Study of lin\|lin CPT for application in vapour cell atomic clocks

Study of lin||lin CPT for application in vapour cell atomic clocks

1 Abstract

We evaluate the use of Coherent Population Trapping (CPT) excited with parallely polarized laser fields in vapour cell atomic clocks. We study the resonance shape, the discriminator slope and signal-to-noise ratio as a function of relevant parameters such as the laser frequency detuning and the applied magnetic field. We show that a stability of may be reached in a compact system using a modulated VCSEL.

2 Introduction

Contrarily to the microwave-optical double resonance scheme, Coherent Population Trapping (CPT) does not require a microwave cavity, which may be an advantage in compact or miniature atomic clocks [1, 2]. CPT usually suffers from smaller signal contrast, even though different techniques have been recently proposed to overcome this potential limitation [3 - 6].

In this communication we present our study on the use of CPT in vapour cell frequency standards. We have investigated the case of Rb D when a longitudinal magnetic field is applied and the CPT is excited by a linearly polarized, unidirectional and multi-frequency light field the so called linlin CPT [7 - 10]. Here below the experimental setup is shortly described. In section two we present the signal shape for different values of magnetic field and we discuss the maximum contrast achievable in our configuration. In section three, the role of the laser frequency detuning, the noise measurements and determination of the optimal lock-in detection frequency are discussed. Finally, we predict the achievable clock frequency stability, basing our considerations on the presented signal-to-noise measurements.

Figure 1 shows our setup. The Rb atoms are confined in a cylindrical glass cell (volume 1 cm) placed in a cylindrical magnetic shield (volume 40 cm). A longitudinal magnetic field (B) is provided by a solenoid placed inside the magnetic shield, B is parallel to the laser beam propagation vector. The experiments were performed by using two cells containing either or kPa of nitrogen as buffer gas; higher buffer gas pressure in the cell are not suitable because of the suppression of quadrupole transitions due to the excited state mixing induced by the buffer gas. Remark that this intrinsic characteristic prohibits the application of the linlin CPT in miniature-clocks unless wall-coating is used, because in the mini-cells (volume mm) a buffer gas pressure of several tens of kPa is necessary.

Figure 1: The experimental setup used for linlin CPT.

The multi-frequency optical spectrum is generated via modulation of the injection current of a single mode VCSEL chip emitting around 795 nm [11]. The VCSEL used in this experiment has a linewidth of (10020) MHz, measured from a heterodyne beatnote. During the experiments the VCSEL was modulated at the frequency of 3.417 GHz (i.e. half of ground state hyperfine separation in Rb) with a power of 10 dBm. We estimated the spectral properties of the modulated VCSEL by recording the Rb one-photon absorption for different modulation frequencies and amplitudes. We did not observe effects related to amplitude modulation. The phase modulation index was about 1.8, corresponding to about 70 of the total laser power in the 1st order side-bands, which are used for CPT preparation. The remaining power is distributed in the carrier, 2nd and 3rd order side-bands, and essentially does not contribute to the CPT signal but increases the dc ”background” level on the photo-detector, induces AC Stark shift and contributes to one-photon absorption processes .

3 Degenerate and non-degenerate CPT

Figure 2 shows the relevant atomic levels and possible transitions for the Rb D line induced by the and components of the linearly polarized light fields. We focus our attention on the group of transitions from the ground state F towards the excited state F = 1 because the maximum contrast is expected in this configuration [7]. For the application in frequency standards we take into account the resonances less sensitive to the magnetic field, i.e. the CPT signal occurring between ground state Zeeman sublevels with m and m. Remark that, in the case of linear polarization, the and groups of transitions starting from the ground state Zeeman sublevels with m, give rise to two orthogonal CPT states which interfere destructively and do not contribute to the CPT signal. As a consequence, we have to consider only the two CPT states created by the coherent superposition of F, m and F, m, represented by the dashed and solid line in figure 2(b), respectively. These two CPT states are symmetrically split by the magnetic field with a factor of 28 Hz T determined by the nuclear g-factor, and are both shifted by a factor of 0.043 Hz T.

