Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition

Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition

We have studied thin layers of Ni50-xCoxMn50-yIny alloys on (001) Si substrate obtained by pulsed laser deposition method (PLD) using YAG Nd3+ laser operating at second harmonic. The target was bulk Ni50-xCoxMn50-yIny (x = 5, y = 14.5) alloy prepared by induction melting of pure elements under argon...

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Main Authors: Dubiel Łukasz, Kuzma Marian, Stefaniuk Ireneusz, Wisz Grzegorz, Wal Andrzej
Format: Article
Language:English
Published: EDP Sciences 2017-01-01
Series:EPJ Web of Conferences
Online Access:http://dx.doi.org/10.1051/epjconf/201713302005
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spelling doaj-efdac9771e954bc09d4cc966d958606a2021-08-02T04:07:42ZengEDP SciencesEPJ Web of Conferences2100-014X2017-01-011330200510.1051/epjconf/201713302005epjconf_icsenob2017_02005Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser depositionDubiel Łukasz0Kuzma Marian1Stefaniuk Ireneusz2Wisz Grzegorz3Wal Andrzej4Faculty of Mathematics and Natural Sciences, Department of Biophysics, University of RzeszowFaculty of Mathematics and Natural Sciences, Department of Biophysics, University of RzeszowFaculty of Mathematics and Natural Sciences, Center for Microelectronics and Nanotechnology, University of RzeszowFaculty of Mathematics and Natural Sciences, Department of Experimental Physics, University of RzeszowFaculty of Mathematics and Natural Sciences, Department of Biophysics, University of RzeszowWe have studied thin layers of Ni50-xCoxMn50-yIny alloys on (001) Si substrate obtained by pulsed laser deposition method (PLD) using YAG Nd3+ laser operating at second harmonic. The target was bulk Ni50-xCoxMn50-yIny (x = 5, y = 14.5) alloy prepared by induction melting of pure elements under argon atmosphere. Magnetic properties were investigated on Bruker X band EPR spectrometer (9.36 GHz) at room temperature. The magnetic resonance spectrum consists of non-symmetric lines with resonance field within wide field range (2500-4800 Gs) depending on the orientation of the static field in the plane perpendicular to the layer. Calculated spectroscopic splitting factor g = 2.09.http://dx.doi.org/10.1051/epjconf/201713302005
collection DOAJ
language English
format Article
sources DOAJ
author Dubiel Łukasz
Kuzma Marian
Stefaniuk Ireneusz
Wisz Grzegorz
Wal Andrzej
spellingShingle Dubiel Łukasz
Kuzma Marian
Stefaniuk Ireneusz
Wisz Grzegorz
Wal Andrzej
Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
EPJ Web of Conferences
author_facet Dubiel Łukasz
Kuzma Marian
Stefaniuk Ireneusz
Wisz Grzegorz
Wal Andrzej
author_sort Dubiel Łukasz
title Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
title_short Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
title_full Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
title_fullStr Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
title_full_unstemmed Shape effect in FMR of Ni-Co-Mn-In layers obtained by pulsed laser deposition
title_sort shape effect in fmr of ni-co-mn-in layers obtained by pulsed laser deposition
publisher EDP Sciences
series EPJ Web of Conferences
issn 2100-014X
publishDate 2017-01-01
description We have studied thin layers of Ni50-xCoxMn50-yIny alloys on (001) Si substrate obtained by pulsed laser deposition method (PLD) using YAG Nd3+ laser operating at second harmonic. The target was bulk Ni50-xCoxMn50-yIny (x = 5, y = 14.5) alloy prepared by induction melting of pure elements under argon atmosphere. Magnetic properties were investigated on Bruker X band EPR spectrometer (9.36 GHz) at room temperature. The magnetic resonance spectrum consists of non-symmetric lines with resonance field within wide field range (2500-4800 Gs) depending on the orientation of the static field in the plane perpendicular to the layer. Calculated spectroscopic splitting factor g = 2.09.
url http://dx.doi.org/10.1051/epjconf/201713302005
work_keys_str_mv AT dubielłukasz shapeeffectinfmrofnicomninlayersobtainedbypulsedlaserdeposition
AT kuzmamarian shapeeffectinfmrofnicomninlayersobtainedbypulsedlaserdeposition
AT stefaniukireneusz shapeeffectinfmrofnicomninlayersobtainedbypulsedlaserdeposition
AT wiszgrzegorz shapeeffectinfmrofnicomninlayersobtainedbypulsedlaserdeposition
AT walandrzej shapeeffectinfmrofnicomninlayersobtainedbypulsedlaserdeposition
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