2021
DOI: 10.1126/sciadv.abe9164
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Coupling light to a nuclear spin gas with a two-photon linewidth of five millihertz

Abstract: Nuclear spins of noble gases feature extremely long coherence times but are inaccessible to optical photons. Here, we realize a coherent interface between light and noble-gas spins that is mediated by alkali atoms. We demonstrate the optical excitation of the noble-gas spins and observe the coherent back action on the light in the form of high-contrast two-photon spectra. We report on a record two-photon linewidth of 5 ± 0.7 mHz above room temperature, corresponding to a 1-min coherence time. This experiment p… Show more

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Cited by 21 publications
(10 citation statements)
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“…Using a linearly polarized optical probe beam, we measure the collective spin of the rubidium along the truex̂ axis via its imprint on the polarization of the probe beam, which rotates after traversing the alkali medium. The polarization rotation is subsequently measured with a set of differential photodiodes in a homodyne configuration ( 44 – 46 ). While the polarized rubidium spins are initially oriented along the trueẑ axis, they are tilted by an angleθRbfalse(f=fDMfalse)=γRbbXeθXefalse∣iΓRb+fRbfDMfalse∣Here, b Xe θ Xe is the transverse spin-exchange field.…”
Section: Resultsmentioning
confidence: 99%
“…Using a linearly polarized optical probe beam, we measure the collective spin of the rubidium along the truex̂ axis via its imprint on the polarization of the probe beam, which rotates after traversing the alkali medium. The polarization rotation is subsequently measured with a set of differential photodiodes in a homodyne configuration ( 44 – 46 ). While the polarized rubidium spins are initially oriented along the trueẑ axis, they are tilted by an angleθRbfalse(f=fDMfalse)=γRbbXeθXefalse∣iΓRb+fRbfDMfalse∣Here, b Xe θ Xe is the transverse spin-exchange field.…”
Section: Resultsmentioning
confidence: 99%
“…Owing to the great separation between the EPR and NMR resonances considered in this search (ω DM , ω K ≫ ω He ) the dynamics of the two spin gases is weaklycoupled [57,[64][65][66]. Consequently, the total collective spin of the potassium The width of this band denotes the strongest and weakest values around each mass point.…”
Section: B Response To Alp Fieldmentioning
confidence: 99%
“…The width and calibration factor remained very stable (< 10% drift) during a single measurement. The EPR resonance however was decreased during the measurement because of temporal change in P He (t); While the helium spins were polarized at B = 70 mG at the onset of each measurement, at lower magnetic fields the decoherence of the helium spins rate was moderately increased, primarily due to spatial inhomogeneity in the alkali-metal spins polarization [57]. The temporal variation in the spin-exchange field which shifted the EPR frequency was included in the analysis.…”
Section: Calibrationsmentioning
confidence: 99%
“…Furthermore, record storage time of ∼ 1 s has been observed with storage of bright pulses [43] by operating at the so-called 'spin exchange relaxation-free' regime. The storage time in these systems has the potential to be pushed beyond hours by transferring the spin excitation from alkali atoms to noble-gas nuclear spins via spin exchange collisions [44].…”
Section: A Warm Vapour Memoriesmentioning
confidence: 99%