Influence of y substitution in gd2-xyxfe17 compounds
Gd2−xYxFe17 (x = 0; 0.6; 1.0) compounds were prepared by standard arc melting method. Thereafter, samples were subjected to annealing for two days at T=1273 K, finishing with quenching to 273 K. The samples were cut into small portions to perform structural, electrical, and thermal characterization....
- Autores:
-
Tróchez, J. C.
Solano Mazo, Cristian Adolfo
Ortiz Muñoz, E.
- Tipo de recurso:
- Article of journal
- Fecha de publicación:
- 2014
- Institución:
- Corporación Universidad de la Costa
- Repositorio:
- REDICUC - Repositorio CUC
- Idioma:
- eng
- OAI Identifier:
- oai:repositorio.cuc.edu.co:11323/1718
- Acceso en línea:
- https://hdl.handle.net/11323/1718
https://repositorio.cuc.edu.co/
- Palabra clave:
- Gd2−xYxFe17
Fusion method
Standard bow
Samples
Tc
Temperature
- Rights
- openAccess
- License
- http://purl.org/coar/access_right/c_abf2
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|
dc.title.eng.fl_str_mv |
Influence of y substitution in gd2-xyxfe17 compounds |
title |
Influence of y substitution in gd2-xyxfe17 compounds |
spellingShingle |
Influence of y substitution in gd2-xyxfe17 compounds Gd2−xYxFe17 Fusion method Standard bow Samples Tc Temperature |
title_short |
Influence of y substitution in gd2-xyxfe17 compounds |
title_full |
Influence of y substitution in gd2-xyxfe17 compounds |
title_fullStr |
Influence of y substitution in gd2-xyxfe17 compounds |
title_full_unstemmed |
Influence of y substitution in gd2-xyxfe17 compounds |
title_sort |
Influence of y substitution in gd2-xyxfe17 compounds |
dc.creator.fl_str_mv |
Tróchez, J. C. Solano Mazo, Cristian Adolfo Ortiz Muñoz, E. |
dc.contributor.author.spa.fl_str_mv |
Tróchez, J. C. Solano Mazo, Cristian Adolfo Ortiz Muñoz, E. |
dc.subject.eng.fl_str_mv |
Gd2−xYxFe17 Fusion method Standard bow Samples Tc Temperature |
topic |
Gd2−xYxFe17 Fusion method Standard bow Samples Tc Temperature |
description |
Gd2−xYxFe17 (x = 0; 0.6; 1.0) compounds were prepared by standard arc melting method. Thereafter, samples were subjected to annealing for two days at T=1273 K, finishing with quenching to 273 K. The samples were cut into small portions to perform structural, electrical, and thermal characterization. Heat flow and Curie temperature (Tc) arise from measurements of thermal properties through Differential Scanning Calorimetry (DSC), structural properties were tested via X-ray diffraction (XRD) at T=273 K, electrical characterization was carried out through the Impedance Spectrometry (IS) method, upon zero applied magnetic field and temperature range between 300 K<T<500 K. Results show that Tc decreases when Y concentration increases. Tc is obtained as the maximum temperature variation of heat flux. The Gd2Fe17 compound shows two endothermic heat flux peaks; this fact can be attributed to not identifying an impurity phase from X-ray diffraction measurements. From Rietveld refined data, the crystal structure for all compounds is established, resulting in a hexagonal Th2Ni17-type structure. Measurements of impedance spectrometry as function of frequency were analyzed in terms of equivalent circuit method, finding that for temperatures below Tc they fit according to the model composed of one RL and two RC parallel circuits, in contrast to temperatures above Tc given by the model that consists of only two RC parallel circuits. |
publishDate |
2014 |
dc.date.issued.none.fl_str_mv |
2014 |
dc.date.accessioned.none.fl_str_mv |
2018-11-22T15:32:30Z |
dc.date.available.none.fl_str_mv |
2018-11-22T15:32:30Z |
dc.type.spa.fl_str_mv |
Artículo de revista |
dc.type.coar.fl_str_mv |
http://purl.org/coar/resource_type/c_2df8fbb1 |
dc.type.coar.spa.fl_str_mv |
http://purl.org/coar/resource_type/c_6501 |
dc.type.content.spa.fl_str_mv |
Text |
dc.type.driver.spa.fl_str_mv |
info:eu-repo/semantics/article |
dc.type.redcol.spa.fl_str_mv |
http://purl.org/redcol/resource_type/ART |
dc.type.version.spa.fl_str_mv |
info:eu-repo/semantics/acceptedVersion |
format |
http://purl.org/coar/resource_type/c_6501 |
status_str |
acceptedVersion |
dc.identifier.issn.spa.fl_str_mv |
1742-6596 |
dc.identifier.uri.spa.fl_str_mv |
https://hdl.handle.net/11323/1718 |
dc.identifier.instname.spa.fl_str_mv |
