01760nas a2200229   4500008004100000022001400041245010300055210006900158260009500227300001200322490000800334520089600342653003601238653001901274653000801293100002201301700002201323700001401345700001901359700002601378856012601404       2011                        eng d  a0022-459600aRoom temperature ferromagnetism in undoped and Fe doped ZnO nanorods: microwave-assisted synthesis0 aRoom temperature ferromagnetism in undoped and Fe doped ZnO nano  a525 B ST, STE 1900, SAN DIEGO, CA 92101-4495 USAbACADEMIC PRESS INC ELSEVIER SCIENCEcFEB  a391-4000 v1843 a<p>One-dimensional (1D) undoped and Fe doped ZnO nanorods of average length similar to 1 mu m and diameter similar to 50 nm have been obtained using a microwave-assisted synthesis. The magnetization (M) and coercivity (H-c) value obtained for undoped ZnO nanorods at room temperature is similar to 5 X 10(-3) emu/g and similar to 150 Oe, respectively. The Fe doped ZnO samples show significant changes in M -H loop with increasing doping concentration. Both undoped and Fe doped ZnO nanorods exhibit a Curie transition temperature (T-c) above 390 K. Electron spin resonance and Mossbauer spectra indicate the presence of ferric ions. The origin of ferromagnetism in undoped ZnO nanorods is attributed to localized electron spin moments resulting from surface defects/vacancies, where as in Fe doped samples is explained by F center exchange mechanism. (C) 2010 Published by Elsevier Inc.</p>10aDiluted magnetic semiconductors10aNanostructures10aZnO1 aLimaye, Mukta, V.1 aSingh, Shashi, B.1 aDas, Raja1 aPoddar, Pankaj1 aKulkarni, Sulabha, K.  uhttps://library.ncl.res.in/content/room-temperature-ferromagnetism-undoped-and-fe-doped-zno-nanorods-microwave-assisted-0