Magnetismo de baixa dimensão no Fe1-xCuxNbO4

Detalhes bibliográficos
Ano de defesa: 2023
Autor(a) principal: Evaristo, Diego da Silva
Orientador(a): Macêdo, Marcelo Andrade
Banca de defesa: Não Informado pela instituição
Tipo de documento: Tese
Tipo de acesso: Acesso aberto
Idioma: por
Instituição de defesa: Não Informado pela instituição
Programa de Pós-Graduação: Pós-Graduação em Física
Departamento: Não Informado pela instituição
País: Não Informado pela instituição
Palavras-chave em Português:
Palavras-chave em Inglês:
Área do conhecimento CNPq:
Link de acesso: https://ri.ufs.br/jspui/handle/riufs/18248
Resumo: In the present work, iron and copper niobates (Fe1xCuxNbO4 with x = 0 - 0.15 and 0.25) were prepared by the modified solid state method and characterized by diffraction of X-rays (XRD), scanning electron microscopy (SEM/EDX), Mössbauer spectroscopy (EM), temperature-dependent (10 - 1000 K) and magnetic field Raman spectroscopy (ER), magnetic measurements as a function of temperature (M-T, 1.8 - 1000 K) and magnetic field (M-H) and measurements of AC magnetic susceptibility as a function of frequency and DC field. The results (DRXs and ER) confirm the phase (mFeNbO4), as well as the local influences caused by the insertion of Cu ions. SEM suggests a non-uniform particle size distribution with a mean diameter of 1.62 µm. Magnetic analyzes (M - H and M - T) confirmed that the FeNbO4 structure presents an antiferromagnetic (AFM) ordering state, with temperature TN ~36.81 K and revealed an antiferromagnetic-ferrimagnetic transition (AFM-FIM) due to the replacement of Fe3+ ions by Cu2+ ions in Fe1-xCuxNbO4 (x > 0.05), which remains above ambient temperature. The analysis by study of the magnetocaloric effect (EMC), through the analysis of the temperature-dependent variation of magnetic entropy (SM) in different magnetic fields (1 to 7 T), confirms the transition of the magnetic order from AFM to FIM, with a transition temperature of T´N = 38 K, for sample Fe0.75Cu0.25NbO4. AC magnetic susceptibility measurements (Xac(T,f ) and Xac(T,f ,H)), show that, at low temperatures, the insertion of Cu2+ causes an increase in magnetic anisotropy and, in the absence of long range order (LRO) it promotes slow magnetic relaxation processes, between 52 and 163 K, which strongly resemble the behavior of a single-chain magnet (SCM). The magnetic studies at high temperatures showed the magnetic transition FIM-PM (ferrimagnetic-paramagnetic) with TC = 908 K, through measurements of temperature-dependent magnetization (M-T) and evidenced by Raman spectroscopy dependent on temperature and field. We also report the direct observation of the magnetic excitation of two magnons and the couplings of magnons-phonons, spin-phonons in the FIM-PM magnetic transition region for Fe0.75Cu0.25NbO4, via temperature-dependent Raman spectroscopy.
