Abstract
LaFe 11·6 Si 1·4 compounds are annealed at different high temperatures from 1323 to 1623 K. The powder X-ray diffraction patterns show that large amount of NaZn13-type phase begins to be observed in LaFe 11·6 Si 1·4 compound after being annealed at 1423 K for 5 h. In the temperature range from 1423 to 1523 K, the \(\boldsymbol{\alpha} \)-Fe and LaFeSi phases rapidly decrease to form 1:13 phase. LaFeSi phase is rarely observed in the XRD pattern in the LaFe 11·6 Si 1·4 compound annealed at 1523 K (5 h). With annealing temperature increasing to 1573 K and 1673 K, La 5 Si 3 phase is detected, and there is a certain amount of LaFeSi phase when the annealing temperature is 1673 K. The amount of impurity phases in the LaFe 11·6 Si 1·4 compound annealed by the two-stage annealing consisting of high temperature (\(\boldsymbol{>}\)1523 K) and 1523 K is larger than that of the single stage annealing at 1523 K under the same time. According to the results of different high-temperature annealing, LaFe\(_{{\bf 11{\cdot}6}-\boldsymbol{x}}\)Co\(_{\boldsymbol{x}}\)Si 1·4 (\(\boldsymbol{0{\cdot}1} \boldsymbol{\le} \boldsymbol{x} \boldsymbol{\le} \boldsymbol{0{\cdot}8}\)) compounds are annealed at 1523 K (5 h). The main phase is NaZn13-type phase, and the impurity phase is a small amount of \(\boldsymbol{\alpha} \)-Fe in LaFe\(_{{\bf 11{\cdot}6}-\boldsymbol{x}}\)Co\(_{\boldsymbol{x}}\)Si 1·4 compounds. With increase in Co content from \(\boldsymbol{x} \boldsymbol{=} \boldsymbol{0{\cdot}1}\) to \(\boldsymbol{0{\cdot}8}\), the Curie temperature \(\boldsymbol{T}_{\!\boldsymbol{\rm C}}\), goes up from 207 to 285 K. The introduction of Co element weakens the itinerant electron metamagnetic transition, and also results in the change of magnetic transition type from first to second order at about \(\boldsymbol{x = 0{\cdot}5}\). The magnetic entropy change decreases from 19·94 to 4·57 J /kg K with increasing Co concentration at a low magnetic field of 0–2 T. But the magnetic hysteresis loss around \(\boldsymbol{T}_{\!\boldsymbol{\rm C}}\) reduces remarkably from 26·2 J /kg for \(\boldsymbol{x = 0{\cdot}1}\) to 0 J /kg for \(\boldsymbol{x} \boldsymbol{=} \bf 0{\cdot}8\).
Similar content being viewed by others
References
Balli M, Fruchart D, Gignoux D, Rosca M and Miraglia S 2007 J. Magn. Magn. Mater. 313 43
Basso Vittorio, Sasso Ccarlo Paolo, Bertotti Giorgio and LoBue Martino 2006 Int. J. Refrig. 29 1358
Fujieda S, Fujita A and Fukamichi K 2002 Appl. Phys. Lett. 81 1276
Fujita A, Akamatsu Y and Fukamichi K 1999 J. Appl. Phys. 85 4756
Fujita A, Fujieda S, Hasegawa Y and Fukamichi K 2003 Phys. Rev. B67 104416
Hashimoto T, Numasawa T, Shino M and Okada T 1981 J. Cryog. 21 647
Hermann R P, Tegus O, Bruck E, Buschow K H J, de Boer F R, Long G J and Grandjean F 2004 Phys. Rev. B70 214425
Huang M Q, Wallace W E and McHenry M E 1998 J. Appl. Phys. 83 6471
Hu F X, Shen B G, Sun J R, Cheng Z H, Rao G H and Zhang X X 2001 Appl. Phys. Lett. 78 3675
Hu F X, Shen B-G, Sun J-R, Wang G-J and Cheng Z-H 2002 Appl. Phys. Lett. 803 826
Hu F X et al 2003 J. Appl. Phys. 93 5503
Liu X B and Altounian Z 2003 J. Magn. Magn. Mater. 264 209
Liu X B, Altounian Z and Tu G H 2004 J. Phys. Condens. Matter 16 8043
Mandal K, Gutfleischb O, Yan A, Handstein A and Muller K-H 2005 J. Magn. Magn. Mater. 290 673
Mira J et al 2003 Phys. Rev. Lett. 90 097203
Pecharsky Vitalij K and Gschneidner Jr Karl A 2006 Int. J. Refrig. 29 1239
Raghavan V 2001 J. Phase Equilib. 22 158
Sasso Carlo P, Basso Vittorio, LoBue Martino and Bertotti Giorgio 2006 Physica B372 9
Shen J, Li Y-X, Gao B, Sun J-R and Shen B-G 2007 J. Magn. Magn. Mater. 310 2823
Tishin A M 2007 J. Magn. Magn. Mater. 316 351
Wada H and Tanabe Y 2001 Appl. Phys. Lett. 79 3302
Zhu Yaomin, Xie Kun, Song Xiaoping, Sun Zhanbo and Lv Weipeng 2005 J. Alloys Compd. 392 20
Zou J D, Shen B G and Sun J R 2007 J. Phys. Condens. Matter. 19 196220
Author information
Authors and Affiliations
Corresponding author
Rights and permissions
About this article
Cite this article
CHEN, X., CHEN, Y. & TANG, Y. Phase relation of LaFe 11·6 Si 1·4 compounds annealed at different high-temperature and the magnetic property of LaFe 11·6– x Co x Si 1·4 compounds. Bull Mater Sci 35, 175–182 (2012). https://doi.org/10.1007/s12034-012-0273-y
Received:
Revised:
Published:
Issue Date:
DOI: https://doi.org/10.1007/s12034-012-0273-y