Abstract
The interplay between electron correlation and spin–orbit coupling in solids has been proven to be an abundant gold mine for emergent topological phases. Here we report the results of systematic magnetotransport study on bandwidthcontrolled pyrochlore iridates R_{2}Ir_{2}O_{7} near quantum metalinsulator transition (MIT). The application of a magnetic field along [001] crystallographic direction (H//[001]) significantly decreases resistivity while producing a unique Hall response, which indicates the emergence of the novel semimetallic state in the course of the magnetic transformation from allin allout (AIAO, 4/0) to 2in 2out (2/2) spin configuration. For H//[111] that favours 3in 1out (3/1) configuration, by contrast, the resistivity exhibits saturation at a relatively high value typical of a semimetal. The observed properties can be identified to reflect the emergence of multiple Weyl semimetal states with varying numbers of Weyl points and line nodes in respective spin configurations. With tuning effective bandwidth, all these states appear to concentrate around the quantum MIT region, which may open a promising venue for topological phenomena and functions.
Similar content being viewed by others
Introduction
The pyrochlore R_{2}Ir_{2}O_{7} is composed of the networks of cornerlinked tetrahedra of rareearth R ions and Ir ones. This geometrically frustrated lattice offers a fertile ground to host exotic electronic/magnetic states^{1,2,3,4}. Recent angleresolved photoemission spectroscopy unveils that the R=Pr compound is a unique semimetal with a quadratic band crossing at Γ point, which is an essential ingredient for versatile topological states^{5}; for instance, the antiferromagnetic allin allout (AIAO) magnetic order, which breaks timereversal symmetry while preserving crystal symmetry, lifts the band degeneracy, leading to linearly dispersed band touching points in three dimension, here termed Weyl semimetal (WSM (4/0))^{3,6,7}. Another possibility for unconventional electronic states is intensively discussed with different magnetic patterns^{8,9,10,11}. Owing to the uniaxial magnetic anisotropy along the cubic [111] or equivalent directions into the center of the tetrahedron, various magnetic pattern can be achieved under the competition between exchange interactions and external magnetic field^{12}. For example, when a magnetic field applied along H//[001] (H//[111]) is strong enough to overcome the exchange interaction, it turns two (three) magnetic moments point inwards and the other two (one) point outwards of the tetrahedron, forming 2/2 (3/1) configuration.
Another key parameter is a oneelectron bandwidth, exemplifying the inverse of the effective electron correlation (U)^{13}. One can finely tune it by applying hydrostatic pressure^{14,15} or substituting R site^{16,17} that can drive metalinsulator transition (MIT); the Pr compound is a paramagnetic semimetal down to 120 mK^{18}, whereas the paramagnetic or antiferromagnetic AIAO insulating phase shows up with smaller R ionic radius^{19,20,21}, seemingly akin to the correlationinduced MIT as widely observed for 3delectron materials^{15,22,23}. On the verge of quantum MIT (in between R=Nd and Pr), however, the unconventional magnetotransport phenomena have been reported, including anomalous Hall effect^{24,25}, highly metallic AIAO domain walls^{26,27} and fieldinduced MIT^{10,11}, which may be potentially correlated to the predicted topological states. The quantum MIT involving such correlated topological states may provide an ideal platform of a novel quantum criticality^{28,29}, but has been rarely explored so far. To address this issue, we perform systematic magnetotransport measurements on R=Nd and its partially Prsubstituted (R=Nd_{0.5}Pr_{0.5}) compounds under external pressures (P) and magnetic fields (H), which allow us to finely and precisely tune the effective bandwidth and magnetic configuration. We have revealed the rich topological phases as a function of bandwidth and magnetic field around the quantum critical point.
Results
Electronic/magnetic phase diagram for pyrochlore iridates
We show the temperature dependence of resistivity at several pressures in Fig. 1d–h. The resistivity at ambient pressure increases rapidly below the transition temperature T_{N}=22 K, which is higher than that of the previous study thanks to the recent improvement of the sample quality (see Methods). The transition temperature systematically shifts to lower temperature with increasing pressure as observed also in previous studies^{14,15}. Figure 1i displays the temperature dependence of resistivity for the mixedcrystal compound of x=0.5 (R=Nd_{1−x}Pr_{x}), which also shows a sharp increase below 4 K. We plot the T_{N} as a function of pressure and chemical substitution x in Fig. 1j, using the established empirical relation between the chemical and physical pressures^{15} that the composition change Δx=0.1 corresponds to the pressure change ΔP=0.65 GPa; hereafter, we regard x=0.5 as being equivalent to the application of P=3.3 GPa on x=0. The T_{N} is almost linearly suppressed as (chemical) pressure increases, enabling us to explore a broad range of effective bandwidthcontrol effect. It should be noted that the AIAO insulating phase persists up to P∼5.0 GPa (P∼1.7 GPa on the x=0.5 compound) as shown in the pressure dependence of resistivity for x=0.5 (Supplementary Fig. 1). Such robustness of the insulating phase is also reported in ref. 14.
