Temperature dependent Mueller matrix of magnetized Ni near the Curie temperature
ORAL
Abstract
Optical properties of magnetized Ni are studied in polar configuration. The temperature dependence of the optical constants of magnetized Ni 1000 Å demonstrates an anomaly near the Curie temperature Tc.
Assuming that magnetized Ni is not depolarizing, the MM is derived up to the first order of Voigt parameter from the Jones matrix. Using spectroscopic ellipsometry at an incident angle of 70° and a UHV cryostat we took three dynamic measurements in a temperature range between 400 and 770 K. The experimental MM describes significant changes in the on-diagonal and negligible ones in off-diagonal blocks about Tc. The authors believe that the changes in off-diagonal elements are due to the magneto-optical Kerr effect.
However, the considerable changes of the on-diagonal blocks of the MM indicate that the variations in optical constants about Tc come from the diagonal elements of the dielectric tensor, which is described by Drude response. This means that either the scattering rate or the carrier density changes under magnetization. Furthermore, inverting the direction of the magnetization shows that all elements of the MM depend only on the magnitude of the magnetization, not the direction. This is in contrast to the theoretical MM.
Assuming that magnetized Ni is not depolarizing, the MM is derived up to the first order of Voigt parameter from the Jones matrix. Using spectroscopic ellipsometry at an incident angle of 70° and a UHV cryostat we took three dynamic measurements in a temperature range between 400 and 770 K. The experimental MM describes significant changes in the on-diagonal and negligible ones in off-diagonal blocks about Tc. The authors believe that the changes in off-diagonal elements are due to the magneto-optical Kerr effect.
However, the considerable changes of the on-diagonal blocks of the MM indicate that the variations in optical constants about Tc come from the diagonal elements of the dielectric tensor, which is described by Drude response. This means that either the scattering rate or the carrier density changes under magnetization. Furthermore, inverting the direction of the magnetization shows that all elements of the MM depend only on the magnitude of the magnetization, not the direction. This is in contrast to the theoretical MM.
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Presenters
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Farzin Abadizaman
New Mexico State University, Physics, New Mexico State Univ
Authors
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Farzin Abadizaman
New Mexico State University, Physics, New Mexico State Univ
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Pablo Paradis
Physics, New Mexico State University
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Stefan Zollner
NMSU, Physics, New Mexico State Univ, New Mexico State University, Physics, New Mexico State University