Figure 2: Interaction scheme for linlin hyperfine CPT. (a) represents all and allowed transitions; while (b) represents the transitions contributing to the resonance approaching the B resonance frequency.

In principle, the sensitivity to the magnetic field makes these CPT states not suitable for atomic clocks. However, their supposed high contrast drove several studies of their metrological properties [7 - 10]. The first observation of the CPT resonance splitting due to the nuclear g-factor, is reported for Cs atoms in reference [8]. In [9], we have presented a detailed theoretical analysis of the linlin CPT lineshape and proposed to use as frequency discriminator the maximum of absorption between the two CPT peaks when degeneracy is removed (so-called pseudo-resonance). Zibrov and co-workers [10] accounted for measuring the main metrological characteristic of the degenerate linlin CPT and pseudo-resonance. In their experimental setup, the multi-frequency spectrum was obtained by modulating the current of a diode laser which was injection locked by the radiation of a single mode ECDL. Therefore, our study constitutes the first experimental evaluation of the achievable clock frequency stability with linlin CPT in a single laser compact set-up.

Figure 3 shows typical degenerate CPT and pseudo-resonance signals obtained in our experiments: in figure 3(a), the relative magnetic shift () between the two CPT states is smaller than their linewidth (). In this case the two CPT states are degenerate and their signals merge. In figure 3(b), the B applied is such as , as a consequence the CPT degeneracy is removed and the pseudo-resonance signal appears.

Figure 3: Degenerate CPT (B T) and pseudo-resonance (B T) signals and their correspondent discriminator signals obtained by phase-sensitive detection.

Note that determines the B to apply for obtaining the maximum pseudo-resonance amplitude, which corresponds to the amplitude of the non-degenerate CPT (A= A). Considering that, in our experimental conditions, the CPT signal is well approximated by a Lorentzian function, A= A means . Since the amplitude of the non-degenerate CPT is smaller than the amplitude of the degenerate CPT, the optimal discriminator slope for pseudo-resonance will be approximately 3 times worse than the degenerate CPT discriminator slope.

In Figure 3 the CPT signal contrast, defined as the ratio between the CPT amplitude and DC level on the photodetector, is less than . By optimizing the experimental parameters (buffer gas pressure, cell temperature, laser diameter) in our setup, a maximum contrast of has been recorded. These values are noticeably smaller than the contrast obtained with the optical microwave double resonance. The main limiting factor to reach a higher CPT contrast is connected with the choice of creating the multi-frequency spectrum by a direct modulation of the VCSEL injection current. Whith this technique, when the amplitude of the -order sidebands is maximized, the of the total laser power is distributed in the carrier and higher order sidebands. Considering that the distance between two consecutive frequencies in the optical spectrum is about GHz and the typical Doppler linewidth is about GHz; in CPT resonance conditions, most of the power of the carrier and higher order sidebands pass trough the cell without being absorbed by Rb atoms, increasing significantly the background photodetector signal. Let us consider, for instance, the case of figure 3: the total laser power was about W of which W contributed mainly to the photodetector background signal. Whith the photodetector sensitivity of about A W, the background signal due to the carrier and the higher order sidebands is roughly A. In principle, a degenerate linlin CPT contrast up to may be reached using a pure bichromatic field.

4 Detection signal and noise: expected short term stability

A comparison of linlin CPT for the laser locked to either F=1 or F=2 group of transitions has been presented in [7], where the authors showed that the group of transitions towards F=1 results in larger A and narrower . In order to determine the optimal laser detuning for frequency standard applications, we studied D(A) versus the laser detuning () around the group of transitions towards F=1 (figure 4).

Figure 4: Experimental (dot) and theoretical (line) D versus laser detuning () for two cells filled with different buffer gas pressure, and kPa, respectively. =0 refers to the absorption F F in an evacuated Rb cell.The shift of the D maximum depends on both the pressure shift (dotted line) and broadening of the D line.

