Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy

碩士 === 國立雲林科技大學 === 材料科技研究所 === 99 === In this study, we focused on the ultrathin CoFeB films with perpendicular magnetic anisotropy (PMA) which can be used for perpendicular magnetic tunnel junctions (pMTJs). The magnetic properties of the films were tuned by varying the CoFeB composition and the a...

Full description

Bibliographic Details
Main Authors: Shin-Hsueh Huang, 黃士學
Other Authors: Te-Ho Wu
Format: Others
Language:zh-TW
Published: 2011
Online Access:http://ndltd.ncl.edu.tw/handle/71170250642387891439
id ndltd-TW-099YUNT5159016
record_format oai_dc
spelling ndltd-TW-099YUNT51590162016-04-08T04:21:57Z http://ndltd.ncl.edu.tw/handle/71170250642387891439 Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy 超薄垂直異向性CoFeB薄膜之磁特性 Shin-Hsueh Huang 黃士學 碩士 國立雲林科技大學 材料科技研究所 99 In this study, we focused on the ultrathin CoFeB films with perpendicular magnetic anisotropy (PMA) which can be used for perpendicular magnetic tunnel junctions (pMTJs). The magnetic properties of the films were tuned by varying the CoFeB composition and the annealing temperatures. Two different compositions of CoFeB were studied: Co40Fe40B20 and Co20Fe60B20. At the first stage of the experiment, we fabricated both the bottom substructure Ta / CoFeB / MgO and the top structure MgO / CoFeB / Ta of pMTJs to look for conditions of PMA. The magnetic properties of the samples were measured by alternating gradient magnetometer (AGM). As for the annealing treatment, the samples were annealed at 300℃ and 350℃ with/without perpendicular applied magnetic field. The results show that the top structures Co40Fe40B20 of thickness 1.4 nm and 1.6 nm retained PMA for both as-deposition and post deposition annealing. The Co20Fe60B20 films of thickness from 1.2 nm to 1.6 nm had PMA from as-deposition condition to post annealing up to 300℃. In contrast with the bottom structures, no strong PMA was present for the top CoFeB structures. To overcome this problem, an ultrathin iron or magnesium layer was inserted between MgO and CoFeB layers. The results show that t adding Fe layer of thickness 0.2 nm together with the post annealing can enhance PMA of the top structures. In addition, we found that the bottom tantalum layer, served as the bottom electrode, becomes crystalline when sputtered on top of ruthenium layer. The crystallinity of tantalum can prevent intermix at Ta-CoFeB interface and reduce the thickness of magnetic dead layer of CoFeB after annealing treatment. Te-Ho Wu 吳德和 2011 學位論文 ; thesis 125 zh-TW
collection NDLTD
language zh-TW
format Others
sources NDLTD
description 碩士 === 國立雲林科技大學 === 材料科技研究所 === 99 === In this study, we focused on the ultrathin CoFeB films with perpendicular magnetic anisotropy (PMA) which can be used for perpendicular magnetic tunnel junctions (pMTJs). The magnetic properties of the films were tuned by varying the CoFeB composition and the annealing temperatures. Two different compositions of CoFeB were studied: Co40Fe40B20 and Co20Fe60B20. At the first stage of the experiment, we fabricated both the bottom substructure Ta / CoFeB / MgO and the top structure MgO / CoFeB / Ta of pMTJs to look for conditions of PMA. The magnetic properties of the samples were measured by alternating gradient magnetometer (AGM). As for the annealing treatment, the samples were annealed at 300℃ and 350℃ with/without perpendicular applied magnetic field. The results show that the top structures Co40Fe40B20 of thickness 1.4 nm and 1.6 nm retained PMA for both as-deposition and post deposition annealing. The Co20Fe60B20 films of thickness from 1.2 nm to 1.6 nm had PMA from as-deposition condition to post annealing up to 300℃. In contrast with the bottom structures, no strong PMA was present for the top CoFeB structures. To overcome this problem, an ultrathin iron or magnesium layer was inserted between MgO and CoFeB layers. The results show that t adding Fe layer of thickness 0.2 nm together with the post annealing can enhance PMA of the top structures. In addition, we found that the bottom tantalum layer, served as the bottom electrode, becomes crystalline when sputtered on top of ruthenium layer. The crystallinity of tantalum can prevent intermix at Ta-CoFeB interface and reduce the thickness of magnetic dead layer of CoFeB after annealing treatment.
author2 Te-Ho Wu
author_facet Te-Ho Wu
Shin-Hsueh Huang
黃士學
author Shin-Hsueh Huang
黃士學
spellingShingle Shin-Hsueh Huang
黃士學
Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
author_sort Shin-Hsueh Huang
title Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
title_short Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
title_full Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
title_fullStr Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
title_full_unstemmed Characteristics of ultrathin CoFeB thin films with perpendicular magnetic anisotropy
title_sort characteristics of ultrathin cofeb thin films with perpendicular magnetic anisotropy
publishDate 2011
url http://ndltd.ncl.edu.tw/handle/71170250642387891439
work_keys_str_mv AT shinhsuehhuang characteristicsofultrathincofebthinfilmswithperpendicularmagneticanisotropy
AT huángshìxué characteristicsofultrathincofebthinfilmswithperpendicularmagneticanisotropy
AT shinhsuehhuang chāobáochuízhíyìxiàngxìngcofebbáomózhīcítèxìng
AT huángshìxué chāobáochuízhíyìxiàngxìngcofebbáomózhīcítèxìng
_version_ 1718219297948434432