Structural and magnetic properties of La2Ni1−xCoxMnO6 compounds
[Display omitted] •Monoclinic La2Ni1−xCoxMnO6 samples have been prepared using Sol-gel technique.•Rietveld analysis shows an octahedrally distorted double perovskite structure.•The nature of FM interaction and TC depend on the B-site ions.•The short range FM ordering above TC is induced by antisite...
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Veröffentlicht in: | Materials research bulletin 2018-06, Vol.102, p.248-256 |
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creator | Pramanik, Debabrata Mukherjee, S. Dan, Shovan Nandy, A. Pradhan, S.K. Dasgupta, Papri Poddar, Asok Mukherjee, Manabendra Manjunath, B. Joy, P.A. |
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•Monoclinic La2Ni1−xCoxMnO6 samples have been prepared using Sol-gel technique.•Rietveld analysis shows an octahedrally distorted double perovskite structure.•The nature of FM interaction and TC depend on the B-site ions.•The short range FM ordering above TC is induced by antisite disorders.•The existence of any spin glass like phase in such system is discarded.
Single phase monoclinic La2Ni1−xCoxMnO6 (x = 0.2, 0.4, 0.8) compounds, henceforth, referred as LNCxMO (x = 0.2, 0.4, 0.8) have been prepared by Sol–gel technique. The structural study and redox titration suggest that the samples are both La and O deficient. The generated atomic models using Rietveld refined structural parameters show octahedral distortion in the double perovskite structure. X-ray photoelectron spectroscopy (XPS) study has been used to determine the predominant valence states of Ni, Mn and Co ions. LNCxMO (x = 0.2, 0.4) are found to be Heisenberg ferromagnets whereas LNC0.8MO is a phase segregated system. In LNC0.4MO and LNC0.8MO, at temperatures above TC, χ−1(T) curve shows the characteristics of Griffiths phase. The study of ac susceptibility and isothermal remanent magnetization (IRM) discard the possibility of any glassy state at low temperatures. The antiphase boundaries (APBs), antisite disorders (ASDs) and oxygen vacancies play important roles in this system. |
doi_str_mv | 10.1016/j.materresbull.2018.01.040 |
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•Monoclinic La2Ni1−xCoxMnO6 samples have been prepared using Sol-gel technique.•Rietveld analysis shows an octahedrally distorted double perovskite structure.•The nature of FM interaction and TC depend on the B-site ions.•The short range FM ordering above TC is induced by antisite disorders.•The existence of any spin glass like phase in such system is discarded.
Single phase monoclinic La2Ni1−xCoxMnO6 (x = 0.2, 0.4, 0.8) compounds, henceforth, referred as LNCxMO (x = 0.2, 0.4, 0.8) have been prepared by Sol–gel technique. The structural study and redox titration suggest that the samples are both La and O deficient. The generated atomic models using Rietveld refined structural parameters show octahedral distortion in the double perovskite structure. X-ray photoelectron spectroscopy (XPS) study has been used to determine the predominant valence states of Ni, Mn and Co ions. LNCxMO (x = 0.2, 0.4) are found to be Heisenberg ferromagnets whereas LNC0.8MO is a phase segregated system. In LNC0.4MO and LNC0.8MO, at temperatures above TC, χ−1(T) curve shows the characteristics of Griffiths phase. The study of ac susceptibility and isothermal remanent magnetization (IRM) discard the possibility of any glassy state at low temperatures. The antiphase boundaries (APBs), antisite disorders (ASDs) and oxygen vacancies play important roles in this system.