We observe that the laser detuning corresponding to the maximum of D depends on the buffer gas pressure in the cell. By comparing experimental and theoretical results, we pointed out that both the pressure shift and broadening of the Rb D influence the linlin CPT signal. In the case of a cell containing a N pressure of kPa, for instance, the maximum value of D corresponds to a detuning of about MHz, while the pressure shift is only MHz (lower plot in figure 4). We interpret this difference as a results of the destructive quantum interference between CPT states occurring when both levels F and F are excited simultaneously. If the laser is tuned resonant to F=1, the influence of the transition towards F=2 is due to the pressure broadening of the hyperfine transitions and/or the laser linewidth. Further experiments are in progress to quantify the dependence of the quantum interference on the experimental parameters.

The short term stability of an atomic clock depends on the parameters of the reference signal (A, ), the resonance frequency () and the detection noise (). It can be evaluated by the Allan deviation, [12].

The noise power spectrum has been measured for different the laser detuning () in our setup, using the cell filled with Rb and 1.5 mbar of N (figure 5). We observed that the detection noise level depends on the laser frequency detuning: when the laser is resonant with the Rb absorption the detection noise level increases significantly, indicating that the dominant contribution to the detection noise is the laser FM-to-AM conversion [13].

Figure 5: Detection noise (N) measured for the dark photo-detector, for the laser field tuned out, tuned to the maximum and to the slope of the Rb D line.

At higher frequency the detection noise is noticeably reduced: a factor 20 when changing from kHz to kHz for the laser tuned to the absorption peak. As a consequence it could be convenient for CPT-based atomic clocks to work with a lock-in modulation frequency () up to several tens of kHz. In this case the is larger than the linewidth of the monitored signal [14, 15], which can not be implemented in the micro-wave optical double resonance clock scheme as presently used. On the contrary, in reference [14], the authors showed that it is possible realize a CPT clock using . In our experimental conditions we verified that up to 40 kHz can be used for phase-sensitive detection when is about kHz. We record a reduction of the discriminator signal amplitude by a factor when we changed from kHz to kHz. Therefore the signal-to-noise ratio results times larger at kHz than kHz.

In table 1 we show the expected optimal short term stability for the cell containing 1.5 mbar of N. The notable difference between the theoretical and experimental short term stability is mainly due to the fact that the theoretical estimation assumed that the shot noise limit may be reached. Moreover, there is a difference between the measured and calculated CPT amplitude because the model is based on a pure bichromatic electromagnetic field, i.e. in the calculation the losses due to the 1-photon absorption of the VCSEL frequencies other than the first-order sidebands are neglected. The experimental results presented are limited by the laser power: with our VCSEL and the optimal beam diameter (0.8 cm) the maximum laser intensity (I) was 0.1 mW cm. Following the model, the optimal should be I mW cm, corresponding to a shot noise limited short term stability .

Parameters Experiments Theory
Signal Amplitude, A (nA) 100 400
Signal linewidth, (kHz) 0.7 0.7
Detection Noise, N (nA Hz) 0.03 0.005 (Shot Noise)
Short-term stability, 6 10 3 10
Table 1: Expected short-term stability () in optimized conditions.

5 Conclusion

We report on our study on the linlin CPT for applications in compact and high performance atomic clocks. We discuss the two relevant cases: degenerate CPT and pseudo-resonance. We showed that a 10 at second may be reached using the degenerate linlin CPT signal and a compact setup. This value is comparable to the short-term-stability of commercial compact atomic clocks. On the contrary the short-term stability of a pseudo-resonance clock may be about 10 at s. According to the model, the expected short-term stability is limited by the choice of the laser source and could be improved by using a pure bichromatic fields with higher laser power (up to mW cm).

6 Acknowledgement

The authors are pleased to acknowledge the financial support of the INTAS-CNES (project 06-1000024-9321), the Swiss National Science Foundation (project 200020-105624) and the Dimitry Zimin foundation ”Dynasty”. Finally we thank for the useful discussion C. Affolderbach, P. Thomann and our collegues of the Laboratoire Temps-Fréquence-IMT

References

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