Anomalous magnetotransport phenomena near MIT
Figure 1d–i also display the resistivity under a magnetic field of 14 T along [001] direction and [111] direction. For H//[001], whereas the resistivity slightly decreases by the application of magnetic field at ambient pressure, the abrupt increase of the resistivity below T_{N} is significantly suppressed above P=1.0 GPa. It means that the systematic application of pressure brings the system to the critical region in which various electronic or magnetic phases strongly compete with each other, as observed for the colossal magnetoresistance in perovskite manganites^{30}. It is noteworthy that the similar large magnetoresistance was reported in refs 10, 11 even at ambient pressure. This can be ascribed to the slight offstoichiometry of the crystal such as iridium deficiency, which somewhat changes the band filling of the system and effectively drive the system closer to the critical region. The applied magnetic field H//[111], on the other hand, induces distinct magnetotransport properties from the case of H//[001]; the resistivity starts to rise gradually even above T_{N} and appears to nearly saturate at lower temperatures. The observed property for each field direction is attributable to the emergence of a novel electronic state induced by H//[001] (H//[111]), which favours the 2/2 (3/1) magnetic configuration in R 4f moments as depicted in Fig. 1b,c. In fact, the saturated values of magnetization for H//[001] (H//[111]) agree well with the expected values in 2/2 (3/1) state (Supplementary Fig. 2a–d). The no delectron analog Nd_{2}Zr_{2}O_{7}, in which the Nd 4f moment forms AIAO magnetic order at zero field, also shows magnetic fieldinduced 2/2 or 3/1 order^{31}. Furthermore, for the x=0.5 compound, the peak of the specific heat divided by temperature gradually shifts to higher temperature, while being broadened on increasing H//[001] (H//[111]) (Supplementary Fig. 2e,f); these features clearly indicate that the increasing magnetic field H//[001] (H//[111]) induces the 2/2 (3/1) type magnetic order at higher temperatures than T_{N}^{32,33}. Owing to the magnetic coupling between 4f and 5d moments, the magnetic structure of 5d moments can follow that of 4f ones, leading to the observed transport properties. It is to be noticed that the magnetic field is always applied perpendicular to the electric current in this experiment (see Methods), which excludes the possibility of chiral anomaly effect, that is, the negative magnetoresistance effect with the current parallel to the magnetic field, recently observed in a WSM material^{34}. Hence, the observed anisotropic magnetoresistance genuinely stems from the modulation of the magnetic configuration.
Magnetotransport properties for H//[001]
The magnetic field dependence of resistivity for H//[001] at several pressures are given in the top panels of Fig. 2. The sharp decrease of resistivity is accompanied by a hysteresis between fieldincreasing and fielddecreasing processes below T_{N}, as discerned in previous studies^{10,11}. The Hall conductivity shown in Fig. 2f–j provides important insights into the observed fieldinduced MIT. Above T_{N}, the Hall conductivity is nearly proportional to magnetic field, typical of normal Hall effect. By contrast, below T_{N}, the Hall conductivity exhibits nonmonotonous field dependence; it is nearly zero at low magnetic fields, abruptly rises up at intermediate fields and eventually decreases towards a negative value at high fields. This feature is more pronounced as temperature is decreased. A similar sign change of Hall response is also observed in the Nd_{2}Ir_{2}O_{7} polycrystals^{25}. The observed complexity of the Hall response can be hardly explained in terms of the conventional normal or anomalous Hall resistivity^{35}. The contour plots of the longitudinal and Hall conductivity in the plane of temperature and magnetic field for H//[001] at various pressures are shown in Fig. 3a–j, respectively.
