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Influence of chirping the Raman lasers in an atom gravimeter: phase shifts due to the Raman light shift and to the finite speed of light

机译:拉曼激光器在原子重力仪中的啁啾影响:相位   由于拉曼光移动和有限的光速而发生偏移

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摘要

We present here an analysis of the influence of the frequency dependence ofthe Raman laser light shifts on the phase of a Raman-type atom gravimeter.Frequency chirps are applied to the Raman lasers in order to compensate gravityand ensure the resonance of the Raman pulses during the interferometer. We showthat the change in the Raman light shift when this chirp is applied only to oneof the two Raman lasers is enough to bias the gravity measurement by a fractionof $\mu$Gal ($1~\mu$Gal~=~$10^{-8}$~m/s$^2$). We also show that this effect isnot compensated when averaging over the two directions of the Raman wavevector$k$. This thus constitutes a limit to the rejection efficiency of the$k$-reversal technique. Our analysis allows us to separate this effect from theeffect of the finite speed of light, which we find in perfect agreement withexpected values. This study highlights the benefit of chirping symmetricallythe two Raman lasers.
机译:我们在此分析拉曼激光移动的频率依赖性对拉曼型原子重力仪的相位的影响。对拉曼激光器施加频率chi以补偿重力并确保拉曼脉冲在共振期间的共振。干涉仪。我们表明,当此线性调频脉冲仅应用于两个拉曼激光器之一时,拉曼光移的变化足以使重力测量偏差$ \ mu $ Gal($ 1〜\ mu $ Gal〜=〜$ 10 ^ {- 8} $〜m / s $ ^ 2 $)。我们还表明,在拉曼波向量$ k $的两个方向上求平均时,这种效果无法得到补偿。因此,这构成了对$ k $反转技术的拒绝效率的限制。我们的分析使我们能够将这种影响与有限光速的影响区分开,我们发现光速与预期值完全吻合。这项研究突出了对称调频两个拉曼激光器的好处。

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