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Room-temperature 1.54 $\mu$m photoluminescence of Er:O$_x$ centers at extremely low concentration in silicon

机译:室温1.54 $ \ mu $ m Er:O $ _x $的光致发光中心位于   硅中的浓度极低

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摘要

The demand for single photon sources at $\lambda~=~1.54~\mu$m, which followsfrom the consistent development of quantum networks based on commercial opticalfibers, makes Er:O$_x$ centers in Si still a viable resource thanks to theoptical transition of $Er^{3+}~:~^4I_{13/2}~\rightarrow~^4I_{15/2}$. Yet, todate, the implementation of such system remains hindered by its extremely lowemission rate. In this Letter, we explore the room-temperaturephotoluminescence (PL) at the telecomm wavelength of very low implantationdoses of $Er:O_x$ in $Si$. The emitted photons, excited by a $\lambda~=~792~nm$laser in both large areas and confined dots of diameter down to $5~\mu$m, arecollected by an inverted confocal microscope. The lower-bound number ofdetectable emission centers within our diffraction-limited illumination spot isestimated to be down to about 10$^4$, corresponding to an emission rate perindividual ion of about $4~\times~10^{3}$ photons/s.
机译:由于基于商业光纤的量子网络的不断发展,对单光子源的需求为$ \ lambda〜=〜1.54〜\ mu $ m,这使得Er:O $ _x $中心在Si中仍然是可行的资源。 $ Er ^ {3+}〜:〜^ 4I_ {13/2}〜\ rightarrow〜^ 4I_ {15/2} $的过渡。然而,迄今为止,由于其极低的排放率,仍然阻碍了该系统的实施。在这封信中,我们探讨了在$ Si $中非常低的$ Er:O_x $注入剂量的电信波长下的室温光致发光(PL)。通过倒置共聚焦显微镜收集发射的光子,这些光子在大面积中都受到792 nm激光的激发,并且直径缩小到5μm的受限点。衍射极限照明点内可检测到的发射中心的下限估计低至约10 $ ^ 4 $,对应于每个离子的发射速率约为$ 4〜\ times〜10 ^ {3} $光子/ s 。

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