Absorption resonance and large negative delay in rubidium vapor with a buffer gas

EE Mikhailov, VA Sautenkov, YV Rostovtsev, GR Welch - JOSA B, 2004 - opg.optica.org
EE Mikhailov, VA Sautenkov, YV Rostovtsev, GR Welch
JOSA B, 2004opg.optica.org
We observe a narrow, isolated, two-photon absorption resonance in^ 87Rb for large one-
photon detuning in the presence of a buffer gas. In the absence of a buffer gas, a standard Λ
configuration of two laser frequencies gives rise to electromagnetically induced
transparency (EIT) for all values of one-photon detuning throughout the inhomogeneously
(Doppler) broadened line. However, when a buffer gas is added and the one-photon
detuning is comparable to or greater than the Doppler width, an absorption resonance …
We observe a narrow, isolated, two-photon absorption resonance in ^87Rb for large one-photon detuning in the presence of a buffer gas. In the absence of a buffer gas, a standard Λ configuration of two laser frequencies gives rise to electromagnetically induced transparency (EIT) for all values of one-photon detuning throughout the inhomogeneously (Doppler) broadened line. However, when a buffer gas is added and the one-photon detuning is comparable to or greater than the Doppler width, an absorption resonance appears instead of the usual EIT resonance. We also observe a large negative group delay (≈−300 μs for a Gaussian pulse that propagates through the media with respect to a reference pulse not affected by the media), corresponding to a superluminal group velocity v_g=−c/(3.6×10^6)=−84 m/s.
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