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Nonlinear optical excitation response and regulation of instabilities in a Y-type atomic system under complex interactions

Shang-Yu Zhai, Rui Shi, Fu-Han Xie

Published Mar 1, 2025• 0 citations
Publisher

Abstract

In this work, a Y-type energy level ensemble of an alkali metal Rydberg rubidium cold atomic system under complex interactions is considered. To solve this nonlinear optical response, Newton’s iterative method is employed with random initial values for solving the multi-body density matrix equations and further observing the Rydberg excitation’s instability. The effects of self-interaction and direct and exchange interactions in the cross-interactions are comprehensively considered via three real cases: (I) only self-interaction; (II) self-interaction and direct interaction; and (III) self-interaction, direct interaction, and exchange interaction simultaneously. The results indicate that under the condition of I, since the system only has self-interaction, it exhibits only a typical bistable phenomenon. With the introduction of direct interaction, the Rydberg population in II shows a bifurcated bistable phenomenon. Finally, a more complex exchange interaction is further introduced. Under the condition of III, the system exhibits a complex multi-stable phenomenon in the same detuning direction. More importantly, such bistable and multi-stable phenomena can be well regulated by changing the cooperative nonlinearity modulated via the pump field. In addition, the bistable and multi-stable atomic excitation responses of the system on one transition branch can also be controlled by the coupling field Rabi frequency on another transition branch. This work applies numerical iterative algorithms to achieve a detailed analysis of the new phenomena with bistable and multi-stable excitation responses for nonlinear characteristics and provides theoretical support for the preparation of optical multistable materials.

