2021
DOI: 10.1088/1612-202x/ac0bc3
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On the polarization rotation by means of electromagnetically induced transparency

Abstract: The limitations on the effect of electromagnetically induced transparency (EIT) imposed by the degeneracy of atomic levels are considered. The dependence of the EIT-induced polarization rotation of the weak probe field on the characteristics of the resonant transitions and that of the control field is studied. The conditions for the 90 • -rotation without absorption are discussed.

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Cited by 1 publication
(1 citation statement)
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“…The photon polarization provides the most natural way for qubit encoding. The qubit encoded in the photon polarization may be stored in the Zeeman sublevels of the ground atomic state by means of reduction of the group velocity of the probe pulse [26][27][28][29], while for the implementation of single-qubit gates the controlled polarization rotation of the probe pulse may be applied [30,31]. For the implementation of two-qubit gates with polarization-encoded photon qubits the double-Λ EIT may be appropriate, which may enable the controlled mutual polarization rotation of the two weak probe fields induced by their cross-phase modulations.…”
Section: Introductionmentioning
confidence: 99%
“…The photon polarization provides the most natural way for qubit encoding. The qubit encoded in the photon polarization may be stored in the Zeeman sublevels of the ground atomic state by means of reduction of the group velocity of the probe pulse [26][27][28][29], while for the implementation of single-qubit gates the controlled polarization rotation of the probe pulse may be applied [30,31]. For the implementation of two-qubit gates with polarization-encoded photon qubits the double-Λ EIT may be appropriate, which may enable the controlled mutual polarization rotation of the two weak probe fields induced by their cross-phase modulations.…”
Section: Introductionmentioning
confidence: 99%