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spelling Evaristo, Diego da SilvaMacêdo, Marcelo Andrade2023-09-04T16:42:31Z2023-09-04T16:42:31Z2023-07-28EVARISTO, Diego da Silva. Magnetismo de baixa dimensão no Fe1-xCuxNbO4. 2023. 133 f. Tese (Doutorado em Física) – Universidade Federal de Sergipe, São Cristóvão, 2023.https://ri.ufs.br/jspui/handle/riufs/18248In the present work, iron and copper niobates (Fe1xCuxNbO4 with x = 0 - 0.15 and 0.25) were prepared by the modified solid state method and characterized by diffraction of X-rays (XRD), scanning electron microscopy (SEM/EDX), Mössbauer spectroscopy (EM), temperature-dependent (10 - 1000 K) and magnetic field Raman spectroscopy (ER), magnetic measurements as a function of temperature (M-T, 1.8 - 1000 K) and magnetic field (M-H) and measurements of AC magnetic susceptibility as a function of frequency and DC field. The results (DRXs and ER) confirm the phase (mFeNbO4), as well as the local influences caused by the insertion of Cu ions. SEM suggests a non-uniform particle size distribution with a mean diameter of 1.62 µm. Magnetic analyzes (M - H and M - T) confirmed that the FeNbO4 structure presents an antiferromagnetic (AFM) ordering state, with temperature TN ~36.81 K and revealed an antiferromagnetic-ferrimagnetic transition (AFM-FIM) due to the replacement of Fe3+ ions by Cu2+ ions in Fe1-xCuxNbO4 (x > 0.05), which remains above ambient temperature. The analysis by study of the magnetocaloric effect (EMC), through the analysis of the temperature-dependent variation of magnetic entropy (SM) in different magnetic fields (1 to 7 T), confirms the transition of the magnetic order from AFM to FIM, with a transition temperature of T´N = 38 K, for sample Fe0.75Cu0.25NbO4. AC magnetic susceptibility measurements (Xac(T,f ) and Xac(T,f ,H)), show that, at low temperatures, the insertion of Cu2+ causes an increase in magnetic anisotropy and, in the absence of long range order (LRO) it promotes slow magnetic relaxation processes, between 52 and 163 K, which strongly resemble the behavior of a single-chain magnet (SCM). The magnetic studies at high temperatures showed the magnetic transition FIM-PM (ferrimagnetic-paramagnetic) with TC = 908 K, through measurements of temperature-dependent magnetization (M-T) and evidenced by Raman spectroscopy dependent on temperature and field. We also report the direct observation of the magnetic excitation of two magnons and the couplings of magnons-phonons, spin-phonons in the FIM-PM magnetic transition region for Fe0.75Cu0.25NbO4, via temperature-dependent Raman spectroscopy.No presente trabalho, niobatos de ferro e cobre (Fe1-xCuxNbO4 com x = 0 - 0.15 e 0.25), foram preparados pelo método do estado sólido modificado e caracterizados por difração de raios X (DRX), microscopia eletrônica de varredura (MEV/EDX), espectroscopia Mössbauer (EM), espectroscopia Raman (ER) dependente da temperatura (10 - 1000 K) e campo magnético, medidas magnéticas em função da temperatura (M-T, 1.8 - 1000 K) e campo magnético (M-H) e medidas de suscetibilidade magnética AC em função da frequência e campo DC. Os resultados (DRXs e ER) confirmam a fase (m-FeNbO4), bem como, as influências locais provocadas pela inserção de íons de Cu. O MEV sugere uma distribuição não uniforme de tamanho de partículas com diâmetro médio de 1.62 µm. Análises magnéticas (M - H e M - T ) confirmaram que a estrutura FeNbO4 apresenta um estado de ordenação antiferromagnético (AFM), com temperatura TN ~36,81 K e revelaram uma transição antiferromagnética- ferrimagnética (AFM-FIM) em função da substituição de íons de Fe3+ por íons Cu2+ na Fe1-xCuxNbO4 (x > 0.05), que permanece acima da temperatura ambiente. A análise por estudo do efeito magnetocalórico (EMC), através da análise da variação da