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....

Full description

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:
http://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
id RCUC2_8751dcb1483a9b116b91f68f02f7c349
oai_identifier_str oai:repositorio.cuc.edu.co:11323/1718
network_acronym_str RCUC2
network_name_str REDICUC - Repositorio CUC
repository_id_str
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
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dc.identifier.issn.spa.fl_str_mv 1742-6596
dc.identifier.uri.spa.fl_str_mv http://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
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https://repositorio.cuc.edu.co/
dc.language.iso.none.fl_str_mv eng
language eng
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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.64bf83df14f41dd24d815fe13cf4e4ddSolano Mazo, Cristian Adolfo3bd992030b0ea553f4f8d17173d49869Ortiz Muñoz, E.4d1549121b81bd49284ca06267488cd92018-11-22T15:32:30Z2018-11-22T15:32:30Z20141742-6596http://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.engUniversidad 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_abf2ORIGINALINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdfINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdfapplication/pdf66643https://repositorio.cuc.edu.co/bitstream/11323/1718/1/INFLUENCE%20OF%20Y%20SUBSTITUTION%20IN%20GD2-XYXFE17%20COMPOUNDS.pdf9703ff7350d773935eafbd181cce8552MD51open accessLICENSElicense.txtlicense.txttext/plain; charset=utf-81748https://repositorio.cuc.edu.co/bitstream/11323/1718/2/license.txt8a4605be74aa9ea9d79846c1fba20a33MD52open accessTHUMBNAILINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.jpgINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.jpgimage/jpeg48620https://repositorio.cuc.edu.co/bitstream/11323/1718/4/INFLUENCE%20OF%20Y%20SUBSTITUTION%20IN%20GD2-XYXFE17%20COMPOUNDS.pdf.jpga5347981377dfc7d6e3adbce58f9a1f8MD54open accessTEXTINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.txtINFLUENCE OF Y SUBSTITUTION IN GD2-XYXFE17 COMPOUNDS.pdf.txttext/plain1528https://repositorio.cuc.edu.co/bitstream/11323/1718/5/INFLUENCE%20OF%20Y%20SUBSTITUTION%20IN%20GD2-XYXFE17%20COMPOUNDS.pdf.txtb6e68c6973e329cbe26b7b7bb141c990MD55open access11323/1718oai:repositorio.cuc.edu.co:11323/17182023-12-14 16:29:59.608open accessRepositorio Universidad de La Costabdigital@metabiblioteca.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