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Conference on Lasers and Electro-Optics Europe & European Quantum Electronics Conference (CLEO/Europe-EQEC)

Frequency doubled tunable diode laser for excitation of Rydberg states in Rb atoms

Vasily M. Entin, I. I. Ryabtsev, Ilya I. Beterov, Denis B. Tretyakov

Published Jun 1, 2007• 0 citations
Publisher

Abstract

In the present paper we used single mode laser diode working near 960 nm to excite Rb atoms into Rydberg states. Using external cavity described above we have obtained stable continuous operation of the frequency doubling of semiconductor laser with linewidth below 10 MHz and output power of several mW.
DOI
10.1109/cleoe-iqec.2007.4385909

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We transfer the frequency stability from a diode laser, which was locked to Doppler-free saturation absorption resonance in lithium vapor cell, to a tunable Ti-sapphire laser. We get the laser linewidth < 100 kHz/100 ms and absolute frequency stability ±0.5 MHz. The uv laser system which included the stabilized Ti-sapphire laser and frequency doubler has output optical beam with power near 100 mW and wavelength 350 nm. This uv laser system will be used for excitation and study of Rydberg states in lithium atoms.
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We have performed high resolution spectroscopy of rubidium with a single mode continuous wave distributed feedback (DFB) laser diode. The saturation spectrum of the D 2 -line of 85 Rb and 87 Rb was recorded with a resolution close to the natural line width. The emission frequency was actively stabilized to Doppler-free transitions with a relative accuracy of better than 7 parts in 10 9 using commercially available servo devices only. An output power of 80 mW was sufficient to allow for two-photon spectroscopy of the 5S-5D-transition of 87 Rb. Further, we report on the spectral properties of the DFB diode, its tuning range and its frequency modulation properties. The line width of the diode laser, determined with high resolution Doppler free two photon spectroscopy, was 4 MHz without applying any active stabilization techniques. For time scales below 5 μs the line width drops below 2 MHz.
A system of three external cavity diode lasers is used to excite Rydberg states in rubidium. The 5S→5P→5D transitions are driven using lasers with λ = 780 and 776 nm respectively. From the 5D state, atoms fluoresce down to the 6P state. The final transition to Rydberg levels is from the 6P state with laser light near λ = 1016 nm. The nS and nD Rydberg states are accessible directly and with the application of a modest electric field nP states can also be excited. As a test of this system, Stark spectra are collected for nD and nP states.
A compact, high-power, and stable blue laser source is essential for Rydberg state excitation of rubidium (Rb) atoms, particularly for emerging Rydberg atom-based sensors that require portability for practical applications. In this work, we present an injection-locked laser system using blue laser diodes for both the leader and follower lasers near 480 nm, enabling efficient Rydberg state preparation of Rb and eliminating the need for nonlinear frequency-doubling. The locked follower laser delivers 263 mW of output power with a linewidth of 591(31) kHz after frequency stabilization. High-efficiency spatial mode matching between the seed light and follower laser is accomplished through a polarization-maintaining fiber, resulting in a power gain of 30.4 dB. The compact optical path design allows the laser system to occupy just 20 × 21 × 4 cm 3 . Such a high-power and compact injection-locked blue laser system provides a low-cost and efficient solution for Rydberg atom-based applications.
Frequency stabilization of a diode laser at 480 nm is crucial for coherently exciting rubidium atoms to Rydberg states.A laser frequency stabilization technique is reported based on electromagnetically induced transparency in a ladder configuration with a polarization spectrum stabilized 780 nm diode laser as the probe laser and a 480 nm laser as the coupling laser.With a uniform magnetic field,a two-photon dichroic atomic vapor laser lock(DAVLL) spectroscopy was generated.Then this spectroscopy was fed back through two proportion-integral-differential circuits to lock the 480 nm diode laser.A combined linewidth of about 1 MHz is achieved during the locking period.