2017
DOI: 10.1007/978-3-319-65436-2_4
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Exciton Spin Dynamics in Semiconductor Quantum Dots

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“…The degrees of circular and linear polarization (DCP and DLP, respectively) are useful quantitative tools for characterizing the EFS of semiconductor materials and are central to this work; we define them in the usual convention as DCP = ( I σ+ – I σ– )/( I σ+ + I σ– ), whatever the circular polarization of the excitation, where I σ+ ( I σ– ) is the intensity of σ + (σ – ) circularly polarized component of the emission and DLP = ( I // – I ⊥ )/( I // + I ⊥ ) , with I // and I ⊥ denoting the intensity of the emission analyzed in a direction parallel or perpendicular to the linearly polarized excitation. In nanoparticles, the application of a strong magnetic field induces a Zeeman splitting in the exciton states which manifests itself as a contrast between σ + and σ – emission, under σ + (σ – ) excitation …”
Section: Results and Discussionmentioning
confidence: 99%
“…The degrees of circular and linear polarization (DCP and DLP, respectively) are useful quantitative tools for characterizing the EFS of semiconductor materials and are central to this work; we define them in the usual convention as DCP = ( I σ+ – I σ– )/( I σ+ + I σ– ), whatever the circular polarization of the excitation, where I σ+ ( I σ– ) is the intensity of σ + (σ – ) circularly polarized component of the emission and DLP = ( I // – I ⊥ )/( I // + I ⊥ ) , with I // and I ⊥ denoting the intensity of the emission analyzed in a direction parallel or perpendicular to the linearly polarized excitation. In nanoparticles, the application of a strong magnetic field induces a Zeeman splitting in the exciton states which manifests itself as a contrast between σ + and σ – emission, under σ + (σ – ) excitation …”
Section: Results and Discussionmentioning
confidence: 99%