We design and implement a low-impedance, high-current radio-frequency (RF) circuit, enabling fast coherent coupling between magnetic levels in cold alkali atomic samples. It is based on a compact, shape-optimized coil that maximizes the RF field coupling with the atomic magnetic dipole, and on coaxial transmission-line transformers that step up the field-generating current flowing in the coil by a factor ∼ 4 to about 7.5 A for 100 W of RF driving. This allows us to obtain a RF coupling field of about 0.035 G / W at the atomic sample location. The system is robust and versatile, as it generates a large RF field without compromising the available optical access, and its central resonant frequency can be adjusted in situ. Our approach provides a cost-effective, reliable solution, featuring a negligible level of interference with surrounding electronic equipment thanks to its symmetric layout. We test the circuit performance using a maximum RF power of 80 W at a frequency around 82 MHz, which corresponds to a measured Rabi frequency ΩR/2π ≃ 18.5 kHz, that is, a π-pulse duration of about 27 μs, between two of the lowest states of 6Li at an offset magnetic field of 770 G. Our solution can be readily adapted to other atomic species and vacuum chamber designs, in view of an increasing modularity of cold atom experiments.
A low-impedance radio-frequency circuit for fast spin manipulations in cold alkali atoms / Scazza, F.; Del Pace, G.; Pieri, L.; Concas, R.; Kwon, W. J.; Roati, G.. - In: REVIEW OF SCIENTIFIC INSTRUMENTS. - ISSN 0034-6748. - ELETTRONICO. - 96:(2025), pp. 104713.0-104713.0. [10.1063/5.0276530]
A low-impedance radio-frequency circuit for fast spin manipulations in cold alkali atoms
Scazza, F.;Del Pace, G.;Pieri, L.;Concas, R.;Kwon, W. J.;Roati, G.
2025
Abstract
We design and implement a low-impedance, high-current radio-frequency (RF) circuit, enabling fast coherent coupling between magnetic levels in cold alkali atomic samples. It is based on a compact, shape-optimized coil that maximizes the RF field coupling with the atomic magnetic dipole, and on coaxial transmission-line transformers that step up the field-generating current flowing in the coil by a factor ∼ 4 to about 7.5 A for 100 W of RF driving. This allows us to obtain a RF coupling field of about 0.035 G / W at the atomic sample location. The system is robust and versatile, as it generates a large RF field without compromising the available optical access, and its central resonant frequency can be adjusted in situ. Our approach provides a cost-effective, reliable solution, featuring a negligible level of interference with surrounding electronic equipment thanks to its symmetric layout. We test the circuit performance using a maximum RF power of 80 W at a frequency around 82 MHz, which corresponds to a measured Rabi frequency ΩR/2π ≃ 18.5 kHz, that is, a π-pulse duration of about 27 μs, between two of the lowest states of 6Li at an offset magnetic field of 770 G. Our solution can be readily adapted to other atomic species and vacuum chamber designs, in view of an increasing modularity of cold atom experiments.| File | Dimensione | Formato | |
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