DOI
10.1063/5.0225161

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arXiv:1303.4927•Physical Review A•Nov 26, 2013•44 citations
In this work, a Y-type energy level ensemble of an alkali metal Rydberg rubidium cold atomic system under complex interactions is considered. To solve this nonlinear optical response, Newton’s iterative method is employed with random initial values for solving the multi-body density matrix equations and further observing the Rydberg excitation’s instability. The effects of self-interaction and direct and exchange interactions in the cross-interactions are comprehensively considered via three real cases: (I) only self-interaction; (II) self-interaction and direct interaction; and (III) self-interaction, direct interaction, and exchange interaction simultaneously. The results indicate that under the condition of I, since the system only has self-interaction, it exhibits only a typical bistable phenomenon. With the introduction of direct interaction, the Rydberg population in II shows a bifurcated bistable phenomenon. Finally, a more complex exchange interaction is further introduced. Under the condition of III, the system exhibits a complex multi-stable phenomenon in the same detuning direction. More importantly, such bistable and multi-stable phenomena can be well regulated by changing the cooperative nonlinearity modulated via the pump field. In addition, the bistable and multi-stable atomic excitation responses of the system on one transition branch can also be controlled by the coupling field Rabi frequency on another transition branch. This work applies numerical iterative algorithms to achieve a detailed analysis of the new phenomena with bistable and multi-stable excitation responses for nonlinear characteristics and provides theoretical support for the preparation of optical multistable materials.
In this work, we have investigated a phase transition and optical bistability in a cold [Formula: see text]Rb sample excited to the [Formula: see text] Rydberg state, using absorption spectroscopy while scanning the Rydberg excitation laser for [Formula: see text]. The system is characterized through its dependence on the Rydberg Rabi frequency and principal quantum number, exhibiting hysteretic behavior indicative of bistability. We further analyze its time evolution, revealing the characteristic dynamics of the transition between stable states. The results are consistent with optical bistability induced by a cold plasma in the presence of Rydberg blockade. This work demonstrates the role of collective many-body interactions in establishing nonlinear optical responses in strongly interacting Rydberg ensembles.
High optical nonlinearities can be achieved at the single photon level by coupling the photon states to strongly interacting Rydberg excitations under the conditions of electromagnetically induced transparency. The nonlinear response in Rydberg quantum optics comes as a direct result of the long range dipole-dipole interactions via Rydberg blockade and interaction induced dephasing. In this thesis, Rydberg quantum optics experiments are performed with two spatially separated mediums with a nonlinear response at the single photon level. Two ultracold rubidium atomic clouds are tightly confined by a pair of in-vacuo aspheric lenses such that only a few Rydberg excitations can exist in each one of the clouds simultaneously. The long range character of the dipole-dipole interactions leads to the generation of quantum states of light. The effective photon-photon interactions are directly observed as an anti-correlation in the simultaneous photon retrieval as a result of the non resonant van der Waals interactions. The collective Rydberg excitations, stored in the non-overlapping mediums, experience an additional spatial non-uniform phase. In addition, we experimentally characterize the cooperative optical response of a cold atomic medium at a single photon level. This aims to exploit the enhancement of the spontaneous emissions decay rate (superradiance) as a dependence of the number of atoms involved in the ensemble. The observed atomic response in two different regimes gives a further understanding of the system dynamics and unlocks a promising potential route towards the implementation in scalable, multichannel quantum optical devices.
Collective behavior in many-body systems, where the dynamics of an individual element depend on the state of the entire ensemble, play an important role in both basic science research and applied technologies. Over the last twenty years, studies of such effects in cold atomic vapors have lead to breakthroughs in areas such as quantum information science and atomic and condensed matter physics. Nevertheless, in order to generate photon-mediated atom-atom coupling strengths that are large enough to produce collective behavior, these studies employ techniques that intrinsically limit their applicability. In this thesis, I describe a novel nonlinear optical process that enables me to overcome these limitations and realize a new regime of collective light-matter interaction. My experiment involves an anisotropic cloud of cold rubidium atoms illuminated by a pair of counterpropagating optical (pump) fields propagating at an angle to the trap's long axis. When the pump beam intensities exceed a threshold value, a collective instability occurs in which new beams of light are generated spontaneously and counterpropagate along the trap's long axis. In order to understand the physical mechanism responsible for this behavior, I study first the system's nonlinear optical response when driven below the instability threshold. I find that the incident optical fields produce an optical lattice that causes the atoms to become spatially organized on the sub-wavelength length scale. This organization corresponds to the formation of an atomic density grating, which effectively couples the involved fields to one another and enables the transfer of energy between them. The loading of atoms into this grating is enhanced by my choice of field polarizations, which simultaneously results in cooling of the atoms from T~30 μK to T~3 μK via the Sisyphus effect. As a result, I observe a fifth-order nonlinear susceptibility χ^{(5)}=1.9x10^-12 (m/V)^4 that is 7 orders of magnitude larger than previously observed. In addition, because of the unique scaling of the resulting nonlinear response with material parameters, the magnitude of the nonlinearity can be large for small pump intensities (\\ie, below the resonant electronic saturation intensity 1.6 mW/cm^2) while simultaneously suffering little linear absorption. I confirm my interpretation of the nonlinearity by developing a theoretical model that agrees quantitatively with my experimental observations with no free parameters. The collective instability therefore corresponds to the situation where the cold vapor transitions spontaneously from a spatially-homogeneous state to an ordered one. This emergent organization leads to the simultaneous emission of new optical fields in a process that one can interpret either in terms of mirrorless parametric self-oscillation or superradiance. By mapping out the phase diagram for this transition, I find that the instability can occur for pump intensities as low as 1 mW/cm^2, which is approximately 50 times smaller than previous observations of similar phenomena. The intensity of the emitted light can be up to 20% of the pump beam intensity and depends superlinearly on the number of atoms, which is a clear signature of collective behavior. In addition, the generated light demonstrates temporal correlations between the counterpropagating modes of up to 0.987 and is nearly coherent over several hundred μs. The most significant attributes of the light, though, are that it consists of multiple transverse spatial modes and persists in steady-state. This result represents the first observation of such dynamics, which have been shown theoretically to lead to a rich array of new phenomena and possible applications.
We study the optical response of cold rubidium atoms driven into the four-level Y configuration exhibiting two high Rydberg levels in the regime of electromagnetically induced transparency (EIT). Atoms excited to either Rydberg level interact with each other just via self-blockade potentials (I) or also via cross blockade potentials (II). Numerical results show a few interesting quantum phenomena on the transmitted properties of a weak probe field owing to controlled single and double Rydberg blockade. In case (I), it is viable to switch between single-photon outputs with vanishing (invariable) two-photon (three-photon) correlation and photon-pair outputs with vanishing (invariable) three-photon (two-photon) correlation. Such output switch can be easily done by modulating frequencies and intensities of two strong coupling fields to create a degenerate EIT window or two separated EIT windows. In case (II), we find that two-photon and three-photon correlations decrease together at a degenerate EIT window center while increasing together between two separated EIT windows. Such consistent changes are observed because both correlations are modified by the identical polarizability degradation though depending on single and double Rydberg blockade, respectively.
Abstract Electromagnetically induced transparency (EIT) and absorption (EIA) are quantum coherence phenomena which result from the interference of excitation pathways. Combining these with Rydberg atoms have opened up many possibilities for various applications. We introduce a theoretical model to study Rydberg-EIT and Rydberg-EIA effects in cold Cs and Rb atomic ensembles in a four-level ladder type scheme taking into account van der Waals type interactions between the atoms. The proposed many-body method for analysis of such systems involves a self-consistent mean field approach and it produces results which display a very good agreement with recent experiments. Our calculations also successfully demonstrate experimentally observed EIT-EIA cross-over in the Rb case. Being able to simulate the interaction effects in such systems has significant importance, especially for controlling the optical response of these.
We investigate dispersive optical nonlinearities that arise from a Rydberg excitation blockade in cold Rydberg gases. We consider a two-photon transition scheme and study the nonlinear response to a weak optical probe in the presence of a strong control beam. For very low probe fields, the dominant nonlinearities are of the third order and they can be evaluated in a steady-state regime. In a more general case, the change in average atomic populations and coherences due to Rydberg interactions can be characterized by properly defined scaling parameters, which are generally complex numbers but in certain situations take the usual meaning of the number of atoms in a blockade sphere. They can be used in a simple ``universal scaling'' formula to determine the dispersive optical nonlinearity of the medium. We also develop a technique to account for the Rydberg interaction effects, by simplifying the treatment of nonlocal interaction terms, the so-called collisional integrals. We find algebraic relations that only involve two-body correlations, which can be solved numerically. All average populations and coherences are then obtained straightforwardly.