</description><identifier>ISSN: 0025-5408</identifier><identifier>EISSN: 1873-4227</identifier><identifier>DOI: 10.1016/j.materresbull.2018.01.040</identifier><language>eng</language><publisher>United States: Elsevier Ltd</publisher><subject>ATOMIC MODELS ; COBALT IONS ; CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY ; Crystal structure ; FERROMAGNETIC MATERIALS ; LANTHANUM COMPLEXES ; Magnetic materials ; MAGNETIC PROPERTIES ; MAGNETIZATION ; MANGANESE IONS ; MONOCLINIC LATTICES ; NICKEL IONS ; Oxides ; PEROVSKITE ; SOL-GEL PROCESS ; Sol–gel chemistry ; SPIN GLASS STATE ; TEMPERATURE RANGE 0065-0273 K ; TITRATION ; VACANCIES ; VALENCE ; X-RAY PHOTOELECTRON SPECTROSCOPY</subject><ispartof>Materials research bulletin, 2018-06, Vol.102, p.248-256</ispartof><rights>2018 Elsevier Ltd</rights><lds50>peer_reviewed</lds50><woscitedreferencessubscribed>false</woscitedreferencessubscribed><orcidid>0000-0003-2125-0976</orcidid></display><links><openurl>$$Topenurl_article</openurl><openurlfulltext>$$Topenurlfull_article</openurlfulltext><thumbnail>$$Tsyndetics_thumb_exl</thumbnail><linktohtml>$$Uhttps://www.sciencedirect.com/science/article/pii/S0025540817333184$$EHTML$$P50$$Gelsevier$$H</linktohtml><link.rule.ids>230,314,776,780,881,3537,27901,27902,65306</link.rule.ids><backlink>$$Uhttps://www.osti.gov/biblio/22803992$$D View this record in Osti.gov$$Hfree_for_read</backlink></links><search><creatorcontrib>Pramanik, Debabrata</creatorcontrib><creatorcontrib>Mukherjee, S.</creatorcontrib><creatorcontrib>Dan, Shovan</creatorcontrib><creatorcontrib>Nandy, A.</creatorcontrib><creatorcontrib>Pradhan, S.K.</creatorcontrib><creatorcontrib>Dasgupta, Papri</creatorcontrib><creatorcontrib>Poddar, Asok</creatorcontrib><creatorcontrib>Mukherjee, Manabendra</creatorcontrib><creatorcontrib>Manjunath, B.</creatorcontrib><creatorcontrib>Joy, P.A.</creatorcontrib><title>Structural and magnetic properties of La2Ni1−xCoxMnO6 compounds</title><title>Materials research bulletin</title><description>[Display omitted]
•Monoclinic La2Ni1−xCoxMnO6 samples have been prepared using Sol-gel technique.•Rietveld analysis shows an octahedrally distorted double perovskite structure.•The nature of FM interaction and TC depend on the B-site ions.•The short range FM ordering above TC is induced by antisite disorders.•The existence of any spin glass like phase in such system is discarded.
Single phase monoclinic La2Ni1−xCoxMnO6 (x = 0.2, 0.4, 0.8) compounds, henceforth, referred as LNCxMO (x = 0.2, 0.4, 0.8) have been prepared by Sol–gel technique. The structural study and redox titration suggest that the samples are both La and O deficient. The generated atomic models using Rietveld refined structural parameters show octahedral distortion in the double perovskite structure. X-ray photoelectron spectroscopy (XPS) study has been used to determine the predominant valence states of Ni, Mn and Co ions. LNCxMO (x = 0.2, 0.4) are found to be Heisenberg ferromagnets whereas LNC0.8MO is a phase segregated system. In LNC0.4MO and LNC0.8MO, at temperatures above TC, χ−1(T) curve shows the characteristics of Griffiths phase. The study of ac susceptibility and isothermal remanent magnetization (IRM) discard the possibility of any glassy state at low temperatures. The antiphase boundaries (APBs), antisite disorders (ASDs) and oxygen vacancies play important roles in this system.