entropia magnética dependente da temperatura (delta SM) em diferentes campos magnéticos (1 a 7 T), confirma a transição da ordem magnética de AFM para FIM, com uma temperatura de transição de T´N = 38 K, para amostra Fe0.75Cu0.25NbO4. Medidas de suscetibilidade magnética AC (Xac(T,f ) e Xac(T,f ,H)), mostram que, em baixas temperaturas, a inserção de Cu2+ provoca um aumento na anisotropia magnética e, na ausência de ordem de longo alcance (LRO) promove processos de relaxações magnéticas lentos, entre 52 e 163 K, que se assemelham fortemente ao comportamento de um magneto da cadeia única (SCM). Os estudos magnéticos em altas temperaturas mostraram a transição magnética FIM-PM (ferrimagnética-paramagnética) com T C = 908 K, através de medidas de magnetização dependente da temperatura (M - T) e evidenciada por espectroscopia Raman dependente da temperatura e campo. Relatamos também a observação direta da excitação magnética de dois mágnons e dos acoplamentos mágnons-fônons, spin-fônons na região de transição magnética FIM-PM para Fe0.75Cu0.25NbO4, via espectroscopia Raman dependente da temperatura.Conselho Nacional de Pesquisa e Desenvolvimento Científico e Tecnológico - CNPqSão CristóvãoporTransição de fase magnéticaDinâmica de spin lentoEfeito HopkinsonAcoplamento spin-fônonMágnonAcoplamento mágnon-fônonMagnetic phase transitionSlow spin dynamicsHopkinson effectSpin-phonon couplingMagnonMagnon-phonon couplingCIENCIAS EXATAS E DA TERRA::FISICAMagnetismo de baixa dimensão no Fe1-xCuxNbO4info:eu-repo/semantics/publishedVersioninfo:eu-repo/semantics/doctoralThesisPós-Graduação em FísicaUniversidade Federal de Sergipe (UFS)reponame:Repositório Institucional da UFSinstname:Universidade Federal de Sergipe (UFS)instacron:UFSinfo:eu-repo/semantics/openAccessLICENSElicense.txtlicense.txttext/plain; charset=utf-81475https://ri.ufs.br/jspui/bitstream/riufs/18248/1/license.txt098cbbf65c2c15e1fb2e49c5d306a44cMD51ORIGINALDIEGO_SILVA_EVARISTO.pdfDIEGO_SILVA_EVARISTO.pdfapplication/pdf39438889https://ri.ufs.br/jspui/bitstream/riufs/18248/2/DIEGO_SILVA_EVARISTO.pdfc7ca9340a67eb303956a808241dc1a87MD52TEXTDIEGO_SILVA_EVARISTO.pdf.txtDIEGO_SILVA_EVARISTO.pdf.txtExtracted texttext/plain234057https://ri.ufs.br/jspui/bitstream/riufs/18248/3/DIEGO_SILVA_EVARISTO.pdf.txteb806589731dd36bb4fed53eca15d217MD53THUMBNAILDIEGO_SILVA_EVARISTO.pdf.jpgDIEGO_SILVA_EVARISTO.pdf.jpgGenerated Thumbnailimage/jpeg1346https://ri.ufs.br/jspui/bitstream/riufs/18248/4/DIEGO_SILVA_EVARISTO.pdf.jpg77c932153a353a491869d5413afc829bMD54riufs/182482023-09-04 13:42:50.168oai:ufs.br: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Repositório InstitucionalPUBhttps://ri.ufs.br/oai/requestrepositorio@academico.ufs.bropendoar:2023-09-04T16:42:50Repositório Institucional da UFS - Universidade Federal de Sergipe (UFS)false
dc.title.pt_BR.fl_str_mv Magnetismo de baixa dimensão no Fe1-xCuxNbO4
title Magnetismo de baixa dimensão no Fe1-xCuxNbO4
spellingShingle Magnetismo de baixa dimensão no Fe1-xCuxNbO4
Evaristo, Diego da Silva
Transição de fase magnética
Dinâmica de spin lento
Efeito Hopkinson
Acoplamento spin-fônon
Mágnon
Acoplamento mágnon-fônon
Magnetic phase transition
Slow spin dynamics
Hopkinson effect
Spin-phonon coupling
Magnon
Magnon-phonon coupling
CIENCIAS EXATAS E DA TERRA::FISICA
title_short Magnetismo de baixa dimensão no Fe1-xCuxNbO4
title_full Magnetismo de baixa dimensão no Fe1-xCuxNbO4
title_fullStr Magnetismo de baixa dimensão no Fe1-xCuxNbO4
title_full_unstemmed Magnetismo de baixa dimensão no Fe1-xCuxNbO4
title_sort Magnetismo de baixa dimensão no Fe1-xCuxNbO4
author Evaristo, Diego da Silva
author_facet Evaristo, Diego da Silva
author_role author
dc.contributor.author.fl_str_mv Evaristo, Diego da Silva
dc.contributor.advisor1.fl_str_mv Macêdo, Marcelo Andrade
