Abstract
An electromagnetically induced transparency (EIT) signal is observed in a V-type energy level scheme in a cesium vapor cell at room temperature. The effects of frequency detuning and the intensity of the pump laser on the EIT signal have been investigated. The performance of the probe-diode laser system, which is frequency stabilized on the EIT signal by using electrical feedback, is explored. The first derivative of the EIT signal offers a steeper slope and better S/N ratio for laser frequency stabilization than that of the Doppler-free hyperfine and crossover resonances. A comparative study of the frequency stability of an external-cavity diode laser stabilized at EIT and at the crossover resonance is presented. The square root of the Allan variance (σ) vs. integration time (τ) plot shows about a tenfold improvement in the frequency stability of the EIT-locked laser (σ ∼ 2.043 × 10-13τ-1/2) over that of the crossover-locked laser under a short integration time (1-10 ms), whereas a twofold improvement is found under a long integration time (∼1 s).
| Original language | English |
|---|---|
| Pages (from-to) | 1353-1360 |
| Number of pages | 8 |
| Journal | Laser Physics |
| Volume | 17 |
| Issue number | 12 |
| DOIs | |
| State | Published - Dec 2007 |
| Externally published | Yes |