机构:
Uppsala Univ, Dept Phys & Astron, Box 516, S-75120 Uppsala, SwedenLeibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
Oppeneer, Peter M.
[3
]
Ognev, Alexey V.
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机构:
Far Eastern Fed Univ, Sch Nat Sci, Vladivostok 690950, RussiaLeibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
Ognev, Alexey V.
[4
]
Samardak, Alexander S.
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机构:
Far Eastern Fed Univ, Sch Nat Sci, Vladivostok 690950, Russia
Ural State Univ, Natl Res South, Chelyabinsk 454080, RussiaLeibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
Samardak, Alexander S.
[4
,5
]
Soldatov, Ivan V.
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机构:
Leibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
Tech Univ Darmstadt, Inst Mat Wissensch, D-64287 Darmstadt, GermanyLeibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
Soldatov, Ivan V.
[1
,6
]
机构:
[1] Leibniz Inst Solid State & Mat Res IFW Dresden, Helmholtzstr 20, D-01069 Dresden, Germany
[2] Tech Univ Dresden, Inst Mat Sci, D-01062 Dresden, Germany
[3] Uppsala Univ, Dept Phys & Astron, Box 516, S-75120 Uppsala, Sweden
[4] Far Eastern Fed Univ, Sch Nat Sci, Vladivostok 690950, Russia
[5] Ural State Univ, Natl Res South, Chelyabinsk 454080, Russia
[6] Tech Univ Darmstadt, Inst Mat Wissensch, D-64287 Darmstadt, Germany
In conventional Kerr and Faraday microscopy, the sample is illuminated with plane-polarized light, and a magnetic domain contrast is generated by an analyzer making use of the Kerr or Faraday rotation. Here, we demonstrate possibilities of analyzer-free magneto-optical microscopy based on magnetization-dependent intensity modulations of the light. (i) The transverse Kerr effect can be applied for in-plane magnetized material, as demonstrated for an FeSi sheet. (ii) Illuminating that sample with circularly polarized light leads to a domain contrast with a different symmetry from the conventional Kerr contrast. (iii) Circular polarization can also be used for perpendicularly magnetized material, as demonstrated for garnet and ultrathin CoFeB films. (iv) Plane-polarized light at a specific angle can be employed for both in-plane and perpendicular media. (v) Perpendicular light incidence leads to a domain contrast on in-plane materials that is quadratic in the magnetization and to a domain boundary contrast. (vi) Domain contrast can even be obtained without a polarizer. In cases (ii) and (iii), the contrast is generated by magnetic circular dichroism (i.e., differential absorption of left- and right-circularly polarized light induced by magnetization components along the direction of light propagation), while magnetic linear dichroism (differential absorption of linearly polarized light induced by magnetization components transverse to propagation) is responsible for the contrast in case (v). The domain-boundary contrast is due to the magneto-optical gradient effect. A domain-boundary contrast can also arise by interference of phase-shifted magneto-optical amplitudes. An explanation of these contrast phenomena is provided in terms of Maxwell-Fresnel theory. (C) 2021 Author(s). All article content, except where otherwise noted, is licensed under a Creative Commons Attribution (CC BY) license