In general, the Hall conductivity is sensitive to the relaxation time. For instance, the vanishing Hall conductivity at low fields reflects the localized nature of electrons, in accord with the relatively large value of resistivity (ρ_{xx}>10 mΩcm). At high fields, on the other hand, the Hall conductivity largely decreases towards a negative value, while the resistivity nearly saturates around ρ_{xx}∼0.4 mΩcm (Fig. 2a–e); one plausible candidate of the electronic phase for this metallic state can be the topological state in the 2/2 configuration, which possesses a nodal line in the k_{z}=0 plane and two Weyl points on the k_{z} axis as presented in Fig. 4b, dubbed here line node semimetal (LSM) following the previous study^{10}. The major result of Hall response presented here is a sizable signal with positive sign in an intermediate field region. On increasing field, the Hall conductivity shows a dramatic change including even a sign reversal, which can be attributed to the crossover between the 4/0 WSM (Fig. 4a) and 2/2 LSM (Fig. 4b), as schematically shown in Fig. 4d,f. As 4/0 WSM and 2/2 LSM have different Fermi surface topology, the transition between them requires a significant modification of the band structure near the Fermi level such as accompanied by emerging electron/hole pockets, which can strongly modify the Hall conductivity including its sign changes. Such competing contribution of the normal and anomalous components to the total Hall conductivity are also theoretically calculated shown in Supplementary Fig. 3, which demonstrates the nonmonotonic magnetic field dependency.
In the contour plots of longitudinal and Hall conductivity shown in Fig. 3a–j, we can unveil the characteristic relation between the observed MIT and Hall conductivity for H//[001]. Both longitudinal and Hall conductivity are relatively small in a lowfield and lowtemperature region (AIAO insulating phase). On increasing field, the Hall conductivity shows a dramatic change with a sign reversal, which can be attributed to the crossover between the WSM and LSM, as schematically shown in Fig. 4d,f. Interestingly, the WSM phase, which was theoretically predicted to exist in quite a narrow temperature window at zero field^{6,7} and hence would be difficult to detect such an electronic band state by optical^{36} and angleresolved photoemission spectroscopy^{37}, can be extended by an application of magnetic field along [001], which deforms the regular 4/0 spin configuration. Moreover, as the pressure increases, both AIAO insulating phase and WSM one appear to shrink, whereas the LSM extends towards zero temperature and zero field. At the quantum critical point, the various competing phases, not only antiferromagnetic Mott insulator and paramagnetic semimetal but also the topological pseudo4/0 WSM and 2/2 LSM, come close to each other in free energy, apparently merging into the quantum critical point.
Unconventional semimetal phases in H//[111]
We now turn to the magnetotransport properties for H//[111], which are shown in Fig. 2k–t. Right above T_{N}, the resistivity is largely enhanced by an applied field, whereas the Hall conductivity shows a sharp upturn and changes its sign in high magnetic field (Fig. 2p–t); similar magnetotransport properties are also reported for the paramagnetic R=Pr compound at a much lower temperature (T=30 mK)^{38}. On lowering temperature below T_{N}, a sharp dip structure is observed around μ_{0}H=3 T in resistivity, attributable to the emergence of metallic domain walls as demonstrated in the previous studies^{26,27}. More importantly, the resistivity exhibits the unique magnetic field dependence accompanied by a hysteresis between fieldincreasing and decreasing processes, which is most pronounced at T=9 K and P=1.0 GPa as shown in Fig. 2k. Furthermore, the resistivity appears to saturate around ρ_{xx}∼7 mΩcm above μ_{0}H=9 T at which the hysteresis loop closes, indicative of a transition from the 4/0 to the 3/1 magnetic state. To see the evolution of the respective phases more clearly, we plot the contour map of longitudinal conductivity and Hall conductivity in Fig. 3k–t, respectively, and its schematic phase diagram in Fig. 4e,g. One can see that the conductivity is relatively small in a high field region where the sign of Hall conductivity is positive, which can be assigned to the emergence of the new semimetal state with the 3/1 magnetic configuration.
