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Kouichi Katayama,Kensuke Miyajima,Masaaki Ashida,Tadashi Itoh 한국물리학회 2008 THE JOURNAL OF THE KOREAN PHYSICAL SOCIETY Vol.52 No.5
By the selective excitation of localized excitons in Cd0:8Mn0:2Te at 2 K, a new nonlinear PL band (hereinafter referred to as the X band) appears on the higher energy side of the ordinary magnetic polaron band. When the X band is observed through a linear analyzer with weak magnetic fields (0 - 0.3 T), under a Faraday configuration, it exhibits an oscillatory structure. The energy interval of this oscillation is half that of the Faraday rotation spectrum observed in the transmission spectrum. Therefore, the oscillation is interpreted as being caused by the Faraday rotation of the X-band luminescence, which is first emitted near the surface of excitation, passes through the sample, is re ected back from the rear surface and then passes through the sample again. By the selective excitation of localized excitons in Cd0:8Mn0:2Te at 2 K, a new nonlinear PL band (hereinafter referred to as the X band) appears on the higher energy side of the ordinary magnetic polaron band. When the X band is observed through a linear analyzer with weak magnetic fields (0 - 0.3 T), under a Faraday configuration, it exhibits an oscillatory structure. The energy interval of this oscillation is half that of the Faraday rotation spectrum observed in the transmission spectrum. Therefore, the oscillation is interpreted as being caused by the Faraday rotation of the X-band luminescence, which is first emitted near the surface of excitation, passes through the sample, is re ected back from the rear surface and then passes through the sample again.
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