Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO

Oriented M-type hexaferrite thin films are deposited using the alternating target laser ablation deposition (ATLAD) technique utilizing PbO and Fe<sub>2</sub>O<sub>3</sub> targets. Crystallographic, dc magnetic, and microwave characterization results confirming the presence o...

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spelling ndltd-NEU--neu-3305442016-04-25T16:14:07ZEpitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbOOriented M-type hexaferrite thin films are deposited using the alternating target laser ablation deposition (ATLAD) technique utilizing PbO and Fe<sub>2</sub>O<sub>3</sub> targets. Crystallographic, dc magnetic, and microwave characterization results confirming the presence of a hexagonal PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> phase are presented. We conclude that the ATLAD technique holds great promise for layer by layer deposition of various hexaferrite materials, the properties of which can be adjusted by varying the composition of the targets as well as the number of laser shots from each target during the deposition process. This would provide control over the uniaxial anisotropy fields and saturation magnetization values that was not possible in the conventional single target LAD technique.http://hdl.handle.net/2047/d20002214
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description Oriented M-type hexaferrite thin films are deposited using the alternating target laser ablation deposition (ATLAD) technique utilizing PbO and Fe<sub>2</sub>O<sub>3</sub> targets. Crystallographic, dc magnetic, and microwave characterization results confirming the presence of a hexagonal PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> phase are presented. We conclude that the ATLAD technique holds great promise for layer by layer deposition of various hexaferrite materials, the properties of which can be adjusted by varying the composition of the targets as well as the number of laser shots from each target during the deposition process. This would provide control over the uniaxial anisotropy fields and saturation magnetization values that was not possible in the conventional single target LAD technique.
title Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
spellingShingle Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
title_short Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
title_full Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
title_fullStr Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
title_full_unstemmed Epitaxial growth of PbFe<sub>1</sub><sub>2</sub>O<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of Fe<sub>2</sub>O<sub>3</sub> and PbO
title_sort epitaxial growth of pbfe<sub>1</sub><sub>2</sub>o<sub>1</sub><sub>9</sub> thin films by alternating target laser ablation deposition of fe<sub>2</sub>o<sub>3</sub> and pbo
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url http://hdl.handle.net/2047/d20002214
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