Paramagnetic anisotropy of Co-doped ZnO single crystal

Applied Physics Letters

Volumn 89, Issue 11, 2006, Pages

  Li, Wei ^a   Kang, Qingqing ^a   Lin, Zhang ^a   Chu, Wangsheng ^c   Chen, Dongliang ^c   Wu, Ziyu ^c   Yan, Yu ^b   Chen, Dagui ^a   Huang, Feng ^a  

^a FUJIAN INSTITUTE OF RESEARCH ON THE STRUCTURE OF MATTER   (China)

^b JILIN UNIVERSITY   (China)

^c NONE

Author keywords

[No Author keywords available]

Indexed keywords

CRYSTAL GROWTH; MAGNETIC ANISOTROPY; PARAMAGNETIC MATERIALS; X RAY ANALYSIS; ZINC OXIDE;

NEAR-EDGE STRUCTURE SPECTRA; PARAMAGNETIC ANISOTROPY; TETRAHEDRAL COORDINATION; ZNO LATTICE;

SINGLE CRYSTALS;

EID: 33748681959     PISSN: 00036951     EISSN: None     Source Type: Journal    
DOI: 10.1063/1.2352726     Document Type: Article

References (17)

1. S. A. Wolf, D. D. Awschalom, R. A. Buhrman, J. M. Daughton, S. von Molnar, M. L. Roukes, A. Y. Chtchelkanova, and D. M. Treger, Science 294, 1488 (2001).
2. T. Dielt, H. Ohno, F. Matsukura, J. Cibert, and D. Ferrand, Science 287, 1019 (2000).
3. K. Sato and H. Katayam-Yoshida, Semicond. Sci. Technol. 17, 367 (2002).
4. K. Ueda, H. Tabata, and T. Kawai, Appl. Phys. Lett. 79, 988 (2001).
5. M. Venkatesan, C. B. Fitzgerald, J. G. Lunney, and J. M. D. Coey, Phys. Rev. Lett. 93, 177206 (2004).
6. J. H. Park, M. G. Kim, H. M. Jang, and S. Ryu, Appl. Phys. Lett. 84, 1338 (2004).
7. M. Bouloudenine, N. Viart, S. Colis, and A. Dinia, Chem. Phys. Lett. 397, 73 (2004).
8. J. M. D. Coey, M. Venkatesan, C. B. Fitzgerald, L. S. Dorneles, P. Stamenov, and J. G. Lunney, J. Magn. Magn. Mater. 290-291, 1405 (2005).
9. W. Prellier, A. Fouchet, B. Mercey, Ch. Simon, and B. Raveau, Appl. Phys. Lett. 82, 3490 (2003).
10. D. A. Schwartz, N. S. Norberg, Q. P. Nguyen, J. M. Parker, and D. M. Gamelin, J. Am. Chem. Soc. 125, 13205 (2003).
11. D. P. Norton, S. J. Pearton, A. F. Hebard, N. Theodoropoulou, L. A. Boatner, and R. G. Wilson, Appl. Phys. Lett. 82, 239 (2003).
12. J. M. D. Coey, M. Venkatesan, and C. B. Fitzgerald, Nat. Mater. 4, 173 (2005).
13. H. Zhang, E. Shi, Z. Chen, X. Liu, and B. Xiao, Solid State Commun. 137, 272 (2006).
14. Both transmission and fluorescence modes are two standard modes for XAFS measurements. The fluorescence mode is a complementary in XAFS measurement, for increasing the signal-to-noise ratio for dilute samples.
15. (a) E. A. Stern, M. Newville, B. Ravel, Y. Yacoby, and D. Haskel, Physica B 208&209, 117 (1995);
16. (b) M. Newville, P. Livins, Y. Yacoby, J. J. Rehr, and E. A. Stern, Phys. Rev. B 47, 14126 (1993).
17. P. Sati, R. Hayn, R. Kuzian, S. Régnier, S. Schäfer, A. Stepanov, C. Morhain, C. Deparis, M. Laügt, M. Goiran, and Z. Golacki, Phys. Rev. Lett. 96, 017203 (2006).