The transition probabilities for induced emission and absorption of electromagnetic radiation by an excited atom interacting, in addition to the radiation field, with a system of "perturbers" (in single, binary, and completed encounters) are evaluated. It is found that Dirac's result $\frac{{W}_{\mathrm{ind}}}{{W}_{\mathrm{abs}}}=\frac{({\overline{n}}_{l\ensuremath{\sigma}}+1)}{{\overline{n}}_{l\ensuremath{\sigma}}}$ must be modified by a factor $\frac{{(1\ensuremath{-}\ensuremath{\alpha}n)}^{2}}{{(1+\ensuremath{\alpha}n)}^{2}}$, where $\ensuremath{\alpha}$ is related to the interaction potential of the emitter-perturber system as well as to the level structure of the "colliding" atoms, and $n$ is the perturber number density.The transition probabilities for induced emission and absorption of electromagnetic radiation by an excited atom interacting, in addition to the radiation field, with a system of "perturbers" (in single, binary, and completed encounters) are evaluated. It is found that Dirac's result $\frac{{W}_{\mathrm{ind}}}{{W}_{\mathrm{abs}}}=\frac{({\overline{n}}_{l\ensuremath{\sigma}}+1)}{{\overline{n}}_{l\ensuremath{\sigma}}}$ must be modified by a factor $\frac{{(1\ensuremath{-}\ensuremath{\alpha}n)}^{2}}{{(1+\ensuremath{\alpha}n)}^{2}}$, where $\ensuremath{\alpha}$ is related to the interaction potential of the emitter-perturber system as well as to the level structure of the "colliding" atoms, and $n$ is the perturber number density.

Physical Review LettersNov 16, 19700 citations

Observation of oscillatory Raman gain associated with two-photon Rabi oscillations of nanofiber-coupled atoms

Christian Liedl, Sebastian Pucher, Philipp Schneeweiß +2 more

Abstract Quantum emitters with a Λ-type level structure enable numerous protocols and applications in quantum science and technology. Understanding and controlling their dynamics is, therefore, one of the central research topics in quantum optics. Here, we drive two-photon Rabi oscillations between the two ground states of cesium atoms and observe the associated oscillatory Raman gain and absorption that stems from the atom-mediated coherent photon exchange between the two drive fields. The atoms are efficiently and homogeneously coupled with the probe field by means of a nanofiber-based optical interface. We study the dependence of the two-photon Rabi frequency on the system parameters and observe Autler–Townes splitting in the probe transmission spectrum. Beyond shedding light on the fundamental processes underlying two-photon Rabi oscillations, our method could also be used to investigate (quantum) correlations between the two drive fields as well as the dynamical establishment of electromagnetically induced transparency.Abstract Quantum emitters with a Λ-type level structure enable numerous protocols and applications in quantum science and technology. Understanding and controlling their dynamics is, therefore, one of the central research topics in quantum optics. Here, we drive two-photon Rabi oscillations between the two ground states of cesium atoms and observe the associated oscillatory Raman gain and absorption that stems from the atom-mediated coherent photon exchange between the two drive fields. The atoms are efficiently and homogeneously coupled with the probe field by means of a nanofiber-based optical interface. We study the dependence of the two-photon Rabi frequency on the system parameters and observe Autler–Townes splitting in the probe transmission spectrum. Beyond shedding light on the fundamental processes underlying two-photon Rabi oscillations, our method could also be used to investigate (quantum) correlations between the two drive fields as well as the dynamical establishment of electromagnetically induced transparency.

arXiv:2207.00437Journal of Physics B Atomic Molecular and Optical PhysicsOct 21, 20223 citations

Nonlinear optical processes in a system of colliding atoms

A. M. Bonch-Bruevich, Sergey G. Przhibel'skii, V. V. Khromov

Bulletin of the Russian Academy of Sciences PhysicsFeb 1, 19790 citations

STRUCTURE OF A HOLE-EXCITATION SPECTRUM OF ATOMS

Vasily V. Balashov, I P Sazhina, N M Kabachnik

Jan 1, 19720 citations

Electromagnetically induced absorption with sub-kHz spectral width in a paraffin-coated Rb vapor cell

Ho-Jung Kim, Han Seb Moon

We report on electromagnetically induced absorption (EIA) with sub-kHz spectral width in a paraffin-coated Rb vapor cell in the Hanle configuration of the 5S(1/2)(F=2)-5P(3/2)(F'=3) transition of 87Rb atoms. Using a linearly polarized laser, the spectral width of the Hanle EIA spectrum was measured to be 0.55 mG (390 Hz). The narrow spectral width was due to the maintaining of atomic coherence between ground states while atoms collided with the anti-relaxation coated wall of the Rb vapor cell. Under a weak transverse residual magnetic field, the angle between the transverse residual magnetic field and the direction of linear polarization affected the magnitude of the narrow Hanle EIA spectrum. This is because of the change of atomic magnetic momentum due to the weak transverse residual magnetic field around the zero value of the longitudinal magnetic field.We report on electromagnetically induced absorption (EIA) with sub-kHz spectral width in a paraffin-coated Rb vapor cell in the Hanle configuration of the 5S(1/2)(F=2)-5P(3/2)(F'=3) transition of 87Rb atoms. Using a linearly polarized laser, the spectral width of the Hanle EIA spectrum was measured to be 0.55 mG (390 Hz). The narrow spectral width was due to the maintaining of atomic coherence between ground states while atoms collided with the anti-relaxation coated wall of the Rb vapor cell. Under a weak transverse residual magnetic field, the angle between the transverse residual magnetic field and the direction of linear polarization affected the magnitude of the narrow Hanle EIA spectrum. This is because of the change of atomic magnetic momentum due to the weak transverse residual magnetic field around the zero value of the longitudinal magnetic field.

Optics ExpressDec 22, 201027 citations

n

is the perturber number density.