journal article·2015-10Open access

Disorder effects in the S=1 antiferromagnetic spin ladder CaV2O4

S.R. Guitarra, A. Caneiro, D. Niebieskikwiat

Abstract

Abstract We study the physical properties of the antiferromagnetic spin ladder CaV 2 O 4 (CVO) and the Y-doped related compound Ca 0.9 Y 0.1 V 2 O 4 . In the latter, X-ray diffraction demonstrates the segregation of a small amount of a vanadium–perovskite impurity phase, leading to the formation of V vacancies within the main CVO-type structure. The 1D character of this calcium–vanadite enhances the influence of the vacancies on the electric and magnetic properties of Ca 0.9 Y 0.1 V 2 O 4 . Electrical transport is characterized by a variable-range hopping mechanism determined by the charging energy of nm-sized segments of V chains delimited by V vacancies, i.e. a Coulomb gap is formed at the Fermi level. These vacancies also locally affect the magnetic correlations, breaking the long-range AFM order observed in CaV 2 O 4 and producing exchange bias when the Y-doped sample is cooled with an applied magnetic field.
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Research context

OpenAlex topics: Advanced Condensed Matter Physics · Physics of Superconductivity and Magnetism · Magnetic and transport properties of perovskites and related materials

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References (31)

Show source-provided references
1. I. Affleck, J. Phys: Condens. Matter 1 (1989) 3047; E. Dagotto, Rep. Prog. Phys. 62 (1999) 1525.10.1088/0953-8984/1/19/001 ↗
2. B.F. Decker, J.S. Kasper, Acta Cryst. 10 (1957) 332; P.M. Hill, et al., Acta Cryst. 9 (1956) 981.10.1107/S0365110X56002862 ↗
3. H. Kikuchi, et al., Can. J. Phys. 79 (2001) 1551; H. Fukushima, et al., Prog. Theor. Phys. Suppl. 145 (2002) 72.10.1143/PTPS.145.345 ↗
4. Zong · Phys. Rev. B · 2008 · 77 · 01441210.1103/PhysRevB.77.014412 ↗
5. Niazi · Phys. Rev. B · 2009 · 79 · 10443210.1103/PhysRevB.79.104432 ↗
6. Pieper · Phys. Rev. B · 2009 · 79 · 18040910.1103/PhysRevB.79.180409 ↗
7. Hastings · J. Phys. Chem. Solids · 1967 · 28 · 108910.1016/0022-3697(67)90051-0 ↗
8. T. Hikihara, et al., Phys. Rev. B 63 (2001) 174430; M. Kaburagi, et al., J. Phys. Soc. Jpn. 68 (1999) 3185; T. Hikihara, Can. J. Phys. 79 (2001) 1593.10.1139/p01-096 ↗
9. A. Kolezhuk, et al., Phys. Rev. Lett. 77 (1996) 5142; S. Todo, et al., Phys. Rev. B 64 (2001) 224412.10.1103/PhysRevB.64.224412 ↗
10. Sakurai · Phys. Rev. B · 2008 · 78 · 09441010.1103/PhysRevB.78.094410 ↗
11. Yamaura · Phys. Rev. Lett. · 2007 · 99 · 19660110.1103/PhysRevLett.99.196601 ↗
12. Qian · J. Phys. Soc. Jpn. · 2009 · 78 · 02470910.1143/JPSJ.78.024709 ↗
13. Kasuya · Phys. Rev. B · 1993 · 47 · 619710.1103/PhysRevB.47.6197 ↗
14. Cintolesi · J. Appl. Phys. · 1996 · 79 · 662410.1063/1.361904 ↗
15. N.F. Mott, E.A. Davis, Electronic processes, in: Non-Crystalline Materials, 2nd ed., 1979, Clarendon Press, Oxford.
16. B.I. Shklovskii, A.L. Efros, Electronic Properties of Doped Semiconductors, Springer, New York, 1984; A.L. Efros, B.I. Shklovskii, J. Phys. C 8 (1975) L49.10.1007/978-3-662-02403-4 ↗
17. Fogler · Phys. Rev. B · 2004 · 69 · 03541310.1103/PhysRevB.69.035413 ↗
18. The term “soft” Coulomb gap refers to the fact that the density of states g(ε) actually vanishes only at the Fermi level, and slowly increases with a power-law dependence for energies close to εF.
19. S. Kirkpatrick, Rev. Mod. Phys. 45 (1973) 574; I. Webman, et al., Phys. Rev. B 14 (1976) 4737.10.1103/PhysRevB.14.4737 ↗
20. D.C. Johnston, et al., in: A. Fujimori, Y. Tokura (Eds.), Spectroscopy of Mott Insulators and Correlated Metals, Springer Series in Solid-State Sciences, vol. 119, Springer-Verlag, Berlin Heidelberg, 1995, p. 241, and references therein.
21. H. Sakurai, et al., J. Phys.: Conf. Ser. 273 (2011) 012119.10.1088/1742-6596/273/1/012119 ↗
22. Ajiro · Phys. Rev. B · 1995 · 51 · 939910.1103/PhysRevB.51.9399 ↗
23. Hase · Phys. Rev. Lett. · 1993 · 71 · 405910.1103/PhysRevLett.71.4059 ↗
24. Laukamp · Phys. Rev. B · 1998 · 57 · 1075510.1103/PhysRevB.57.10755 ↗
25. Azuma · Phys. Rev. B · 1997 · 55 · R865810.1103/PhysRevB.55.R8658 ↗
26. For reviews see for example, S. Giri, et al., J. Phys.: Condens. Matter 23 (2011) 073201; J. Nogués, I.K. Schuller, J. Magn. Magn. Mater. 192 (1999) 203.10.1088/0953-8984/23/7/073201 ↗
27. Niebieskikwiat · Phys. Rev. B · 2005 · 72 · 17442210.1103/PhysRevB.72.174422 ↗
28. We note that, with the high purity raw materials used for the sample preparation (99.999%), FM impurities in these chemicals can be ruled out as the origin of the FM component. A thorough calculation indicates that the remanent magnetization in the FC curve in the inset of Fig. 5 is at least two orders of magnitude larger than all possible FM iron impurities could contribute.
29. Zorko · Phys. Rev. B · 2006 · 73 · 10443610.1103/PhysRevB.73.104436 ↗
30. Chern · Phys. Rev. B · 2009 · 80 · 22040510.1103/PhysRevB.80.220405 ↗
31. In samples with small FM regions immersed within a dominant AFM matrix, quantification of the EB field (the displacement of the M–H loop to the left of the origin) is very unreliable due to its large sensitivity to the AFM contribution that must be subtracted from M(H). However, an alternative description of EB can be done through the vertical shift of the remanence, which does not require any manipulation of the data (see D. Niebieskikwiat, M.B. Salamon, Phys. Rev. B 72 (2005) 174422).