contributor_str_mv Macêdo, Marcelo Andrade
dc.subject.por.fl_str_mv Transição de fase magnética
Dinâmica de spin lento
Efeito Hopkinson
Acoplamento spin-fônon
Mágnon
Acoplamento mágnon-fônon
topic Transição de fase magnética
Dinâmica de spin lento
Efeito Hopkinson
Acoplamento spin-fônon
Mágnon
Acoplamento mágnon-fônon
Magnetic phase transition
Slow spin dynamics
Hopkinson effect
Spin-phonon coupling
Magnon
Magnon-phonon coupling
CIENCIAS EXATAS E DA TERRA::FISICA
dc.subject.eng.fl_str_mv Magnetic phase transition
Slow spin dynamics
Hopkinson effect
Spin-phonon coupling
Magnon
Magnon-phonon coupling
dc.subject.cnpq.fl_str_mv CIENCIAS EXATAS E DA TERRA::FISICA
description In the present work, iron and copper niobates (Fe1xCuxNbO4 with x = 0 - 0.15 and 0.25) were prepared by the modified solid state method and characterized by diffraction of X-rays (XRD), scanning electron microscopy (SEM/EDX), Mössbauer spectroscopy (EM), temperature-dependent (10 - 1000 K) and magnetic field Raman spectroscopy (ER), magnetic measurements as a function of temperature (M-T, 1.8 - 1000 K) and magnetic field (M-H) and measurements of AC magnetic susceptibility as a function of frequency and DC field. The results (DRXs and ER) confirm the phase (mFeNbO4), as well as the local influences caused by the insertion of Cu ions. SEM suggests a non-uniform particle size distribution with a mean diameter of 1.62 µm. Magnetic analyzes (M - H and M - T) confirmed that the FeNbO4 structure presents an antiferromagnetic (AFM) ordering state, with temperature TN ~36.81 K and revealed an antiferromagnetic-ferrimagnetic transition (AFM-FIM) due to the replacement of Fe3+ ions by Cu2+ ions in Fe1-xCuxNbO4 (x > 0.05), which remains above ambient temperature. The analysis by study of the magnetocaloric effect (EMC), through the analysis of the temperature-dependent variation of magnetic entropy (SM) in different magnetic fields (1 to 7 T), confirms the transition of the magnetic order from AFM to FIM, with a transition temperature of T´N = 38 K, for sample Fe0.75Cu0.25NbO4. AC magnetic susceptibility measurements (Xac(T,f ) and Xac(T,f ,H)), show that, at low temperatures, the insertion of Cu2+ causes an increase in magnetic anisotropy and, in the absence of long range order (LRO) it promotes slow magnetic relaxation processes, between 52 and 163 K, which strongly resemble the behavior of a single-chain magnet (SCM). The magnetic studies at high temperatures showed the magnetic transition FIM-PM (ferrimagnetic-paramagnetic) with TC = 908 K, through measurements of temperature-dependent magnetization (M-T) and evidenced by Raman spectroscopy dependent on temperature and field. We also report the direct observation of the magnetic excitation of two magnons and the couplings of magnons-phonons, spin-phonons in the FIM-PM magnetic transition region for Fe0.75Cu0.25NbO4, via temperature-dependent Raman spectroscopy.
publishDate 2023
dc.date.accessioned.fl_str_mv 2023-09-04T16:42:31Z
dc.date.available.fl_str_mv 2023-09-04T16:42:31Z
dc.date.issued.fl_str_mv 2023-07-28
dc.type.status.fl_str_mv info:eu-repo/semantics/publishedVersion
dc.type.driver.fl_str_mv info:eu-repo/semantics/doctoralThesis
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dc.identifier.citation.fl_str_mv EVARISTO, Diego da Silva. Magnetismo de baixa dimensão no Fe1-xCuxNbO4. 2023. 133 f. Tese (Doutorado em Física) – Universidade Federal de Sergipe, São Cristóvão, 2023.
dc.identifier.uri.fl_str_mv https://ri.ufs.br/jspui/handle/riufs/18248
identifier_str_mv EVARISTO, Diego da Silva. Magnetismo de baixa dimensão no Fe1-xCuxNbO4. 2023. 133 f. Tese (Doutorado em Física) – Universidade Federal de Sergipe, São Cristóvão, 2023.
url https://ri.ufs.br/jspui/handle/riufs/18248
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