To elucidate the electronic band structure in the 3/1 state, we perform a meanfield calculation (see Methods). The important feature in the 3/1 state is that there is only one trigonal axis parallel to H//[111], contrary to the 4/0 state with four trigonal axes. It is noteworthy that a pair of Weyl points are always on one of the four trigonal axes in the AIAO state. As each pair of Weyl points is constrained to be on a onedimensional line, pairannihilation can be easily achieved by increasing the pair separation until they merge at the Brillouin zone boundary. In the 3/1 state, however, broken threefold rotation symmetry allows six Weyl points to be shifted away from the relevant onedimensional subspace and, instead, to move in twodimensional mirror plane. Whereas the remaining two Weyl points on the trigonal axis parallel to H are still constrained, their pairannihilation results in another WSM with six Weyl points (termed here WSM (3/1)) as described in Fig. 4c. Considering that the point nodes moving in twodimensional space have smaller collision probability than those moving in onedimensional space, it is natural to expect that WSM (3/1) is more stable than WSM (4/0), and hence occupies a wider range in the phase diagram; WSM (3/1) phase survives all the way as H increases, whereas it is stable within a finite window as U increases.
By combining the systematic transport experiments with the theoretical calculations, we suggest that multiple topological states can show up as a function of effective bandwidth (or effective electron correlation U) and magnetic field, as schematically shown in Fig. 4d–f. Future neutron and Xray experiments on the magnetic states as done in refs 19, 20, 21 will serve to verify the present interpretation for the fieldinduced emergent topological states. Another important feature revealed here is that all these topological states appear to merge towards the magnetic quantum critical point; this may enable the further exploration for new topological quantum states and related exotic electromagnetic responses in this ideal system endowed with Mott criticality.
Methods
Single crystal growth
Single crystals of Nd_{2}Ir_{2}O_{7} and its partially Prreplaced (Nd_{1−x}Pr_{x})_{2}Ir_{2}O_{7} were grown by the KF flux method as described in ref. 39. Initially, polycrystalline samples of them were prepared by solid state reactions of rareearth oxides (Nd_{2}O_{3} and Pr_{6}O_{11}) and iridate IrO_{2}. The materials with the prescribed molar ratios were ground, pressed into pellet, and then sintered at 1,273 K for several days. After taken out from the furnace, the polycrystals were ground again and mixed with KF flux in a ratio of 1:200. The mixtures are placed in a platinum crucible covered with a lid. The crucible was cooled down to 1,123 K at a rate of 2 K h^{−1} following anneal for 3–5 h at 1,373 K. After cooling, crystals were separated from the KF residual flux by rinsing it out with distilled water. Octahedralshaped single crystals were obtained as reported in ref. 39. The crystals were characterized by xray diffraction. The qualities of the present samples are improved and the transition temperature becomes higher than that of the crystals previously reported in ref. 10.
Transport and specific heat measurements
Transport, magnetization and specific heat measurements were performed using Physical Property Measurement System (Quantum Design). Resistivity (Hall conductivity) was measured by a standard fourprobe method with the current direction parallel to [110] crystalline direction while the magnetic field along both [001] and [111] crystallographic directions was applied perpendicular to the current. The Hall conductivity is deduced by the antisymmetrization of the raw transverse signals perpendicular to the electric current. Pressure was generated by a pistoncylinder pressure cell for Physical Property Measurement System. To keep the samples in a hydrostatic pressure, Daphne 7474 oil was used as the pressuretransmitting medium. Pressure was determined by examining the superconducting transition temperature of lead.
Theoretical analysis
To understand the magnetotransport experiment, we first performed a numerical study of the lattice Hamiltonian^{8}, where +. Here t_{1,2} indicates the hopping amplitude between nearestneighbour (next nearest neighbour) Ir sites, and the Pauli matrices s_{x,y,z} represent the doublets with the total angular momentum J_{eff}=1/2. The real vectors d_{ij}, R_{ij}, D_{ij} describe s dependent hopping terms. denotes Zeeman coupling to external magnetic field H. H_{fd} indicates the f–d exchange coupling between Ir and rareearth moments, which has the following form where h_{fd,i} indicates the effective magnetic field at the ith Ir site due to six neighbouring rareearth spins around it. Here we treat each rareearth spin as an Ising spin aligned along its local trigonal axis. Finally, the last term describes electron correlation effect due to the local Hubbardtype interaction (U) between Ir electrons. To treat the Coulomb interaction, we employ a mean field approximation by introducing local order parameters m_{1,2,3,4} at each site i=1, 2, 3, 4 in a unit cell. To facilitate the analysis, we assumed that the main role of the f–d exchange and the external magnetic field is to rotate the Ir spin orientation from the AIAO to 2in 2out (or 3in 1out) state when H//[001] (H//[111]). Then, we can examine the band structure by changing the direction of Ir moments continuously for a given magnitude of Ir moments.
