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Coherent exciton dynamics: time-resolved polarimetry

机译:相干激子动力学:时间分辨极化

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When coherent optical radiation is incident on a material, the polarisation that is produced within the sample initially has a well defined spatial and temporal phase relationship (or coherence) that is determined by the phase of the exciting field. That coherence persists until it is destroyed by scattering processes within the material. For the excitation of carriers in bulk semiconductors and quantum-confined semiconductor structures (e.g., multiple quantum wells, MQWs), these dephasing times typically range from a few femtoseconds (at room temperature) to a few picoseconds (at liquid helium temperatures). For this reason, the study of elementary coherent processes in semiconductors had to await the relatively recent development of picosecond and femtosecond mode-locked lasers. By comparison, the coherent regimes in atoms and molecules have been studied extensively.
机译:当相干光辐射入射到材料上时,样品内产生的偏振最初具有定义明确的空间和时间相位关系(或相干性),该关系由激发场的相位确定。这种连贯性一直持续到被材料中的散射过程破坏为止。为了激发体半导体和量子限制的半导体结构(例如,多个量子阱,MQW)中的载流子,这些移相时间通常在几飞秒(在室温下)到几皮秒(在液氦温度下)的范围内。由于这个原因,半导体中基本相干过程的研究不得不等待皮秒和飞秒锁模激光器的最新发展。相比之下,原子和分子中的相干态已被广泛研究。

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