2007/05/31 by Muhammad Naeem, M. Naeem, S. K. Hasanain +2
Materials Science · Physics and Astronomy · #Copper-based nanomaterials and applications #Ga2O3 and related materials #ZnO doping and properties #cond-mat.mtrl-sci #cond-mat.soft
paper · pdf · doi:10.1088/0953-8984/20/02/025210
published as J. Phys.: Condens. Matter 20 (2008) 025210 · 7 pages, 6 figures
openalex publication_date 2007/12/06 · arxiv created 2007/12/08 · arxiv updated 2009/12/01 · openalex created_date 2025/10/10 · openalex updated_date 2026/07/30
The observed correlation of oxygen vacancies and room temperature ferromagnetic ordering in Co doped ZnO 1−δ nanoparticles reported earlier (Naeem et al 2006 Nanotechnology 17 2675–80) has been further explored by transport and optical measurements. In these particles room temperature ferromagnetic ordering had been observed to occur only after annealing in forming gas. In the current work the optical properties have been studied by diffuse-reflection spectroscopy in the ultraviolet–visible (UV–vis) region and the band gap of the Co doped compositions has been found to decrease with Co addition. Reflection minima are observed at the energies characteristic of Co 2+ d–d (tethrahedral symmetry) crystal field transitions, further establishing the presence of Co in substitutional sites. Electrical transport measurements on pelletized samples of the nanoparticles show that the effect of a forming gas is to strongly decrease the resistivity with increasing Co concentration. For the air annealed and non-ferromagnetic samples the variation in the resistivity as a function of Co content are opposite to those observed in the particles prepared in forming gas. The ferromagnetic samples exhibit an apparent change from insulator to metal with increasing temperatures for T >380 K and this change becomes more pronounced with increasing Co content. The magnetic and resistive behaviors are correlated by considering the model by Calderon and Sarma (2007 Ann. Phys. at press) where the ferromagnetism changes from being mediated by polarons in the low temperature insulating region to being mediated by the carriers released from the weakly bound states in the higher temperature metallic region.