论文标题
C $ _ {2}^{ - } $的光谱和离子温度法使用激光冷却过渡
Spectroscopy and ion thermometry of C$_{2}^{-}$ using laser-cooling transitions
论文作者
论文摘要
到目前为止尚未实现的激光冷却分子阴离子的先决条件是对冷却方案中相关过渡频率的确切知识。为了确定这些频率,我们提出了一种多功能方法,该方法使用一个泵和一个光检查光束。我们将这种方法应用于c $ _ {2} ^{ - } $,并研究电子基态和第二个电子兴奋状态之间的激光冷却过渡,在其各自的振动基础水平,$ b ^{2}σ_{u}σ_{u} ^{u} ^{+} ^{+}(v = 0)(v = 0)提出了r(0),r(2)和p(2)过渡的测量值,以基于WaveMeter的精度确定过渡频率$ 0.7 \ times10^{ - 3} $ cm $^{ - 1} $或20 MHz。解决了自旋旋转拆分,可以更精确地确定分裂常数为$γ'= 7.15(19)\ times10^{ - 3} $ cm $ $^{ - 1} $和$γ'= 4.10(27)\ times10(27)\ times10^{ - 3} $ cm $ $ cm $^{ - 1} $} $} $} $} $} $。这些结果用于表征该实验中使用的低温16极束陷阱中的离子。由氦气缓冲液气体冷却的离子的平移和旋转温度源自多普勒宽度和测量过渡的振幅比。结果支持常见的观察结果,即由于微功能下的碰撞加热,尤其是在低温下,转化温度高于缓冲气温的温度。此外,旋转温度明显低于转化的测量,这与C $ _ {2}^{ - } $的质量加权碰撞温度的观点相符。
A prerequisite for laser cooling a molecular anion, which has not been achieved so far, is the precise knowledge of the relevant transition frequencies in the cooling scheme. To determine these frequencies we present a versatile method that uses one pump and one photodetachment light beam. We apply this approach to C$_{2}^{-}$ and study the laser cooling transitions between the electronic ground state and the second electronic excited state in their respective vibrational ground levels, $B ^{2} Σ_{u} ^{+}(v=0) \leftarrow X ^{2} Σ_{g} ^{+}(v=0) $. Measurements of the R(0), R(2), and P(2) transitions are presented, which determine the transition frequencies with a wavemeter-based accuracy of $0.7\times10^{-3}$ cm$^{-1}$ or 20 MHz. The spin-rotation splitting is resolved, which allows for a more precise determination of the splitting constants to $γ' = 7.15(19)\times10^{-3}$ cm$^{-1}$ and $γ'' = 4.10(27)\times10^{-3}$ cm$^{-1}$. These results are used to characterize the ions in the cryogenic 16-pole wire trap employed in this experiment. The translational and rotational temperature of the ions cooled by helium buffer gas are derived from the Doppler widths and the amplitude ratios of the measured transitions. The results support the common observation that the translational temperature is higher than the buffer gas temperature due to collisional heating under micromotion, in particular at low temperatures. Additionally, a rotational temperature significantly lower than the translational is measured, which agrees with the notion that the mass weighted collision temperature of the C$_{2}^{-}$-He system defines the internal rotational state population.