Abstract:We report experimental observation of electromagnetically induced transparency (EIT) in an inhomogeneously broadened V-type Na 2 molecular system. The experiment is performed with both co-and counter-propagating arrangements for the propagation direction of the coupling and probe laser beams. In our theoretical model we employ the density matrix formalism, as well as perturbative methods for obtaining the probe field absorption profile for both open and closed systems. Simulations of the experimental data show… Show more
“…A dip appears near the resonance is caused by EIT which is not related to saturation. By comparison, saturation and EIT cause the dip respectively in free space [27]. So the contributions of saturation and EIT in V-type reflection spectra are different from those spectra in free space.…”
Section: We Use (16a)-(16f) (19a)-(19f) Andmentioning
confidence: 88%
“…[27], EIT and saturation occur simultaneously in a V-type system in free space, which is induced by pump field. In order to analyze EIT and saturation in reflection spectra at the interface, we study the reduced density matrix equations (16a)-(16f) and (19a)-(19f).…”
Section: Electromagnetically Induced Transparency and Saturation mentioning
confidence: 99%
“…EIT has been studied in Λ, Ξ and V-type systems in free space [25][26][27], and has also been studied in Λ and Ξ systems at the interface [28,29]. However, there is no report about EIT in V-type system at the interface as far as we know.…”
Section: Introductionmentioning
confidence: 99%
“…However, there is no report about EIT in V-type system at the interface as far as we know. V-type system has an essential difference compared to Λ or Ξ -type systems, which has been studied in reference [27]. For a three-level Λ system, atoms are mainly populated in two ground states.…”
We theoretically study electromagnetically induced transparency (EIT) in reflection spectra of V-type system at the gas-solid interface. In addition to a narrow dip arising from the EIT effect, we find the other particular saturation effect induced by pump field, which does not exist in Λ or Ξ -type system reflection spectra. The saturation effect only induces an intensity decrement in the reflection spectra, and there is no influence on the narrow dip arising from the EIT effect. We detailedly calculate and analyze the dependence of V-type system reflection spectra on probe field intensity, pump field intensity, coherent decay rate, and the initial population after the collision between atoms and the interface.
“…A dip appears near the resonance is caused by EIT which is not related to saturation. By comparison, saturation and EIT cause the dip respectively in free space [27]. So the contributions of saturation and EIT in V-type reflection spectra are different from those spectra in free space.…”
Section: We Use (16a)-(16f) (19a)-(19f) Andmentioning
confidence: 88%
“…[27], EIT and saturation occur simultaneously in a V-type system in free space, which is induced by pump field. In order to analyze EIT and saturation in reflection spectra at the interface, we study the reduced density matrix equations (16a)-(16f) and (19a)-(19f).…”
Section: Electromagnetically Induced Transparency and Saturation mentioning
confidence: 99%
“…EIT has been studied in Λ, Ξ and V-type systems in free space [25][26][27], and has also been studied in Λ and Ξ systems at the interface [28,29]. However, there is no report about EIT in V-type system at the interface as far as we know.…”
Section: Introductionmentioning
confidence: 99%
“…However, there is no report about EIT in V-type system at the interface as far as we know. V-type system has an essential difference compared to Λ or Ξ -type systems, which has been studied in reference [27]. For a three-level Λ system, atoms are mainly populated in two ground states.…”
We theoretically study electromagnetically induced transparency (EIT) in reflection spectra of V-type system at the gas-solid interface. In addition to a narrow dip arising from the EIT effect, we find the other particular saturation effect induced by pump field, which does not exist in Λ or Ξ -type system reflection spectra. The saturation effect only induces an intensity decrement in the reflection spectra, and there is no influence on the narrow dip arising from the EIT effect. We detailedly calculate and analyze the dependence of V-type system reflection spectra on probe field intensity, pump field intensity, coherent decay rate, and the initial population after the collision between atoms and the interface.
Despite the essential difference in underlying physics, electromagnetically induced transparency (EIT) and Autler–Townes splitting (ATS) are difficult to be discriminated because they cause resemble absorption and dispersion to a probe electromagnetic field. They are mainly discerned in the sense of absorption profile fitting. Here, the breakdown of the time‐reversal symmetry (TRS), namely optical nonreciprocity in the EIT and ATS configurations are experimentally observed by using warm rubidium atoms. The microscopic Doppler effect due to atomic thermal motion causes strong optical nonreciprocity to the probe field in the EIT configuration. In stark contrast, the propagation of the probe field is primarily reciprocal in the ATS configuration. The experimental observations in this study objectively distinguish the EIT and ATS effects in the fundamental physics of breaking the TRS. This experiment proves a concept of using the TRS as a testbed for discerning fundamental physical effects.
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