To confirm the results from the lattice Hamiltonian analysis, we also performed the effective model analysis by constructing low energy Hamiltonian near Γ or L points. For H//[001], the results from the lattice Hamiltonian study are already reported in ref. 10. Here we performed additional lowenergy Hamiltonian analysis near Γ point and obtained consistent results. Namely, magnetic fieldinduced modulation of Ir spin orientation induces a WSM with point nodes and also an LSM with a line node (LSM) accompanying two additional point nodes. On the other hand, when H//[111], we found the transition from a WSM (4/0) with eight Weyl points to a WSM (3/1) with six Weyl points numerically. To support this, we provide detailed effective Hamiltonian analysis as shown in the following.
As a pair annihilation of Weyl points occurs at an L point, we need an effective Hamiltonian constructed near the L point. In the absence of magnetic field H//[111], the Hamiltonian at the L point is invariant under inversion (P), a combination of a mirror and time reversal (MT), and a threefold rotation about Γ–L (C_{3}). One can find that P, MT and C_{3} can be represented by P=σ_{z} , MT=K, C_{3}= where σ_{x,y,z} denotes the two bands touching at the L point and K stands for complex conjugation. Then the effective Hamiltonian near the L point can generally be written as where v, Δ, A_{xy}, A_{z} are constants and q_{z} is the momentum along the Γ–L direction. This Hamiltonian describes a WSM (a gapped insulator) when . In the presence of H//[111], the Weyl points can be separated into two groups. First, in the case of the Weyl point pair located parallel to H//[111], P, MT and C_{3} symmetries are all preserved, thus the relevant Hamiltonian maintains the same form as above, except the fact that the constants v, Δ, A_{xy} and A_{z} depend on H. For example, . Thus, the magnetic field H can control the transition between a WSM and a gapped insulator. On the other hand, in the case of the other six Weyl points, the relevant effective Hamiltonian has a more complicated form since C_{3} symmetry is broken and the magnetic field is not along the local z axis. Assuming , the effective Hamiltonian becomes where and other constant terms have similar structure. One can clearly see that the location of Weyl points is no longer on the Γ–L direction (or the local z direction) due to the magnetic field. Although a pair annihilation of Weyl points can also occur in principle, the comparison to the tightbinding analysis shows that, in general, the magnetic field shifts the location of Weyl points away from the L point stabilizing the WSM phase whereas the electron correlation forces the Weyl points to move towards the L point inducing the transition to a gapped insulator.
Data availability
The data that support the findings of this study are available from the corresponding author upon reasonable request.
Additional information
How to cite this article: Ueda, K. et al. Magneticfield induced multiple topological phases in pyrochlore iridates with Mott criticality. Nat. Commun. 8, 15515 doi: 10.1038/ncomms15515 (2017).
Publisher’s note: Springer Nature remains neutral with regard to jurisdictional claims in published maps and institutional affiliations.
References
WitczakKrempa, W., Chen, G., Kim, Y. B. & Balents, L. Correlated quantum phenomena in the strong spinorbit coupling. Annu. Rev. Condens. Matter Phys. 5, 57–82 (2014).
Pesin, D. & Balents, L. Mott physics and band topology in materials with strong spinorbit interaction. Nat. Phys. 6, 376–381 (2010).
Wan, X., Turner, A. M., Vishwanath, A. & Savrasov, S. Y. Topological semimetal and Fermiarc surface states in the electronic structure of pyrochlore iridates. Phys. Rev. B 83, 205101 (2011).
Yang, B.J. & Kim, Y. B. Topological insulators and metalinsulator transition in the pyrochlore iridates. Phys. Rev. B 82, 085111 (2010).
Kondo, T. et al. Quadratic Fermi node in a 3D strongly correlated semimetal. Nat. Commun. 6, 10042 (2015).
WitczakKrempa, W. & Kim, Y. B. Topological and magnetic phases of interacting electrons in the pyrochlore iridates. Phys. Rev. B 85, 045124 (2012).
Yamaji, Y. & Imada, M. Metallic interface emerging at magnetic domain wall of antiferromagnetic insulator: fate of extinct Weyl electrons. Phys. Rev. X 4, 021035 (2014).
Chen, G. & Hermele, H. Magnetic orders and topological phases from fd exchange in pyrochlore iridates. Phys. Rev. B 86, 235129 (2012).