Corporación Universidad de la Costa |
dc.identifier.reponame.spa.fl_str_mv |
REDICUC - Repositorio CUC |
dc.identifier.repourl.spa.fl_str_mv |
https://repositorio.cuc.edu.co/ |
identifier_str_mv |
1742-6596 Corporación Universidad de la Costa REDICUC - Repositorio CUC |
url |
https://hdl.handle.net/11323/1718 https://repositorio.cuc.edu.co/ |
dc.language.iso.none.fl_str_mv |
eng |
language |
eng |
dc.rights.accessrights.spa.fl_str_mv |
info:eu-repo/semantics/openAccess |
dc.rights.coar.spa.fl_str_mv |
http://purl.org/coar/access_right/c_abf2 |
eu_rights_str_mv |
openAccess |
rights_invalid_str_mv |
http://purl.org/coar/access_right/c_abf2 |
dc.publisher.spa.fl_str_mv |
Universidad de la Costa CUC |
institution |
Corporación Universidad de la Costa |
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spelling |
Tróchez, J. C.Solano Mazo, Cristian AdolfoOrtiz Muñoz, E.2018-11-22T15:32:30Z2018-11-22T15:32:30Z20141742-6596https://hdl.handle.net/11323/1718Corporación Universidad de la CostaREDICUC - Repositorio CUChttps://repositorio.cuc.edu.co/Gd2−xYxFe17 (x = 0; 0.6; 1.0) compounds were prepared by standard arc melting method. Thereafter, samples were subjected to annealing for two days at T=1273 K, finishing with quenching to 273 K. The samples were cut into small portions to perform structural, electrical, and thermal characterization. Heat flow and Curie temperature (Tc) arise from measurements of thermal properties through Differential Scanning Calorimetry (DSC), structural properties were tested via X-ray diffraction (XRD) at T=273 K, electrical characterization was carried out through the Impedance Spectrometry (IS) method, upon zero applied magnetic field and temperature range between 300 K<T<500 K. Results show that Tc decreases when Y concentration increases. Tc is obtained as the maximum temperature variation of heat flux. The Gd2Fe17 compound shows two endothermic heat flux peaks; this fact can be attributed to not identifying an impurity phase from X-ray diffraction measurements. From Rietveld refined data, the crystal structure for all compounds is established, resulting in a hexagonal Th2Ni17-type structure. Measurements of impedance spectrometry as function of frequency were analyzed in terms of equivalent circuit method, finding that for temperatures below Tc they fit according to the model composed of one RL and two RC parallel circuits, in contrast to temperatures above Tc given by the model that consists of only two RC parallel circuits.Tróchez, J. C.-0e799f1a-c6f8-47d5-8220-247c4122eb53-0Solano Mazo, Cristian Adolfo-0000-0002-7683-4656-600Ortiz Muñoz, E.-a8dc74e1-6c9e-4e0c-a44e-56b2c8be7e98-0engUniversidad de la Costa CUCGd2−xYxFe17Fusion methodStandard bowSamplesTcTemperatureInfluence of y substitution in gd2-xyxfe17 compoundsArtículo de revistahttp://purl.org/coar/resource_type/c_6501http://purl.org/coar/resource_type/c_2df8fbb1Textinfo:eu-repo/semantics/articlehttp://purl.org/redcol/resource_type/ARTinfo:eu-repo/semantics/acceptedVersioninfo:eu-repo/semantics/openAccesshttp://purl.org/coar/access_right/c_abf2PublicationORIGINALINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdfINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdfapplication/pdf66643https://repositorio.cuc.edu.co/bitstreams/4458c5f4-1c6e-4999-b27d-dfb33d97efc2/download9703ff7350d773935eafbd181cce8552MD51LICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorio.cuc.edu.co/bitstreams/49330f3d-86f1-40c7-be5d-505f917b26bc/download8a4605be74aa9ea9d79846c1fba20a33MD52THUMBNAILINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.jpgINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.jpgimage/jpeg48620https://repositorio.cuc.edu.co/bitstreams/9d467914-756e-4783-a084-ae953dc5dcc5/downloada5347981377dfc7d6e3adbce58f9a1f8MD54TEXTINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.txtINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.txttext/plain1528https://repositorio.cuc.edu.co/bitstreams/564e4f2f-1fbc-4eab-bcf8-f5b313cb48b7/downloadb6e68c6973e329cbe26b7b7bb141c990MD5511323/1718oai:repositorio.cuc.edu.co:11323/17182024-09-17 14:11:33.931open.accesshttps://repositorio.cuc.edu.coRepositorio de la Universidad de la Costa CUCrepdigital@cuc.edu.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 |