TY - JOUR
T1 - Polarization memory effect on nonlinear photoluminescence of semimagnetic semiconductor Cd0.8Mn0.2Te
AU - Katayama, Kouichi
AU - Miyajima, Kensuke
AU - Ashida, Masaaki
AU - Itoh, Tadashi
PY - 2009
Y1 - 2009
N2 - Polarization memory effect was found in the nonlinear photoluminescence band (hereinafter referred to as the X band) of semimagnetic semiconductor Cd0.8Mn0.2Te. The X band appears only when high-density selective excitation of localized exciton has done. The origin of the X band is proposed as the high-spin state of the dense magnetic polarons: in this state, every spins of electrons (holes) point one direction and this spm alignment leads to enhanced magnetic polaron effect. The inclusion of linearly polarized component of the X band, which is excited by the linearly polarized excitation laser, is confirmed from the analyzer dependence of the intensity of the X band. The characteristic oscillatory structure of the X band under magnetic field was explained by Faraday rotation of the X band and the structure is reproduced with supposition of step function like absorption. Polarization memory effect of the X band is confirmed by the behavior of the peak energy of the oscillatory structure; the structure varies with tilt of the polarization plane of the excitation laser. The polarization memory effect of the X band most likely originates from the sufficiently long phase relaxation time of the photo-excited electrons and holes of the X band.
AB - Polarization memory effect was found in the nonlinear photoluminescence band (hereinafter referred to as the X band) of semimagnetic semiconductor Cd0.8Mn0.2Te. The X band appears only when high-density selective excitation of localized exciton has done. The origin of the X band is proposed as the high-spin state of the dense magnetic polarons: in this state, every spins of electrons (holes) point one direction and this spm alignment leads to enhanced magnetic polaron effect. The inclusion of linearly polarized component of the X band, which is excited by the linearly polarized excitation laser, is confirmed from the analyzer dependence of the intensity of the X band. The characteristic oscillatory structure of the X band under magnetic field was explained by Faraday rotation of the X band and the structure is reproduced with supposition of step function like absorption. Polarization memory effect of the X band is confirmed by the behavior of the peak energy of the oscillatory structure; the structure varies with tilt of the polarization plane of the excitation laser. The polarization memory effect of the X band most likely originates from the sufficiently long phase relaxation time of the photo-excited electrons and holes of the X band.
UR - http://www.scopus.com/inward/record.url?scp=63449126901&partnerID=8YFLogxK
U2 - 10.1002/pssc.200879848
DO - 10.1002/pssc.200879848
M3 - Conference article
AN - SCOPUS:63449126901
SN - 1862-6351
VL - 6
SP - 34
EP - 37
JO - Physica Status Solidi (C) Current Topics in Solid State Physics
JF - Physica Status Solidi (C) Current Topics in Solid State Physics
IS - 1
T2 - 8th International Conference on Excitonic Processes in Condensed Matter, EXCON'08
Y2 - 22 June 2008 through 27 June 2008
ER -