doublet (pseudosextet) of the Hund’s rule ground state with J=5/2, and include intersite interactions between multipoles by the meanfield theory. The model leads to a multipole order with representation 5u, and shows the following
features: (i) increasing transition temperature T_{MI} with increasing magnetic field; (ii) an anomaly in specific heat and other thermodynamic quantities at lower temperature T_{1} < T_{MI}, (iii) sharpening of the anomaly at T_{1} as the magnetic field increases. These behaviors reproduce salient features observed experimentally in SmRu_{4}P_{12}. Possible mechanisms for spontaneous magnetic moment are discussed as well.
A. Kiss and Y. Kuramoto:
J. Phys. Soc. Jpn. 78, 124702 (2009).
Magnetic orders and fluctuations in strongly correlated electron systems
We review experimental and theoretical results on higher electronic multipoles in solids with strong correlations. Recent experiments and their theoretical interpretation have confirmed the ordering of octupoles and even higher multipoles in rareearth and actinide compounds with f electrons.
The concept of multipoles is critically examined in point groups where spherical tensors of different ranks mix. Using a phenomenological approach, we demonstrate how linear and nonlinear couplings of different multipoles lead to rich phase diagrams and anomalies in physical observables. As actual
representative systems, we consider Ce_{x}La_{1x}B_{6} with octupole order, NpO_{2} where quadrupoles induced by the octupole order have been
observed, PrFe_{4}P_{12} with scalar order and URu_{2}Si_{2}.
It is pointed out that multipole orders, particularly the scalar order, should provide a new route for studying the
dichotomy between the itinerant and localized behaviors of electrons.
Y. Kuramoto, H. Kusunose, and A. Kiss:
J. Phys. Soc. Jpn. 78, 072001 (2009).
Lowtemperature ordered phase of Pr in PrBa_{2}Cu_{3}O_{6+x}
We present a theoretical model to describe the anomalous ordered phase of Pr ions in PrBa_{2}Cu_{3}O_{6+x} below
T_{Pr}≈12–17K. The model considers the Pr multipole degrees of freedom and coupling between the Cu and Pr subsystems. We identify the symmetry allowed coupling of Cu and Pr ions and conclude that only an abplane Pr dipole ordering can explain the Cu spin rotation observed at T_{Pr} by neutron diffraction by Boothroyd et al.
[Phys. Rev. Lett. 78, 130 (1997)]. A substantial enhancement of the Pr ordering temperature is shown to arise from the CuPr coupling which is the key for the anomalous magnetic behavior in PrBa_{2}Cu_{3}O_{6+x}.
A. Kiss and F. Simon:
Phys. Rev. B 82, 174413 (2010).
Reverse Kondo effect and antiresonance
We derive accurate numerical results for transport properties of Kondo impurity systems with potential scattering and orbital degeneracy. Using the continuoustime quantum Monte Carlo (CTQMC) method, static and dynamic physical quantities are derived in a wide temperature range across the Kondo temperature T_{K}. With strong potential scattering, the resistivity tends to decrease with decreasing temperature, in contrast to the ordinary Kondo effect. Correspondingly, the quasiparticle density of states obtains the antiresonance around the Fermi level. Thermopower also shows characteristic deviation from the standard Kondo behavior, while magnetic
susceptibility follows the universal temperature dependence even with strong potential scattering. It is found that the t matrix in the presence of potential scattering is not a relevant quantity for the Friedel sum rule, for which a proper limit of the f electron Green’s function is introduced. The optical theorem is also discussed in context of Kondo impurity models with potential scattering.
A. Kiss, Y. Kuramoto and S. Hoshino:
Phys. Rev. B 84, 174402 (2011).
NMR relaxation and carbon hyperfine coupling in singlewall carbon nanotubes
Recent transport measurements [Churchill et al. Nature Phys. 5 321 (2009)] found a surprisingly large, 2–3 orders of magnitude larger than usual ^{13}C hyperfine coupling (HFC) in ^{13}C enriched singlewall carbon nanotubes. We formulate the theory of the nuclear relaxation time in the framework of the TomonagaLuttinger liquid theory to enable the determination of the HFC from recent data by Ihara et al. [ Europhys. Lett. 90 17004 (2010)]. Though we find that 1/T_{1} is orders of magnitude enhanced with respect to a Fermiliquid behavior, the HFC has its usual, small value. Thus, we reexamine the theoretical description used to extract the HFC from transport experiments. We find that similar features can be obtained with HFCindependent system parameters producing HFC with usual small value.
A. Kiss, A. Pályi, Y. Ihara, P. Wzietek, P. Simon, H. Alloul, V. Zólyomi, J. Koltai, J. Kürti, B. Dóra, and F. Simon:
Phys. Rev. Lett. 107, 187204 (2011).
