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Simulations of return flux of polychromatic laser guide stars based on Bloch equations

机译:基于Bloch方程的多色激光导向恒星返回通量模拟

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Sodium laser guide star (LGS) becomes an essential part in modern astronomical adaptive optics system, especially for the next generation extremely large ground based telescope. The LGS technology has experienced the developmental stages as natural guide star, Rayleigh LGS, sodium LGS and constellation of LGS. The sky coverage is still limited in that the LGS cannot not be used to detect the tip/tilt aberrations. While the polychromatic laser guide star (PLGS) is one of the most effective ways to enlarge the sky coverage to 100%. Previous simulation models are insufficient for the accurate calculation of the return flux, especially for the simulation model of PLGS which is generated by one-photon excitation of mesospheric sodium atoms. The simulation model based on Bloch equations proposed in this paper can be used to compute the return flux of one-photon excited PLGS precisely. Doppler broadening, beam atom exchanging, collisions and recoil are taken into account in the model. The return flux is validated by the return efficiency. The simulation results indicate that with one-photon excitation of sodium atoms, a return efficiency of 330 nm is minimum compared with those of other wavelengths; the saturation power density will decrease with recoil increasing and increase with collision rate increasing; an optimal line-width exists up to maximum the photon return efficiency. In the best case, when the power density is 10 W/m(2) at the sodium layer, the maximum return efficiency at 330 nm is 0.907 photons/s/sr/atom/(W/m(2)) with an optimal laser line-width of 18 MHz.
机译:钠激光导航星(LGS)成为现代天文自适应光学系统的重要组成部分,特别是对于下一代非常大的地面望远镜。 LGS技术已经经历了天然导航星,Rayleigh LGS,LGS和LGS的星座的发展阶段。天空覆盖范围仍然有限,因为LG不能用于检测尖端/倾斜像差。虽然多色激光导灯(PLG)是扩大天空覆盖范围至100%的最有效方法之一。以前的仿真模型对于返回通量的精确计算不足,特别是对于由态化钠原子的单光子激发产生的PLG的模拟模型。基于本文提出的基于BLOCH方程的仿真模型可用于计算单光子激发PLG的返回通量。在模型中考虑了多普勒扩大,束原子交换,碰撞和反冲。返回通量通过返回效率验证。仿真结果表明,对于钠原子的单光子激发,与其他波长相比,返回效率为330nm;饱和功率密度将随着反冲的增加和随着冲突速率的增加而降低;最佳的线宽最大限度地存在于光子返回效率。在最佳情况下,当在钠层的功率密度为10W / m(2)时,330nm的最大收益效率为0.907光子/ s / sr /原子/(w / m(2)),具有最佳激光线宽18 MHz。

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