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Journal of Physics B Atomic Molecular and Optical Physics

Phase control of fluorescence quenching and line narrowing

Qing Yang Xu, Xiangming Hu, Jian-wu Yin

Published Jan 24, 2008• 3 citations
Publisher

Abstract

The resonance fluorescence from a three-level Λ atom is studied, in which each optical transition is driven by a coherent field and the metastable states are coupled to each other via a microwave field. It is shown that the fluorescence depends not only on the relative intensities of the coupling fields but also on the relative phase delay between the envelopes of the amplitudes of the three fields. For the case of equal intensity of the two coherent fields, the fluorescence is completely inhibited once the phase delay is set to be 0 or π, while the fluorescence emerges once the phase delay is changed to π/2; moreover, the fluorescence spectrum ultimately reverts to an ultranarrow triplet by decreasing the relative intensity of the coherent field to the microwave field.

DOI
10.1088/0953-4075/41/3/035503

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Physical Review A•Sep 1, 1996•48 citations
The resonance fluorescence from a three-level Λ atom is studied, in which each optical transition is driven by a coherent field and the metastable states are coupled to each other via a microwave field. It is shown that the fluorescence depends not only on the relative intensities of the coupling fields but also on the relative phase delay between the envelopes of the amplitudes of the three fields. For the case of equal intensity of the two coherent fields, the fluorescence is completely inhibited once the phase delay is set to be 0 or π, while the fluorescence emerges once the phase delay is changed to π/2; moreover, the fluorescence spectrum ultimately reverts to an ultranarrow triplet by decreasing the relative intensity of the coherent field to the microwave field.
It is shown that simultaneous narrowing occurs upon the central peak and outer sidebands in the resonance fluorescence spectrum by simulating vacuum-induced quantum interference in a Λ-type three-level atomic system, where the transition dipole moments are orthogonal, the metastable states are coupled to each other via a microwave field and a laser field is applied to one dipole-allowed atomic transition. With the decrease in the ratio of the laser Rabi frequency to the microwave Rabi frequency, the fluorescence spectrum eventually reverts to an ultrasharp triplet. The physical interpretation of the spectral characteristics is given in terms of dressed states.
We present a scheme for sub-half-wavelength localization based on phase-dependent coherent effects on resonance fluorescence. A three-level atom in the Λ configuration is considered. Two metastable states are so separated from each other that the fluorescence spectra from the different transitions do not overlap. Two dipole-allowed transitions and one dipole-forbidden transition are driven by a standing-wave laser field, a travelling-wave laser field and a microwave field, respectively. The spectrum of fluorescence from the standing-wave coupled transition is dependent not only on the position but also on the collective phase of all applied fields. When the phase is varied and fluorescence photons are detected, 50% probability is achieved in a half-wavelength region. This scheme is as efficient as previous ones based on coherence-controlled Autler–Townes spectra.
We investigate theoretically the features of the spontaneous emission spectrum of a four-level atomic system driven by a coherent probe field,a coupling laser field and a microwave field.The two upper levels are coupled by a microwave field with lower frequency.The time evolution of the populations is calculated.It is shown that the spectra behavior,such as spectral-line narrowing,spectral-line enhancement,spectral-line suppression,and total cancellation of fluorescence quenching,can be easily controlled by changing the phase and the amplitude of the microwave field.
The resonance fluorescence from a four-level atom driven by two coherent fields is studied. If the dipole moments between the two upper levels and each of the two lower levels are parallel, the spontaneous emission paths from the upper levels to the lower levels will have strongly or even completely destructive quantum interference. We show that this quantum interference will result in a complete inhibition of the fluorescence when one of the driving fields is tuned at the middle point of the upper levels. The quantum interference will lead to the dependence of atomic populations at steady state on the initial condition, when both of the driving fields are tuned to the middle point of the upper levels. When the dipole moments are close to but not exactly parallel, or none of the driving fields is tuned at the middle point of the upper levels and there is a small difference between detunings of the two driving fields to the uppermost level, ultranarrow lines at the spectral center appear because of the destructive quantum interference.
Abstract The resonance fluorescence of a four-level atom in J = 1/2 to J = 1/2 transition driven by two coherent fields is studied. We find that the incoherent fluorescence spectrum shows a direct indication of vacuum-induced coherence in the atomic system. We show that such coherence manifests itself via an enhancement or suppression of the spectral peaks in the π -polarized fluorescence. The effect of the relative phase of the driving fields on the spectral features is also investigated. We show that phase-dependent enhancement or suppression of the fluorescence peaks appears in the incoherent spectrum emitted along the σ transitions. It is found that this phase dependence occurs because of the polarization-detection scheme employed for the observation of the fluorescence light. We present an analytical explanation, based on dressed-states of the atom-field system, to interpret the numerical results.
The fluorescence field from one of the two allowed transitions in a three-level atom can sense squeezed fluctuations of a vacuum field coupled to the other transition. We examine the fluorescence spectra of strongly driven three-level atoms in \ensuremath{\Lambda}, V, and cascade configurations in which one of the two one-photon transitions is coupled to a finite-bandwidth squeezed vacuum field, when the bandwidth is much smaller than the difference in the atomic transition frequencies, though much larger than atomic decay rates and Rabi frequencies of the driving fields. The driving fields are on one-photon resonance, and the squeezed vacuum field is generated by a degenerate parameter oscillator. Details are only given for the \ensuremath{\Lambda} configuration. The extension to the V and cascade configurations is straightforward. We find that in all configurations the fluorescence spectra of the transition not coupled to the squeezed vacuum field are composed of five lines, one central and two pairs of sidebands, with intensities and widths strongly influenced by the squeezed vacuum field. However, only the central component and the outer sidebands exhibit a dependence on the squeezing phase. We also examine the fluorescence spectrum for the cascade configuration with a squeezed vacuum field on resonance with the two-photon transition between the ground and the most excited states and now generated by a nondegenerate parametric oscillator. In this case, where the squeezed vacuum field can be made coupled to both transitions, all spectral lines depend on the squeezing phase. The spectral features are explained in terms of the dressed-atom model of the system. We show that the coherent mixing of the atomic states by the strong driving fields modifies transition rates between the dressed states, which results in the selective phase dependence of the spectral features. \textcopyright{} 1996 The American Physical Society.