Lee, S.B., Paramekanti, A. & Kim, Y. B. RKKY interactions and the anomalous Hall effect in metallic rareearth pyrochlores. Phys. Rev. Lett. 111, 196601 (2013).
Ueda, K. et al. Magnetic fieldinduced insulatorsemimetal transition in a pyrochlore Nd2Ir2O7 . Phys. Rev. Lett. 115, 056402 (2015).
Tian, Z. et al. Fieldinduced quantum metalinsulator transition in the pyrochlore iridate Nd2Ir2O7 . Nat. Phys. 12, 134 138 (2016).
Bramwell, S. T. & Harris, M. J. Frustration in Isingtype spin models on the pyrochlore lattice. J Phys. Condens. Matter 10, L215–L220 (1998).
Imada, M., Fujimori, A. & Tokura, Y. Metalinsulator transitions. Rev. Mod. Phys. 70, 1039 (1998).
Sakata, M. et al. Suppression of metalinsulator transition at high pressure and pressureinduced magnetic ordering in pyrochlore oxide Nd2Ir2O7 . Phys. Rev. B 83, 041102 (2011).
Ueda, K., Fujioka, J., Terakura, C. & Tokura, Y. Pressure and magnetic field effects on metalinsulator transitions of bulk and domain wall states in pyrochlore iridates. Phys. Rev. B 92, 121110 (2015).
Matsuhira, K., Wakeshima, M., Hinatsu, Y. & Takagi, S. Metalinsulator transitions in pyrochlore oxides Ln2Ir2O7 . J. Phys. Soc. Jpn 80, 094701 (2011).
Ueda, K., Fujioka, J. & Tokura, Y. Variation of optical conductivity spectra in the course of bandwidthcontrolled metalinsulator transitions in pyrochlore iridates. Phys. Rev. B 93, 245120 (2016).
Nakatsuji, S. et al. Metallic spinliquid behavior of the geometrically frustrated Kondo lattice Pr2Ir2O7 . Phys. Rev. Lett. 96, 087204 (2006).
Tomiyasu, K. et al. Emergence of metallic longrange order in frustrated pyrochlore Nd2Ir2O7 with metalinsulator transition. J. Phys. Soc. Jpn 81, 034709 (2012).
Sagayama, H. et al. Determination of longrange allinallout ordering of Ir4+ moments in a pyrochlore iridate Eu2Ir2O7 by resonant Xray diffraction. Phys. Rev. B 87, 100403 (2013).
Donnerer, C. et al. Allin allout magnetic order and propagating spin waves in Sm2Ir2O7 . Phys. Rev. Lett. 117, 037201 (2016).
McWhan, D. B., Menth, A., Remeika, J. P., Brinkman, W. F. & Rice, T. M. Metalinsulator transitions in pure and doped V2O3 . Phys. Rev. B 7, 1920 (1973).
Torrance, J. B., Lacorre, P., Nazzal, A. I., Ansaldo, E. J. & Niedermayer, C. Systematic study of insulatormetal transitions in perovskite RNiO3 (R=Pr, Nd, Sm, Eu) due to closing of chargetransfer gap. Phys. Rev. B 45, 8209 (1992).
Machida, Y. et al. Unconventional anomalous Hall effect enhanced by a noncoplanar spin texture in the frustrated Kondo lattice Pr2Ir2O7 . Phys. Rev. Lett. 98, 057203 (2007).
Disseler, S. M. et al. Magnetization and Hall effect studies on the pyrochlore iridate Nd2Ir2O7 . Phys. Rev. B 87, 060403 (2013).
Ueda, K. et al. Anomalous domainwall conductance in pyrochloretype Nd2Ir2O7 on the verge of the metalinsulator transition. Phys. Rev. B 89, 075127 (2014).
Ma, E. Y. et al. Mobile metallic domainwalls in an allin allout magnetic insulator. Science 350, 538–541 (2015).
Yang, B.J., Moon, E.G., Isobe, H. & Nagaosa, N. Quantum criticality of topological phase transitions in threedimensional interacting electronic systems. Nat. Phys. 10, 774–778 (2014).
Savary, L., Moon, E.G. & Balents, L. New type of quantum criticality in the pyrochlore iridates. Phys. Rev. X 4, 041027 (2014).
Tokura, Y. Critical features of colossal magnetoresistive manganites. Rep. Prog. Phys. 69, 797–851 (2006).
