Noncollinear magnetic phases of a triangular-lattice antiferromagnet and of doped CuFeO2

Physical Review B - Condensed Matter and Materials Physics

Volumn 81, Issue 2, 2010, Pages

  Fishman, Randy S ^a   Okamoto, Satoshi ^a  

^a OAK RIDGE NATIONAL LABORATORY   (United States)

Author keywords

[No Author keywords available]

Indexed keywords

EID: 77954790008     PISSN: 10980121     EISSN: 1550235X     Source Type: Journal    
DOI: 10.1103/PhysRevB.81.020402     Document Type: Article

References (30)

1. D. I. Khomskii, J. Magn. Magn. Mater. 306, 1 (2006) 10.1016/j.jmmm.2006. 01.238
2. S.-W. Cheong and M. Mostovoy, Nature Mater. 6, 13 (2007). 10.1038/nmat1804
3. H. Katsura, N. Nagaosa, and A. V. Balatsky, Phys. Rev. Lett. 95, 057205 (2005) 10.1103/PhysRevLett.95.057205
4. M. Mostovoy, Phys. Rev. Lett. 96, 067601 (2006). 10.1103/PhysRevLett.96. 067601
5. T. Nakajima, S. Mitsuda, S. Kanetsuki, K. Prokes, A. Podlesnyak, H. Kimura, and Y. Noda, J. Phys. Soc. Jpn. 76, 043709 (2007) 10.1143/JPSJ.76.043709
6. T. Nakajima, S. Mitsuda, S. Kanetsuki, K. Tanaka, K. Fujii, N. Terada, M. Soda, M. Matsuura, and K. Hirota, Phys. Rev. B 77, 052401 (2008). 10.1103/PhysRevB.77.052401
7. T. Nakajima, S. Mitsuda, T. Inami, N. Terada, H. Ohsumi, K. Prokes, and A. Podlesnyak, Phys. Rev. B 78, 024106 (2008). 10.1103/PhysRevB.78.024106
8. N. Terada, T. Nakajima, S. Mitsuda, H. Kitazawa, K. Kaneko, and N. Metoki, Phys. Rev. B 78, 014101 (2008). 10.1103/PhysRevB.78.014101
9. A. H. Arkenbout, T. T. M. Palstra, T. Siegrist, and T. Kimura, Phys. Rev. B 74, 184431 (2006) 10.1103/PhysRevB.74.184431
10. K. Taniguchi, N. Abe, T. Takenobu, Y. Iwasa, and T. Arima, Phys. Rev. Lett. 97, 097203 (2006). 10.1103/PhysRevLett.97.097203
11. C. Jia, S. Onoda, N. Nagaosa, and J. H. Han, Phys. Rev. B 74, 224444 (2006). 10.1103/PhysRevB.74.224444
12. T. Arima, J. Phys. Soc. Jpn. 76, 073702 (2007). 10.1143/JPSJ.76.073702
13. In a three-dimensional crystal, the instability and ordering wave vectors all have a z component of 3/2 in units of 2 π / c, where the separation between layers is c / 3. In (H, K, L) notation, Q (0.21, 0.21, 3 / 2), Q ′ = 2 π x - Q (0.29, 0.29, 3 / 2), the third harmonic of Q is equivalent to (0.37, 0.37, 3/2), and the third harmonic of Q ′ is equivalent to (0.13, 0.13, 3/2).
14. T. Takagi and M. Mekata, J. Phys. Soc. Jpn. 64, 4609 (1995). 10.1143/JPSJ.64.4609
15. S. Mitsuda, H. Yoshizawa, N. Yaguchi, and M. Mekata, J. Phys. Soc. Jpn. 60, 1885 (1991). 10.1143/JPSJ.60.1885
16. M. Mekata, N. Yaguchi, T. Takagi, T. Sugino, S. Mitsuda, H. Yoshizawa, N. Hosoito, and T. Shinjo, J. Phys. Soc. Jpn. 62, 4474 (1993). 10.1143/JPSJ.62.4474
17. N. Terada, S. Mitsuda, Y. Oohara, H. Yoshizawa, and H. Takei, J. Magn. Magn. Mater. 272-276, e997 (2004) 10.1016/j.jmmm.2003.12.509
18. N. Terada, S. Mitsuda, K. Prokes, O. Suzuki, H. Kitazawa, and H. A. Katori, Phys. Rev. B 70, 174412 (2004) 10.1103/PhysRevB.70.174412
19. N. Terada, S. Mitsuda, T. Fujii, and D. Petitgrand, J. Phys. Condens. Matter 19, 145241 (2007). 10.1088/0953-8984/19/14/145241
20. F. Ye, J. A. Fernandez-Baca, R. S. Fishman, Y. Ren, H. J. Kang, Y. Qiu, and T. Kimura, Phys. Rev. Lett. 99, 157201 (2007) 10.1103/PhysRevLett.99.157201
21. R. S. Fishman, F. Ye, J. A. Fernandez-Baca, J. T. Haraldsen, and T. Kimura, Phys. Rev. B 78, 140407 (R) (2008). 10.1103/PhysRevB.78.140407
22. R. S. Fishman, J. Appl. Phys. 103, 07B109 (2008). 10.1063/1.2834428
23. S. Kanetsuki, S. Mitsuda, T. Nakajima, D. Anazawa, H. A. Katori, and K. Prokes, J. Phys. Condens. Matter 19, 145244 (2007). 10.1088/0953-8984/19/14/ 145244
24. S. Seki, Y. Yamasaki, Y. Shiomi, S. Iguchi, Y. Onose, and Y. Tokura, Phys. Rev. B 75, 100403 (R) (2007). 10.1103/PhysRevB.75.100403
25. J. T. Haraldsen, M. Swanson, G. Alvarez, and R. S. Fishman, Phys. Rev. Lett. 102, 237204 (2009). 10.1103/PhysRevLett.102.237204
26. M. Swanson, J. T. Haraldsen, and R. S. Fishman, Phys. Rev. B 79, 184413 (2009). 10.1103/PhysRevB.79.184413
27. N. Terada, S. Mitsuda, H. Ohsumi, and K. Tajima, J. Phys. Soc. Jpn. 75, 023602 (2006) 10.1143/JPSJ.75.023602
28. N. Terada, Y. Tanaka, Y. Tabata, K. Katsumata, A. Kikkawa, and S. Mitsuda, J. Phys. Soc. Jpn. 75, 113702 (2006). 10.1143/JPSJ.75.113702
29. An expansion of the lattice in the x direction will also suppress the magnitude of J 1 (1) compared to J 1 (2). However, a uniform change in J 1 (1) (with wave vector q = 0) does not produce any additional elastic peaks.
30. F. Ye, Y. Ren, Q. Huang, J. A. Fernandez-Baca, P. Dai, J. W. Lynn, and T. Kimura, Phys. Rev. B 73, 220404 (R) (2006). 10.1103/PhysRevB.73.220404