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Physical Review A

Electromagnetically induced transparency without a Doppler background in a multilevel ladder-type cesium atomic system

Baodong Yang, Jing Gao, Tiancai Zhang, Junmin Wang

Published Jan 21, 2011• 30 citations
Publisher

Abstract

We present an investigation of electromagnetically induced transparency (EIT) without Doppler background due to a locked probe laser. The EIT is theoretically studied based on a multilevel ladder-type cesium atomic system 6${S}_{1/2}$--6${P}_{3/2}$--8${S}_{1/2}$ in a room-temperature vapor cell. The experimental results agree with the theoretical calculations. Compared with the traditional EIT spectra with a Doppler profile limiting the spectral resolution for keeping the coupling laser locked and scanning the probe laser, these EIT spectra with the probe laser locked and the coupling laser scanned have a flat background, which seem be of great benefit for applications such as the measurement of hyperfine intervals between excited states, the study of highly excited Rydberg states, laser-frequency stabilization, etc.

DOI
10.1103/physreva.83.013818

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Laser Physics Letters•Aug 1, 2026•0 citations
We present an investigation of electromagnetically induced transparency (EIT) without Doppler background due to a locked probe laser. The EIT is theoretically studied based on a multilevel ladder-type cesium atomic system 6S1/2{S}_{1/2}S1/2​--6P3/2{P}_{3/2}P3/2​--8S1/2{S}_{1/2}S1/2​ in a room-temperature vapor cell. The experimental results agree with the theoretical calculations. Compared with the traditional EIT spectra with a Doppler profile limiting the spectral resolution for keeping the coupling laser locked and scanning the probe laser, these EIT spectra with the probe laser locked and the coupling laser scanned have a flat background, which seem be of great benefit for applications such as the measurement of hyperfine intervals between excited states, the study of highly excited Rydberg states, laser-frequency stabilization, etc.
Based on the cesium 6S1/2 -6P3/2 -8S1/2 ladder-type system, electromagnetically-induced transparency (EIT) is further investigated in a room-temperature vapor cell. When the probe laser is locked to one of the hyperfine transitions between the ground state 6S1/2 (F=3) and the intermediate state 6P3/2 while the coupling laser scans the transition between the intermediate state 6P3/2 and the excited state 8S1/2, the EIT spectrum has a flat background improving the spectral resolution. The theoretically calculated EIT spectral profiles from a multi-level ladder-type model are consistent well with the obtained experimental phenomena.
Electromagnetically induced transparency (EIT) was observed in a mismatched-wavelength cascade system using a room temperature vapor cell and laser-cooled atoms. A cw probe laser beam monitored the cesium ${6S}_{1/2}\ensuremath{\rightarrow}{6P}_{3/2}$ transition while another cw laser coupled the 6P3/2{6P}_{3/2}6P3/2​ state to a higher excited state. The ratio of the observed Rabi frequencies for coupling to the ${6P}_{3/2}\ensuremath{\rightarrow}(11--{13)D}_{3/2,5/2}$ transitions agreed closely with that predicted using the transition oscillator strengths. A comparison of the EIT signals obtained using cold atoms and the vapor cell is made.
A high sensitivity spectroscopy of Rydberg atoms is presented by using electromagnetically induced transparency (EIT) in the 6S(1/2)-6P(3/2)-n D ladder-type system of cesium vapor cell at room temperature. The EIT spectra of 40 D Rydberg state are measured and the dependences of the EIT magnitude and linewidth on the coupling laser power are investigated in detail. The Rydberg EIT linewidth is measured to be about 5.6 MHz when the powers of probe and coupling lasers are 50 microW and 5.2 mW, respectively, and which is close to the natural linewidth of cesium atoms. The effect of double resonance optical pumping on EIT is also investigated. The fine structures of nD (n = 39-55) are measured and the experimental result is in agreement with quantum defect theory.
Rydberg atoms, with large principal quantum number n, have been widely investigated in recent years due to their peculiar properties, such as big sizes, long lifetimes and strong interactions with fields and other Rydberg atoms. Rydberg atoms are very sensitive to external fields due to their large polarizabilities scaling as n7.These make Rydberg atoms an ideal candidate for the quantum information, the many-body interaction, etc.In this work, we investigate the Rydberg atoms using electromagneticlly induced transparency (EIT) in a ladder three-level system. The EIT is a quantum interference effect between two excitation path-ways driven by two laser fields. The main idea is performed in a room temperature cesium vapor cell, where the probe laser frequency is modulated. The ground state (6P1/2), excited state (6P3/2), and Rydberg state (nS1/2) constitute a Rydberg three-level system, in which the probe laser is fixed to the 6S1/2 (F = 4)6P3/2 (F = 5) transition by saturated absorption spectrum technique, whereas the coupling laser is scanned across the 6P3/249S1/2 transition. We detect the demodulated EIT signal with the lock-in amplifier (SR830). The modulated EIT signal shows a two-peak structure. The measured spacing between two peaks increases with the frequency detuning, caused by the modulation amplitude, and half the spacing between the peak-to-peak is nearly 1.67 times the modulation amplitude of the probe laser; the measured result shows that the splitting is independent of the modulation frequency. The experimental results are in agreement with the theoretical calculations. The results in our work can be used for real-time monitoring of the laser-line profiles and the fluctuation of laser frequency.
We present a laser frequency locking to Rydberg transition with electromagnetically induced transparency (EIT) spectra in a room-temperature cesium vapor cell. Cesium levels 6S 1/2 , 6P 3/2 , and the n D 5/2 state, compose a cascade three-level system, where a coupling laser drives Rydberg transition, and probe laser detects the EIT signal. The error signal, obtained by demodulating the EIT signal, is used to lock the coupling laser frequency to Rydberg transition. The laser frequency fluctuation, ∼0.7 MHz, is obtained after locking on, with the minimum Allan variance to be 8.9 × 10 −11 . This kind of locking method can be used to stabilize the laser frequency to the excited transition.
Abstract The double resonance phenomenon of electromagnetically induced transparency (EIT) in a ladder-type Rydberg atomic system is theoretically investigated. Based on the cesium 6 S 1 / 2 → 6 P 3 / 2 → n D 5 / 2 transition, we establish a density-matrix model incorporating the Doppler effect and simulate the absorption spectra under counter-propagating laser configurations. The numerical approach is adopted: a two-velocity-group approximation (Lorentzian line-shape superposition). The results show that when the probe detuning Δ p is fixed and nonzero, scanning the coupling laser frequency yields two symmetric transparency peaks separated by δ = 2 ( λ p / λ c ) | Δ p | , in excellent agreement with recent experimental observations. The two-velocity-group approximation is computationally efficient and physically transparent, while the high-precision integration confirms its validity. We also reveal that conventional uniform velocity averaging fails to resolve the narrow EIT peaks due to insufficient sampling, and propose effective numerical strategies. This work provides a reliable theoretical tool for simulating Rydberg EIT spectra and offers insights into Doppler-induced double resonance, which may find applications in laser frequency stabilization and self-calibration of Rydberg atom-based sensors.