Lhotel, E. et al. Fluctuations and allinallout ordering in dipoleoctupole Nd2Zr2O7 . Phys. Rev. Lett. 115, 197202 (2015).
Hiroi, Z., Matsuhira, K., Takagi, S., Tayama, T. & Sakakibara, T. Specific heat of Kagome ice in the pyrochlore oxide Dy2Ti2O7 . J. Phys. Soc. Jpn 72, 411–418 (2003).
Onose, Y., Taguchi, Y., Ito, T. & Tokura, Y. Specificheat study of the spinstructural change in pyrochlore Nd2Mo2O7 . Phys. Rev. B 70, 060401 (2004).
Huang, X. et al. Observation of the chiralanomalyinduced negative magnetoresistance in 3D Weyl semimetal TaAs. Phys. Rev. X 5, 031023 (2015).
Nagaosa, N., Sinova, J., Onoda, S., MacDonald, A. H. & Ong, N. P. Anomalous Hall effect. Rev. Mod. Phys. 82, 1539 (2010).
Ueda, K. et al. Variation of charge dynamics in the course of metalinsulator transition for pyrochloretype Nd2Ir2O7 . Phys. Rev. Lett. 109, 136402 (2012).
Nakayama, M. et al. Slater to Mott crossover in the metal to insulator transition of Nd2Ir2O7 . Phys. Rev. Lett. 117, 056403 (2016).
Balicas, L., Nakatsuji, S., Machida, Y. & Onoda, S. Anisotropic hysteretic Hall effect and magnetic control of chiral domains in the chiral spin states of Pr2Ir2O7 . Phys. Rev. Lett. 106, 217204 (2011).
Millican, J. N. et al. Crystal growth and structure of R2Ir2O7 (R=Pr, Eu) using molten KF. Mater. Res. Bull. 42, 928–934 (2007).
Acknowledgements
This work was supported by the Japan Society for the Promotion of Science through the Funding Program for WorldLeading Innovative R&D on Science and Technology (FIRST Program) on ‘Quantum Science on Strong Correlation’ initiated by the Council for Science and Technology Policy and by JSPS GrantinAid for Scientific Research (grant numbers 80609488, 26103006 and 24224009). T.O. and B.J.Y. were supported by IBSR009D1, Research Resettlement Fund for the new faculty of Seoul National University and Basic Science Research Program through the National Research Foundation of Korea (NRF) funded by the Ministry of Education (grant number 042620150011).
Author information
Authors and Affiliations
Contributions
Y.T. and N.N. conceived and guided the project. K.U. performed single crystal growth and transport, magnetization and specific heat measurements with help from R.K. and J.F. T.O. and B.J.Y. carried out theoretical calculation of the band structure and the Hall conductivity. All authors discussed the results and contributed to the manuscript.
Corresponding author
Ethics declarations
Competing interests
The authors declare no competing financial interests.
Supplementary information
Supplementary Information
Supplementary Figures and Supplementary References (PDF 696 kb)
Rights and permissions
This work is licensed under a Creative Commons Attribution 4.0 International License. The images or other third party material in this article are included in the article’s Creative Commons license, unless indicated otherwise in the credit line; if the material is not included under the Creative Commons license, users will need to obtain permission from the license holder to reproduce the material. To view a copy of this license, visit http://creativecommons.org/licenses/by/4.0/
About this article
Cite this article
Ueda, K., Oh, T., Yang, BJ. et al. Magneticfield induced multiple topological phases in pyrochlore iridates with Mott criticality. Nat Commun 8, 15515 (2017). https://doi.org/10.1038/ncomms15515
Received:
Accepted:
Published:
DOI: https://doi.org/10.1038/ncomms15515
This article is cited by

Magnetotransport of Sm2Ir2O7 across the pressureinduced quantumcritical phase boundary
npj Quantum Materials (2024)

Spontaneous topological Hall effect induced by noncoplanar antiferromagnetic order in intercalated van der Waals materials
Nature Physics (2023)

Progress and prospects in magnetic topological materials
Nature (2022)

Unconventional free charge in the correlated semimetal Nd2Ir2O7
Nature Physics (2020)

Spontaneous Hall effect in the Weyl semimetal candidate of allin allout pyrochlore iridate
Nature Communications (2018)
Comments
By submitting a comment you agree to abide by our Terms and Community Guidelines. If you find something abusive or that does not comply with our terms or guidelines please flag it as inappropriate.