2013
DOI: 10.1117/12.2016676
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Experimental studies of cobalt ferrite nanoparticles doped silica matrix 3D magneto-photonic crystals

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Cited by 2 publications
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“…After preparing the samples, the Faraday rotation cycle was measured using a spectral polarimeter in LT2C laboratory [9],to inspect the orientation of the nanoparticles. When a linearly polarized light wave passes through the sample in the presence of a magnetic field parallel to the propagation of the light, the formers' linear polarization state will convert into an elliptical one and will be characterized by two angles; the Faraday rotation (θ F )and the Faraday ellipticity (ε F ) [9] as can be seen in figure 6.…”
Section: Resultsmentioning
confidence: 99%
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“…After preparing the samples, the Faraday rotation cycle was measured using a spectral polarimeter in LT2C laboratory [9],to inspect the orientation of the nanoparticles. When a linearly polarized light wave passes through the sample in the presence of a magnetic field parallel to the propagation of the light, the formers' linear polarization state will convert into an elliptical one and will be characterized by two angles; the Faraday rotation (θ F )and the Faraday ellipticity (ε F ) [9] as can be seen in figure 6.…”
Section: Resultsmentioning
confidence: 99%
“…When a linearly polarized light wave passes through the sample in the presence of a magnetic field parallel to the propagation of the light, the formers' linear polarization state will convert into an elliptical one and will be characterized by two angles; the Faraday rotation (θ F )and the Faraday ellipticity (ε F ) [9] as can be seen in figure 6. The Faraday rotation was presented as function of the applied magnetic field during the measurement at a specific wavelength chosen according to less noise factor and more signal intensity of the Faraday rotation and ellipticity cycles.…”
Section: Resultsmentioning
confidence: 99%
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