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arXiv physics/0503096physics.atom-ph
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原子速度传感器的噪声灵敏度

Noise sensitivity of an atomic velocity sensor

Pierre Cladé, Saïda Guellati-Khélifa, Catherine Schwob, François Nez, Lucile Julien, François Biraben

摘要:

我们利用布洛赫振荡来相干加速铷原子。由该加速度引起的速度的变化是由于吸收一个光子而引起的反冲速度的整数倍。利用两个速度选择拉曼π脉冲实现了速度变化的测量:第一个脉冲将原子从超精细态5S_(1/2)转移|F=2,mF=0至5S 1/2,|F=1,mF = 0>,并将其转化为窄速度类。在这个选定的原子切片加速之后,我们施加第二拉曼脉冲以使共振原子回到初始状态5S 1/2,|F=2,mF = 0>。通过使用一维飞行时间技术分别测量(F=1和F=2)中的群体。为了绘制最终的速度分布,我们通过扫描第二脉冲的拉曼光束频率来重复该过程。然后,这两个π脉冲系统构成速度传感器。拉曼光束的相对相移中的任何噪声都会引起测量速度的误差。在本文中,我们提出了一个理论和实验分析,这种速度传感器,考虑到在拉曼脉冲的相位波动。

英文摘要:

We use Bloch oscillations to accelerate coherently Rubidium atoms. The variation of the velocity induced by this acceleration is an integer number times the recoil velocity due to the absorption of one photon. The measurement of the velocity variation is achieved using two velocity selective Raman pi-pulses: the first pulse transfers atoms from the hyperfine state 5S1/2 |F=2, mF=0> to 5S1/2, |F=1, mF = 0> into a narrow velocity class. After the acceleration of this selected atomic slice, we apply the second Raman pulse to bring the resonant atoms back to the initial state 5S1/2, |F=2, mF = 0>. The populations in (F=1 and F=2) are measured separately by using a one-dimensional time-of-flight technique. To plot the final velocity distribution we repeat this procedure by scanning the Raman beam frequency of the second pulse. This two pi-pulses system constitutes then a velocity sensor. Any noise in the relative phase shift of the Raman beams induces an error in the measured velocity. In this paper we present a theoretical and an experimental analysis of this velocity sensor, which take into account the phase fluctuations during the Raman pulses.

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