</description><subject>ATOMIC MODELS</subject><subject>COBALT IONS</subject><subject>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</subject><subject>Crystal structure</subject><subject>FERROMAGNETIC MATERIALS</subject><subject>LANTHANUM COMPLEXES</subject><subject>Magnetic materials</subject><subject>MAGNETIC PROPERTIES</subject><subject>MAGNETIZATION</subject><subject>MANGANESE IONS</subject><subject>MONOCLINIC LATTICES</subject><subject>NICKEL IONS</subject><subject>Oxides</subject><subject>PEROVSKITE</subject><subject>SOL-GEL PROCESS</subject><subject>Sol–gel chemistry</subject><subject>SPIN GLASS STATE</subject><subject>TEMPERATURE RANGE 0065-0273 K</subject><subject>TITRATION</subject><subject>VACANCIES</subject><subject>VALENCE</subject><subject>X-RAY PHOTOELECTRON SPECTROSCOPY</subject><issn>0025-5408</issn><issn>1873-4227</issn><fulltext>true</fulltext><rsrctype>article</rsrctype><creationdate>2018</creationdate><recordtype>article</recordtype><recordid>eNpN0E1OwzAQhmELgUQp3CGCdcLYcRJnWZVfqdAFsLYcewyu0riyXdQjsOaInIRGZcFqNo9Gn15CLikUFGh9vSrWKmEIGLtt3xcMqCiAFsDhiEyoaMqcM9YckwkAq_KKgzglZzGuAICLppmQ2UsKW522QfWZGky2Vu8DJqezTfAbDMlhzLzNFoo9O_rz9b2b-93TsKwz7dcbvx1MPCcnVvURL_7ulLzd3b7OH_LF8v5xPlvkyDhPeVlCqwztDLa2Q26Erq0qubEUq1YLIarW0BpohZYz5ExbyygXrLKATHe2nJKrw18fk5NRu4T6Q_thQJ0kYwLKtmV7dXNQuJ_y6TCMEgeNxoURGu8kBTnGkyv5P54c40mgch-v_AX7M2mV</recordid><startdate>20180601</startdate><enddate>20180601</enddate><creator>Pramanik, Debabrata</creator><creator>Mukherjee, S.</creator><creator>Dan, Shovan</creator><creator>Nandy, A.</creator><creator>Pradhan, S.K.</creator><creator>Dasgupta, Papri</creator><creator>Poddar, Asok</creator><creator>Mukherjee, Manabendra</creator><creator>Manjunath, B.</creator><creator>Joy, P.A.</creator><general>Elsevier Ltd</general><scope>OTOTI</scope><orcidid>https://orcid.org/0000-0003-2125-0976</orcidid></search><sort><creationdate>20180601</creationdate><title>Structural and magnetic properties of La2Ni1−xCoxMnO6 compounds</title><author>Pramanik, Debabrata ; Mukherjee, S. ; Dan, Shovan ; Nandy, A. ; Pradhan, S.K. ; Dasgupta, Papri ; Poddar, Asok ; Mukherjee, Manabendra ; Manjunath, B. ; Joy, P.A.</author></sort><facets><frbrtype>5</frbrtype><frbrgroupid>cdi_FETCH-LOGICAL-e244t-3309ad1bde9fbe4d8c6fa34df1e59c88859d16015ef42e42cff214825f0e2cbf3</frbrgroupid><rsrctype>articles</rsrctype><prefilter>articles</prefilter><language>eng</language><creationdate>2018</creationdate><topic>ATOMIC MODELS</topic><topic>COBALT IONS</topic><topic>CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY</topic><topic>Crystal structure</topic><topic>FERROMAGNETIC MATERIALS</topic><topic>LANTHANUM COMPLEXES</topic><topic>Magnetic materials</topic><topic>MAGNETIC PROPERTIES</topic><topic>MAGNETIZATION</topic><topic>MANGANESE IONS</topic><topic>MONOCLINIC LATTICES</topic><topic>NICKEL IONS</topic><topic>Oxides</topic><topic>PEROVSKITE</topic><topic>SOL-GEL PROCESS</topic><topic>Sol–gel chemistry</topic><topic>SPIN GLASS STATE</topic><topic>TEMPERATURE RANGE 0065-0273 K</topic><topic>TITRATION</topic><topic>VACANCIES</topic><topic>VALENCE</topic><topic>X-RAY PHOTOELECTRON SPECTROSCOPY</topic><toplevel>peer_reviewed</toplevel><toplevel>online_resources</toplevel><creatorcontrib>Pramanik, Debabrata</creatorcontrib><creatorcontrib>Mukherjee, S.