在对In As单量子点施加流体静压的实验中,使用了带有压电陶瓷的连续加压装置,在低温连续施加流体静压的情况下,可以调节量子点单激子能量兰移约320 me V。在对不同流体静压下单激子发光的二阶关联函数测量之后,证明流体静压并不影响单...在对In As单量子点施加流体静压的实验中,使用了带有压电陶瓷的连续加压装置,在低温连续施加流体静压的情况下,可以调节量子点单激子能量兰移约320 me V。在对不同流体静压下单激子发光的二阶关联函数测量之后,证明流体静压并不影响单激子发光的单光子特性。同时通过流体静压,可以实现量子点双激子态由反束缚态到束缚态的转变,并且给出了这一过程的偏振分辨光谱图。最后观察到单量子点精细结构劈裂随流体静压的增加而增加,而且精细结构劈裂的增加量可以达到约150μe V。展开更多
Luminescent properties of Tm^(3+)-doped GdYTaO_(4) are studied for exploring their potential applications in temperature and pressure sensing.Two main emission peaks from ^(3)H_(4)→^(3)H_(6) transition of Tm^(3+)are ...Luminescent properties of Tm^(3+)-doped GdYTaO_(4) are studied for exploring their potential applications in temperature and pressure sensing.Two main emission peaks from ^(3)H_(4)→^(3)H_(6) transition of Tm^(3+)are investigated.Intensity ratio between the two peaks evolves exponentially with temperature and has a highest sensitivity of 0.014 K^(−1) at 32 K.The energy difference between the two peaks increases linearly with pressure increasing at a rate of 0.38 meV/GPa.Intensity ratio between the two peaks and their emission lifetimes are also analyzed for discussing the pressure-induced variation of the sample structure.Moreover,Raman spectra recorded under high pressures indicate an isostructural phase transition of GdYTaO_(4) occurring at 4.46 GPa.展开更多
文摘在对In As单量子点施加流体静压的实验中,使用了带有压电陶瓷的连续加压装置,在低温连续施加流体静压的情况下,可以调节量子点单激子能量兰移约320 me V。在对不同流体静压下单激子发光的二阶关联函数测量之后,证明流体静压并不影响单激子发光的单光子特性。同时通过流体静压,可以实现量子点双激子态由反束缚态到束缚态的转变,并且给出了这一过程的偏振分辨光谱图。最后观察到单量子点精细结构劈裂随流体静压的增加而增加,而且精细结构劈裂的增加量可以达到约150μe V。
基金the National Natural Science Foundation of China(Grant No.11804047)the Science and Technology Development Program of Jilin City,China(Grant No.201831733).
文摘Luminescent properties of Tm^(3+)-doped GdYTaO_(4) are studied for exploring their potential applications in temperature and pressure sensing.Two main emission peaks from ^(3)H_(4)→^(3)H_(6) transition of Tm^(3+)are investigated.Intensity ratio between the two peaks evolves exponentially with temperature and has a highest sensitivity of 0.014 K^(−1) at 32 K.The energy difference between the two peaks increases linearly with pressure increasing at a rate of 0.38 meV/GPa.Intensity ratio between the two peaks and their emission lifetimes are also analyzed for discussing the pressure-induced variation of the sample structure.Moreover,Raman spectra recorded under high pressures indicate an isostructural phase transition of GdYTaO_(4) occurring at 4.46 GPa.
