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| 024 | 7 | _ | |2 DOI |a 10.1016/j.ssc.2009.11.030 |
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| 082 | _ | _ | |a 540 |
| 084 | _ | _ | |2 WoS |a Physics, Condensed Matter |
| 100 | 1 | _ | |0 P:(DE-HGF)0 |a Phan, M.H. |b 0 |
| 245 | _ | _ | |a Complex magnetic phases in LuFe2O4 |
| 260 | _ | _ | |a New York, NY [u.a.] |b Elsevier Science |c 2010 |
| 336 | 7 | _ | |a Journal Article |0 PUB:(DE-HGF)16 |2 PUB:(DE-HGF) |
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| 440 | _ | 0 | |0 5564 |a Solid State Communications |v 150 |x 0038-1098 |y 7 |
| 500 | _ | _ | |a The work at USF was supported by DOE BES Physical Behavior of Materials Program through grant number DE-FG02-07ER46438. The research at ORNL was sponsored by the Division of Materials Sciences and Engineering, Office of Basic Energy Sciences, US Department of Energy. |
| 520 | _ | _ | |a DC magnetization and AC susceptibility measurements on LuFe2O4 single crystals reveal a ferrimagnetic transition at 240 K followed by additional magnetic transitions at 225 K and 170 K, separating cluster glass phases, and a kinetically arrested state below 55 K. The origin of giant magnetic coercivity is attributed to the collective freezing of ferrimagnetic clusters and enhanced domain wall pinning associated with a structural transition at 170 K. Magnetocaloric effect measurements provide additional vital information about the multiple magnetic transitions and the glassy states. Our results lead to the emergence of a complex magnetic phase diagram in LuFe2O4. (C) 2009 Elsevier Ltd. All rights reserved. |
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| 653 | 2 | 0 | |2 Author |a Magnetic oxide |
| 653 | 2 | 0 | |2 Author |a Cluster glass |
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| 653 | 2 | 0 | |2 Author |a Magnetic susceptibility |
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| 773 | _ | _ | |0 PERI:(DE-600)1467698-9 |a 10.1016/j.ssc.2009.11.030 |g Vol. 150 |q 150 |t Solid state communications |v 150 |x 0038-1098 |y 2010 |
| 856 | 7 | _ | |u http://dx.doi.org/10.1016/j.ssc.2009.11.030 |
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