</creatorcontrib><creatorcontrib>Dan, Shovan</creatorcontrib><creatorcontrib>Nandy, A.</creatorcontrib><creatorcontrib>Pradhan, S.K.</creatorcontrib><creatorcontrib>Dasgupta, Papri</creatorcontrib><creatorcontrib>Poddar, Asok</creatorcontrib><creatorcontrib>Mukherjee, Manabendra</creatorcontrib><creatorcontrib>Manjunath, B.</creatorcontrib><creatorcontrib>Joy, P.A.</creatorcontrib><collection>OSTI.GOV</collection><jtitle>Materials research bulletin</jtitle></facets><delivery><delcategory>Remote Search Resource</delcategory><fulltext>fulltext</fulltext></delivery><addata><au>Pramanik, Debabrata</au><au>Mukherjee, S.</au><au>Dan, Shovan</au><au>Nandy, A.</au><au>Pradhan, S.K.</au><au>Dasgupta, Papri</au><au>Poddar, Asok</au><au>Mukherjee, Manabendra</au><au>Manjunath, B.</au><au>Joy, P.A.</au><format>journal</format><genre>article</genre><ristype>JOUR</ristype><atitle>Structural and magnetic properties of La2Ni1−xCoxMnO6 compounds</atitle><jtitle>Materials research bulletin</jtitle><date>2018-06-01</date><risdate>2018</risdate><volume>102</volume><spage>248</spage><epage>256</epage><pages>248-256</pages><issn>0025-5408</issn><eissn>1873-4227</eissn><abstract>[Display omitted]
•Monoclinic La2Ni1−xCoxMnO6 samples have been prepared using Sol-gel technique.•Rietveld analysis shows an octahedrally distorted double perovskite structure.•The nature of FM interaction and TC depend on the B-site ions.•The short range FM ordering above TC is induced by antisite disorders.•The existence of any spin glass like phase in such system is discarded.
Single phase monoclinic La2Ni1−xCoxMnO6 (x = 0.2, 0.4, 0.8) compounds, henceforth, referred as LNCxMO (x = 0.2, 0.4, 0.8) have been prepared by Sol–gel technique. The structural study and redox titration suggest that the samples are both La and O deficient. The generated atomic models using Rietveld refined structural parameters show octahedral distortion in the double perovskite structure. X-ray photoelectron spectroscopy (XPS) study has been used to determine the predominant valence states of Ni, Mn and Co ions. LNCxMO (x = 0.2, 0.4) are found to be Heisenberg ferromagnets whereas LNC0.8MO is a phase segregated system. In LNC0.4MO and LNC0.8MO, at temperatures above TC, χ−1(T) curve shows the characteristics of Griffiths phase. The study of ac susceptibility and isothermal remanent magnetization (IRM) discard the possibility of any glassy state at low temperatures. The antiphase boundaries (APBs), antisite disorders (ASDs) and oxygen vacancies play important roles in this system.</abstract><cop>United States</cop><pub>Elsevier Ltd</pub><doi>10.1016/j.materresbull.2018.01.040</doi><tpages>9</tpages><orcidid>https://orcid.org/0000-0003-2125-0976</orcidid></addata></record> |
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subjects | ATOMIC MODELS COBALT IONS CONDENSED MATTER PHYSICS, SUPERCONDUCTIVITY AND SUPERFLUIDITY Crystal structure FERROMAGNETIC MATERIALS LANTHANUM COMPLEXES Magnetic materials MAGNETIC PROPERTIES MAGNETIZATION MANGANESE IONS MONOCLINIC LATTICES NICKEL IONS Oxides PEROVSKITE SOL-GEL PROCESS Sol–gel chemistry SPIN GLASS STATE TEMPERATURE RANGE 0065-0273 K TITRATION VACANCIES VALENCE X-RAY PHOTOELECTRON SPECTROSCOPY |
title | Structural and magnetic properties of La2Ni1−xCoxMnO6 compounds |
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