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New method for detection of excition Bose condensation using stimulated two-photon emission

机译:激发双光子发射检测兴奋性玻色凝聚的新方法

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An investigation is reported of stimulated two-photon emission by Bose-condensed excitons accompanied by a coherent two-exciton recombination, i.e., by simultaneous recombination of two excitons with opposite momenta leaving unchanged the occupation numbers of exciton states with momenta p non = 0. Raman light scattering (RLS)accompanied by a similar two-exciton recombination (or production of two excitons) is also analyzed. The processes under consideration can occur only if a system contains Bose condensate, so their detection can be used as a new method to reveal Bose condensation of excitons. The recoil momentum, which corresponds to a change in the momentum of the electromagnetic field in the processes, is transferred to phonons or impurities. If the recoil momentum is transmitted to optical phonons with frequency #omega#_(0~s), whose occupation numbers are negligible, and the incident light frequency satisfies #omega# < 2#OMEGA#_-, where #OMEGA#_- = #OMEGA# - #omega#_0~s is the difference frequency and #OMEGA# is the light frequency corresponding to the recombination of an exciton with zero momentum, stimulated two-photon emission and RLS with coherent two-exciton recombination give rise to a line at 2#OMEGA#_- -#omega# and an anti-Stokes component at #omega# + 2#OMEGA#_-, respectively. For #omega# > 2#OMEGA#_- the RLS spectrum contains Stocks and anti-Stokes components at frequencies #omega# +- 2#OMEGA#_-, whereas stimulated two-photon emission is impossible. Formulas for the cross sections at finite temperatures are obtained for the processes under consideration. Our estimates indicate that a spectral line at 2#OMEGA#_- - #omega#, corresponding to the stimulated two-photon emission accompanied by coherent optical phonon-assisted two-exciton recombination can be experimentally detected in Cu_2O.
机译:据报道,玻色凝聚的激子伴随相干的两个激子复合而激发了两个光子的发射,这是通过两个具有相反动量的激子同时复合而使动子态的职业数不变,即p non = 0引起的。还分析了拉曼光散射(RLS)以及类似的两个激子复合(或两个激子的产生)。所考虑的过程只有在系统包含Bose冷凝物的情况下才能发生,因此它们的检测可以用作揭示激子Bose冷凝的新方法。与过程中电磁场的动量变化相对应的反冲动量被转移到声子或杂质中。如果反冲动量被传输到频率为#omega #_(0〜s)的光子,其占有数可以忽略,并且入射光频率满足#omega#<2#OMEGA#_-,其中#OMEGA#_- =#OMEGA#-#omega#_0〜s是差分频率,而#OMEGA#是与零动量的激子复合,激发的双光子发射和相干的二激子复合的RLS相对应的光频率在2#OMEGA#_--#omega#处的一行和在#omega#+ 2#OMEGA#_-处的anti-Stokes组件。对于#omega#> 2#OMEGA#_-,RLS频谱在#omega#+-2#OMEGA#_-频率处包含Stocks和anti-Stokes分量,而不可能激发双光子。对于所考虑的过程,获得了在有限温度下的横截面公式。我们的估计表明,可以在Cu_2O中通过实验检测到对应于受激双光子发射并伴有相干光声子辅助的两个激子复合的2#OMEGA#-#omega#的谱线。

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