Abstract
Pyrochlore rare-earth iridates Ln\(_2\)Ir\(_2\)O\(_7\) (Ln: lanthanides) is a unique frustrated Kondo lattice system composed of localized 4f moments and Ir 5d conduction electrons. Recent active research has revealed that the Kondo coupling between the 4f electron and the Ir 5d bands leads to novel transport properties. First, we will make an overview of the phase diagram of pyrochlore rare-earth iridates Ln\(_2\)Ir\(_2\)O\(_7\). Next, we focus on the phenomena associated with spin ice physics. Ln\(_2\)Ir\(_2\)O\(_7\) (Ln \(=\) Nd, Sm, Eu, \(\ldots \)) exhibits a metal-insulator transition, while Pr\(_2\)Ir\(_2\)O\(_7\) does not show any sign of long range ordering. Both Pr and Nd moments have a local \(\langle 111 \rangle \) Ising anisotropy. In the metallic state, localized 4f moments are coupled through the RKKY interaction. For Pr\(_2\)Ir\(_2\)O\(_7\), a ferromagnetic correlation between Pr moments is developed on cooling. On the other hand, Nd\(_2\)Ir\(_2\)O\(_7\) exhibits a metal-insulator transition at 33 K, and then, all-in all-out magnetic structure of Nd moments emerges below 10 K, as observed in the neutron scattering experiments. For Nd\(_2\)Ir\(_2\)O\(_7\), antiferromagnetic correlation between Nd moments is dominant. Metal insulator transition of Nd\(_2\)Ir\(_2\)O\(_7\) can be suppressed by the application of pressure. The insulating phase disappears above 10 GPa. In the pressure induced metallic state, a new phase transition emerges around 3 K. This phase transition is likely due to ferromagnetic ordering, suggesting an ordered spin ice of Nd moment. In the metallic frustrated magnet Pr\(_2\)Ir\(_2\)O\(_7\), a spontaneous Hall effect is observed at zero field in the absence of uniform magnetization, suggesting an emergence of a chiral spin liquid. The origin of this spontaneous Hall effect is ascribed to chiral spin textures, which are inferred from the magnetic measurements indicating the spin ice-rule formation.
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Notes
- 1.
A tetrahedron, a building block of pyrochlore lattice, is a triangle-based object.
References
M. Hanawa, Y. Muraoka, T. Tayama, T. Sakakibara, J. Yamaura, and Z. Hiroi, Phys. Rev. Lett. 87, 187001 (2001). https://doi.org/10.1103/PhysRevLett.87.187001
Y. Taguchi, Y. Oohara, H. Yoshizawa, N. Nagaosa, and Y. Tokura, Science 291, 2573 (2001). https://doi.org/10.1126/science.1058161
S. Yonezawa, Y. Muraoka, Y. Matsushita, and Z. Hiroi, J. Phys.: Condens. Matter 16, L9 (2004). https://doi.org/10.1088/0953-8984/16/3/L01
S. Nakatsuji, Y. Machida, Y. Maeno, T. Tayama, T. Sakakibara, J. van Duijn, L. Balicas, J. N. Millican, R. T. Macaluso, and J. Y. Chan, Phys. Rev. Lett. 96, 087204 (2006). https://doi.org/10.1103/PhysRevLett.96.087204
K. Matsuhira, M. Wakeshima, R. Nakanishi, T. Yamada, A. Nakamura, W. Kawano, S. Takagi, and Y. Hinatsu, J. Phys. Soc. Jpn. 76, 043706 (2007). https://doi.org/10.1143/JPSJ.76.043706
A. Yamamoto, P. A. Sharma, Y. Okamoto, A. Nakao, H. A. Katori, S. Niitaka, D. Hashizume, and H. Takagi, J. Phys. Soc. Jpn. 76, 043703 (2007). https://doi.org/10.1143/JPSJ.76.043703
Y. Machida, S. Nakatsuji, S. Onoda, T. Tayama, T. sakakibara, Nature 463, 210 (2009). https://doi.org/10.1038/nature08680
K. Momma, and F. Izumi, J. Appl. Crystallogr. 44, 1272 (2011). https://doi.org/10.1107/S0021889811038970
K. Matsuhira, M. Wakeshima, Y. Hinatsu, and S. Takagi, J. Phys. Soc. Jpn. 80, 094701 (2011). https://doi.org/10.1143/JPSJ.80.094701
D. Yanagishima and Y. Maeno, J. Phys. Soc. Jpn. 70, 28 (2001) . https://doi.org/10.1143/JPSJ.70.28
K. Matsuhira, K. Kuroda, T. Sakakibara, M. Wakeshima, and Y. Hinatsu, JPS Conf. Proc. 3, 013017 (2014). https://doi.org/10.7566/JPSCP.3.013017
L. Savary, E.-G. Moon, and L. Balents, Phys. Rev. X 4, 041027 (2014). https://doi.org/10.1103/PhysRevX.4.041027
M. Watahiki, K. Tomiyasu, K. Matsuhira, K. Iwasa, M. Yokoyama, S. Takagi, M. Wakeshima, and Y. Hinatsu, J. Phys.: Conf. Ser. 320, 012080 (2011). https://doi.org/10.1088/1742-6596/320/1/012080
K. Matsuhira, Y. Hinatsu, K. Tenya, H. Amitsuka, and T. Sakakibara, J. Phys. Soc. Jpn. 71, 1576 (2002). https://doi.org/10.1143/JPSJ.71.1576
