2017
DOI: 10.1088/1742-6596/810/1/012002
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Towards passive and active laser stabilization using cavity-enhanced atomic interaction

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Cited by 5 publications
(4 citation statements)
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“…Here, For linearly polarized light, the above expression can be conveniently represented in terms of rank 0 and 2 tensors as [26,28,32]…”
Section: Methods Of Evaluationmentioning
confidence: 99%
See 1 more Smart Citation
“…Here, For linearly polarized light, the above expression can be conveniently represented in terms of rank 0 and 2 tensors as [26,28,32]…”
Section: Methods Of Evaluationmentioning
confidence: 99%
“…The laser induced light shifts can be avoided by trapping the atoms in optical lattice at the magic wavelength (λ magic ) [22][23][24]. This is a well known technique used in passive atomic clocks [25][26][27][28] where the magic wavelength trapping is constructed for a ground state and an excited state. Theoretical determination of magic wavelengths in these atoms involves calculation of frequency-dependent polarizabilities of the considered states to find the magic wavelengths, where dynamic polarizability of both states participating in the transition is equal, in other words, the differential Stark shift for the states involved in the transition is zero [24].…”
Section: Introductionmentioning
confidence: 99%
“…Through laser cooling technique, the Doppler effect can be largely suppressed. The Niels Bohr Institute at the University of Copenhagen has chosen 88 Sr atoms as a quantum reference for laser frequency stabilization based on cavityenhanced atomic interaction, using both passive and active methods [73]. In the passive scheme [74,75], a cavityenhanced modulation transfer spectrum is employed and the corresponding atomic phase shift is used as an error signal.…”
Section: Atomic Beam Two-level Aocmentioning
confidence: 99%
“…By exploiting the high Q factor of the atomic transitions and using cavities with comparatively low Q factors the systems are far less sensitive to thermal fluctuations of the cavity components, and the experimental requirements are simplified. In these approaches active as well as passive atomic systems have been suggested [13][14][15][16][17][18]. The active atomic systems are optical equivalents of the maser, relying on cooperative quantum phenomena such as superradiance or superfluorescence of atoms inside the cavity mode.…”
Section: Introductionmentioning
confidence: 99%