2019
DOI: 10.1016/j.jmmm.2018.10.083
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MOKE study of magnetic compensation in polycrystalline gadolinium iron garnet thin film

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Cited by 16 publications
(6 citation statements)
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“…The compensation temperature proves to be a sensitive measure of defect populations, and the presence of several types of point defects likely explains the discrepancies between compensation temperatures found in many reports of REIG thin films versus bulk values. [18,19,22,39,40] The stabilization of large defect populations in epitaxial films has important implications for the design of REIGs for spintronic applications and more generally for the engineering of complex oxide films for electronics and other applications. Defect engineering through co-deposition or control of growth parameters, therefore, emerges as a powerful method to control the magnetic properties of REIGs.…”
Section: Discussionmentioning
confidence: 99%
See 1 more Smart Citation
“…The compensation temperature proves to be a sensitive measure of defect populations, and the presence of several types of point defects likely explains the discrepancies between compensation temperatures found in many reports of REIG thin films versus bulk values. [18,19,22,39,40] The stabilization of large defect populations in epitaxial films has important implications for the design of REIGs for spintronic applications and more generally for the engineering of complex oxide films for electronics and other applications. Defect engineering through co-deposition or control of growth parameters, therefore, emerges as a powerful method to control the magnetic properties of REIGs.…”
Section: Discussionmentioning
confidence: 99%
“…[ 18,38 ] PLD‐grown single‐crystal DyIG/GGG had T comp = 190 K [ 22 ] whereas bulk DyIG has T comp = 220 K. [ 38 ] PLD‐grown polycrystalline GdIG showed T comp = 377 K, ≈100 K higher than that of bulk GdIG. [ 40 ] Sputtered Tb‐deficient TbIG films showed T comp 25–60 K below that of bulk TbIG. [ 41 ] In other studies, the T comp of thin films matched that of bulk such as polycrystalline DyIG [ 22 ] and single crystal and polycrystalline TbIG.…”
Section: Introductionmentioning
confidence: 99%
“…Recently PMA was achieved in polycrystalline films of europium iron garnet (EuIG) on (0001) quartz, Dy 3− x Bi x Fe 5− y Ga y O 12 on glass, and for Dy 3− x Ce x Fe 5− y Al y O 12 on Si due to a dominant magnetoelastic anisotropy. A mixed anisotropy has also been reported for Gd 3 Fe 5 O 12 on Si . To obtain PMA, a combination of positive (negative) magnetostriction and an in‐plane compressive (tensile) strain state is required.…”
Section: Introductionmentioning
confidence: 93%
“…A mixed anisotropy has also been reported for Gd 3 Fe 5 O 12 on Si. [42] To obtain PMA, a combination of positive (negative) magnetostriction and an in-plane compressive (tensile) strain state is required. Since iron garnets have a relatively high thermal expansion coefficient (e.g., 10.4 10 −6 K −1 for YIG [43] ), the garnet will be under in-plane tensile strain on many common substrates after annealing, with the exception of high thermal expansion materials such as (0001)-oriented quartz.…”
Section: Introductionmentioning
confidence: 99%
“…Through replacing a nonmagnetic Re element (Y, for example) by the other Re elements with large magnetic moments (Gd, [41,42] Eu, [43] Ho, [44,45] Tb, [46,47] and Dy [48,49] in particular), additional source of magnetism, together with many intriguing properties are introduced. [50][51][52][53][54][55] Using Gd 3 Fe 5 O 12 (GdIG) as an example, it contains three magnetic sublattices, [56,57] the a-site Fe 3+ ions octahedrally coordinated with the surrounding O 2− ions, the d-site Fe 3+ ions tetrahedrally coordinated with the O 2− ions, and the c-site Gd 3+ ions dodecahedrally coordinated with the O 2− ions.…”
Section: Introductionmentioning
confidence: 99%