A. Ikeda and H. Kawamura, J. Phys. Soc. Jpn. 77, 073707 (2008). https://doi.org/10.1143/JPSJ.77.073707
S. Onoda and Y. Tanaka, Phys. Rev. B 86, 094411 (2011). https://doi.org/10.1103/PhysRevB.86.094411
H. Ishizuka, M. Udagawa, and Y. Motome, J. Phys. Soc. Jpn. 81, 113706 (2012). https://doi.org/10.1143/JPSJ.81.113706
G. Chen and M. Hermele, Phys. Rev. B 86, 235129 (2012). https://doi.org/10.1103/PhysRevB.86.235129
M. Udagawa, H. Ishizuka, and Y. Motome, Phys. Rev. Lett. 108, 066406 (2012). https://doi.org/10.1103/PhysRevLett.108.066406
The anomaly in specific heat shows a strong sample dependence. As MIT is sharper, the anomaly is clearly observed. Even when an anomaly in magnetic susceptibility caused by MIT is observed, the specific heat has no clear peak
J. J. Ishikawa, E. C. T. O’ Farrell, and S. Nakatsuji, Phys. Rev. B 85, 245109 (2012). https://doi.org/10.1103/PhysRevB.85.245109
S. Zhao, J. M. Mackie, D. E. MacLaughlin, O. O. Bernal, J. J. Ishikawa, Y. Ohta, and S. Nakatsuji, Phys. Rev. B 83, 180402(R) (2011). https://doi.org/10.1103/PhysRevB.83.180402
K. Tomiyasu, K. Matsuhira, K. Iwasa, M. Watahiki, S. Takagi, M. Wakeshima, Y. Hinatsu, M. Yokoyama, K. Ohoyama, and K. Yamada, J. Phys. Soc. Jpn. 81, 034709 (2012). https://doi.org/10.1143/JPSJ.81.034709
H. Guo, K. Matsuhira, I. Kawasaki, M. Wakeshima, Y. Hinatsu, I. Watanabe, and Z. Xu, Phys. Rev. B 88, 060411(R) (2013). https://doi.org/10.1103/PhysRevB.88.060411
H. Sagayama, D. Uematsu, T, Arima, K. Sugimoto, J. J. Ishikawa, E. O’Farrell, and S. Nakatsuji, Phys. Rev. B 87, 100403(R) (2013). https://doi.org/10.1103/PhysRevB.87.100403
J. Yamaura, K. Ohgushi, H. Ohsumi, T. Hasegawa, I. Yamauchi, K. Sugimoto, S. Takeshita, A. Tokuda, M. Takata, M. Udagawa, M. Takigawa, H. Harima, T. Arima and Z. Hiroi, Phys. Rev. Lett. 108, 247205 (2012). https://doi.org/10.1103/PhysRevLett.108.247205
The XRD measurements for single crystal Nd\(_2\)Ir\(_2\)O\(_7\) were performed by J. Yamaura
T. Hasegawa, N. Ogita, K. Matsuhira, S. Takagi, M. Wakeshima, Y. Hinatsu, and M. Udagawa, J. Phys.: Conf. Ser. 200, 012054 (2010). https://doi.org/10.1088/1742-6596/200/1/012054
M. Sakata, T. Kagayama, K, Shimizu, K. Matsuhira, S. Takagi, M. Wakeshima, and Y. Hinatsu, Phys. Rev. B 83, 041102(R) (2011). https://doi.org/10.1103/PhysRevB.83.041102
The present resistance value of 1 \(\Omega \) approximately corresponds to 5 m\(\Omega cm\) although it is hard to convert the resistance into the resistivity because the shape of sample is not exactly a rectangular parallelepiped. The resistivity of Nd\(_2\)Ir\(_2\)O\(_7\) is roughly twice as large as that of Pr\(_2\)Ir\(_2\)O\(_7\)
F. F. Tafti, J. J. Ishikawa, A. McCollam, S. Nakatsuji, and S. R. Julian, Phys. Rev. B 85, 205104 (2012). https://doi.org/10.1103/PhysRevB.85.205104
S. K. Pandey and L. Maiti, Phys. Rev. B 82, 035110 (2010). https://doi.org/10.1103/PhysRevB.82.035110
F. Ishii et al., J. Phys. Soc. Jpn. 84, 073703 (2015). https://doi.org/10.1143/JPSJ.84.073703
Y. Machida et al., J. Phys. Chem. Solids 66, 1435 (2005). https://doi.org/10.1016/j.jpcs.2005.05.026
S. Nakatsuji et al., J. Phys. Conf. Ser. 320, 012056 (2011). https://doi.org/10.1088/1742-6596/320/1/012056
Y. Tokiwa, J. J. Ishikawa, S. Nakatsuji, P. Gegenwart, Nat. Mater. 13, 356 (2014). https://doi.org/10.1038/nmat3900
D. R. Hamann, Phys. Rev. 158, 570 (1967). https://doi.org/10.1103/PhysRev.158.570
A. C. Hewson, The Kondo Problem of Heavy Fermions (Cambridge University Press, Cambridge, England, 1993). https://doi.org/10.1017/CBO9780511470752
Y. Taguchi et al., Science 291, 2573 (2001). https://doi.org/10.1126/science.1058161
Y. Machida et al., Phys. Rev. Lett. 98, 057203 (2007). https://doi.org/10.1103/PhysRevLett.98.057203
L. Balicas, S. Nakatsuji, Y. Machida and S. Onoda, Phys. Rev. Lett. 106, 217204 (2011). https://doi.org/10.1103/PhysRevLett.106.217204
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Matsuhira, K., Nakatsuji, S. (2021). Anomalous Transport Properties of Pyrochlore Iridates. In: Udagawa, M., Jaubert, L. (eds) Spin Ice. Springer Series in Solid-State Sciences, vol 197. Springer, Cham. https://doi.org/10.1007/978-3-030-70860-3_14
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