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DC Field | Value | Language |
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dc.contributor.author | Koçkar, Hakan | - |
dc.contributor.author | Karaağaç, Öznur | - |
dc.contributor.author | Kuru, Hilal | - |
dc.date.accessioned | 2023-06-08T11:00:16Z | - |
dc.date.available | 2023-06-08T11:00:16Z | - |
dc.date.issued | 2013-04 | - |
dc.identifier.citation | Kalsen, S. vd. (2013). “Properties of electrodeposited CoFeNi/Cu superlattices: The effect of CoFeNi and Cu layers thicknesses”. Journal of Superconductivity and Novel Magnetism, 26(4) Special Issue, 813-817. | en_US |
dc.identifier.issn | 1557-1939 | - |
dc.identifier.issn | 1557-1947 | - |
dc.identifier.uri | https://doi.org/10.1007/s10948-012-1912-7 | - |
dc.identifier.uri | https://link.springer.com/article/10.1007/s10948-012-1912-7 | - |
dc.identifier.uri | http://hdl.handle.net/11452/32980 | - |
dc.description | Bu çalışma, 29 Nisan-04 Mayıs 2012 tarihleri arasında İstanbul[Türkiye]’da düzenlenen 3. International Conference on Superconductivity and Magnetism (ICSM)’da bildiri olarak sunulmuştur. | tr_TR |
dc.description.abstract | CoFeNi/Cu superlattices were grown on Ti substrate by electrodeposition as a function of the ferromagnetic and non-magnetic layer thicknesses. In order to examine the effect of the Cu layer thickness on the film properties, the Cu layer thickness was changed from 0.5 to 6 nm, while the CoFeNi layer thickness was kept constant at 4 nm. Also, for the CoFeNi layer effect, the CoFeNi layer thickness was changed from 2 to 15 nm, while the Cu layer thickness was fixed at 4 nm. The structural analysis studied by X-ray diffraction indicated that the superlattices have face-centered-cubic structure. Magnetic characteristics were investigated by vibrating sample magnetometer. From the hysteresis curves, the coercivity and the saturation magnetization were determined. It was found that the easy-axis of the films is parallel to the film plane. Magnetoresistance measurements were made by the Van der Pauw method at the room temperature with magnetic fields up to +/- 12 kOe. All superlattices exhibited giant magnetoresistance (GMR). As the ferromagnetic layer thickness increased up to 4 nm, the GMR value increases up to 22 % and then decreases. The superlattices saturated at the lower magnetic layers with increasing ferromagnetic layer thickness. The maximum GMR value was obtained to be 22 % for a superlattice with 375[CoFeNi(4 nm)/Cu(4 nm)]. | en_US |
dc.description.sponsorship | Balıkesir Üniversitesi 2005K120170, BAP 2001/02 | tr_TR |
dc.language.iso | en | en_US |
dc.publisher | Springer | en_US |
dc.rights | info:eu-repo/semantics/closedAccess | en_US |
dc.subject | Physics | en_US |
dc.subject | Electrodeposition | en_US |
dc.subject | CoFeNi/Cu superlattices | en_US |
dc.subject | XRD | en_US |
dc.subject | VSM | en_US |
dc.subject | GMR | en_US |
dc.subject | Giant magnetoresistance | en_US |
dc.subject | Growth | en_US |
dc.subject | Electrodeposition | en_US |
dc.subject | Giant magnetoresistance | en_US |
dc.subject | Magnetic materials | en_US |
dc.subject | Saturation magnetization | en_US |
dc.subject | Superlattices | en_US |
dc.subject | X ray diffraction | en_US |
dc.subject | Face-centered-cubic structures | en_US |
dc.subject | Ferromagnetic layer thickness | en_US |
dc.subject | Giant magnetoresistances (GMR) | en_US |
dc.subject | GMR | en_US |
dc.subject | Magnetoresistance measurements | en_US |
dc.subject | Vibrating sample magnetometer | en_US |
dc.subject | VSM | en_US |
dc.subject | XRD | en_US |
dc.subject | Copper | en_US |
dc.title | Properties of electrodeposited CoFeNi/Cu superlattices: The effect of CoFeNi and Cu layers thicknesses | en_US |
dc.type | Article | en_US |
dc.type | Proceedings Paper | en_US |
dc.identifier.wos | 000317014500016 | tr_TR |
dc.identifier.scopus | 2-s2.0-84876470274 | tr_TR |
dc.relation.publicationcategory | Konferans Öğesi - Uluslararası | tr_TR |
dc.contributor.department | Uludağ Üniversitesi/Fen-Edebiyat Fakültesi/Fizik Bölümü. | tr_TR |
dc.relation.bap | BAP | tr_TR |
dc.contributor.orcid | 0000-0001-5648-3230 | tr_TR |
dc.identifier.startpage | 813 | tr_TR |
dc.identifier.endpage | 817 | tr_TR |
dc.identifier.volume | 26 | tr_TR |
dc.identifier.issue | 4, Special Issue | en_US |
dc.relation.journal | Journal of Superconductivity and Novel Magnetism | en_US |
dc.contributor.buuauthor | Kalsen, Sonser | - |
dc.contributor.buuauthor | Alper, Mürsel | - |
dc.contributor.buuauthor | Hacıismailoğlu, Mürşide | - |
dc.contributor.researcherid | AAH-9719-2021 | tr_TR |
dc.contributor.researcherid | AAG-8795-2021 | tr_TR |
dc.relation.collaboration | Yurt içi | tr_TR |
dc.subject.wos | Physics, applied | en_US |
dc.subject.wos | Physics, condensed matter | en_US |
dc.indexed.wos | SCIE | en_US |
dc.indexed.wos | CPCIS | en_US |
dc.indexed.scopus | Scopus | en_US |
dc.wos.quartile | Q3 (Physics, applied) | en_US |
dc.wos.quartile | Q4 (Physics, condensed matter) | en_US |
dc.contributor.scopusid | 55537933800 | tr_TR |
dc.contributor.scopusid | 7005719283 | tr_TR |
dc.contributor.scopusid | 36482867500 | tr_TR |
dc.subject.scopus | Copper; Coercivity; Saturation Magnetization | en_US |
Appears in Collections: | Scopus Web of Science |
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