Over the past decades, alkali atoms have been the subject of intensive and diverse research, ranging from fundamental studies on ultra-cold atoms and Bose-Einstein condensates to technological applications. Since they possess only a single valance s-electron, the alkali atoms manifest a simple low-lying electronic structure compared to other atoms. Moreover, unlike conventional solid state systems their dispersion-free features make them an ideal candidate for sensing applications and referencing tasks. These two features have introduced alkali atoms as promising quantum emitters for the new paradigm of hybrid quantum optics and quantum electrodynamics. This new concept benefits from the existing integrated photonics technology for squeezing and confining the light in sub-wavelength scales to substantially enhance the light-atom interaction. The hybrid chip is envisioned to have light sources, waveguides, devices, and detectors to realize a complex quantum network down to a single photon level. In this talk I will discuss about our recent theoretical and experimental works on atomic vapor spectroscopy in the vicinity of the plasmonic and nanophotonic devices. I start from a density matrix-based formalism describing the evolution of Rb vapor atomic levels, excited with an incoherent pump and coupled to a plasmonic lattice. When designed properly, the lattice plasmon mode efficiently captures the spontaneously emitted photons from the excited Rb atoms and a coherent coupling between the lattice mode and the atomic levels would occur. I will elaborate on the effect of pumping rate and decoherence on the steady state of the hybrid system and the feasibility of achieving a lasing state. In the second part of the talk I will present the results of our experiments on Rb vapor coupled to such a plasmonic lattice. Starting from the pumping mechanism, I describe the collisional scheme we employed to transfer the excited Rb atoms from (_^5)P_(3/2) to(_^5)P_(1/2) , hence achieving a population inversion between P and S levels and an optical gain at 795 nm, eventually. I present the experimental results of this atomic vapor interaction with a plasmonic lattice resonating at 795 nm. The spectroscopy of Rb cloud modified with tightly squeezed and enhanced field of the lattice plasmons shows the clear signature of Fano resonances in the passive gas, followed by amplified spontaneous emission in the active gas and the lasing at higher pumping powers. The results of this study would pave the way toward hybrid atom-quantum photonic chips.
Over the past decades, alkali atoms have been the subject of intensive and diverse research, ranging from fundamental studies on ultra-cold atoms and Bose-Einstein condensates to technological applications. Since they possess only a single valance s-electron, the alkali atoms manifest a simple low-lying electronic structure compared to other atoms. Moreover, unlike conventional solid state systems their dispersion-free features make them an ideal candidate for sensing applications and referencing tasks. These two features have introduced alkali atoms as promising quantum emitters for the new paradigm of hybrid quantum optics and quantum electrodynamics. This new concept benefits from the existing integrated photonics technology for squeezing and confining the light in sub-wavelength scales to substantially enhance the light-atom interaction. The hybrid chip is envisioned to have light sources, waveguides, devices, and detectors to realize a complex quantum network down to a single photon level. In this talk I will discuss about our recent theoretical and experimental works on atomic vapor spectroscopy in the vicinity of the plasmonic and nanophotonic devices. I start from a density matrix-based formalism describing the evolution of Rb vapor atomic levels, excited with an incoherent pump and coupled to a plasmonic lattice. When designed properly, the lattice plasmon mode efficiently captures the spontaneously emitted photons from the excited Rb atoms and a coherent coupling between the lattice mode and the atomic levels would occur. I will elaborate on the effect of pumping rate and decoherence on the steady state of the hybrid system and the feasibility of achieving a lasing state. In the second part of the talk I will present the results of our experiments on Rb vapor coupled to such a plasmonic lattice. Starting from the pumping mechanism, I describe the collisional scheme we employed to transfer the excited Rb atoms from (^5)P(3/2) to(^5)P(1/2) , hence achieving a population inversion between P and S levels and an optical gain at 795 nm, eventually. I present the experimental results of this atomic vapor interaction with a plasmonic lattice resonating at 795 nm. The spectroscopy of Rb cloud modified with tightly squeezed and enhanced field of the lattice plasmons shows the clear signature of Fano resonances in the passive gas, followed by amplified spontaneous emission in the active gas and the lasing at higher pumping powers. The results of this study would pave the way toward hybrid atom-quantum photonic chips.
Abstract The incorporation of neutral atoms in nanophotonic structures offers significant potential to realize novel quantum optical devices. Here, the possibility of creating low‐threshold integrated lasers in hybrid systems based on coupling room‐temperature atomic gases with both dielectric and metallic nanophotonic systems is investigated. Two different classes of devices resulting from incorporating an optically pumped Rb–ethane mixture in a dielectric ring resonator and a plasmonic lattice are studied. It is shown that the combination of the optical gain provided by the atomic vapor, along with the unique field‐confinement properties of nanophotonic structures, enables the generation of coherent radiation, that is, laser light, at moderate power levels. In addition, general design guidelines for these hybrid nanophotonic lasers are provided. These results pave the way toward a novel class of active nanophotonic and metamaterial systems.
The entry into the new millennium was marked in the quantum community by the first experimental realizations of the Bose-Einstein condensation of atoms in a vapor, achieved in different research groups. Twenty-five years later, such systems are 'routinely' produced and are the core of many experiments. At the frontier between condensed matter their y, quantum optics, and atomic physics, ultra-cold atoms are subjects of high scientific interest.Ultra-cold gas can be trapped in optical lattices, giving a realistic way of experimentally realizing a new range of lattice Hamiltonians, that are used to simulate condensed matter systems. In these simulations, ultra-cold atoms are used to mimic the behavior of electrons in a solid-state material and could be used to simulate a wide range of complex condensed matter phenomena, such as the fractional quantum Hall effect, topological insulators, and high-temperature superconductivity.In order to study such systems, diffraction-limited quantum gas microscopes have emerged as a way to manipulate and detect atoms trapped in lattice potentials. Using far-field interference, experiments have mainly been restricted to a lattice spacing of 500 nm. This limits the speed of dynamics of all physical processes.Higher energy regimes could be accessed by reducing the lattice spacing. For this purpose, one of the long-term goals of the team is to trap atoms in the near-field of a surface and to make use of the Casimir-Polder forces to shape sub-wavelength potentials. Thanks to nano-fabrication capabilities, the spacing can be reduced to a few tens of nanometers. However, this requires to adapt the imaging techniques to observe cold-atoms with sub-wavelength spatial resolutions.In this PhD thesis, I report first on the advances toward implementing an atom chip in our experiment, which will serve as an integrated platform to manipulate the quantum gas. I present simulations and study an experimental solution allowing the cloud to be transported to the near-field. The method is based on the interference of a laser radiation in the near field of a rotating surface. It has been fully simulated, and the limitations have been numerically and experimentally assessed. I conclude this part by presenting the first model of chip that has been fabricated.In a second part, I report on the development of a sub-wavelength imaging method of cold Rubidium 87 atoms which is based on excited state dressing. I detail the concept of this nano-metric spatial resolution method and apply it to super-resolve a single longitudinal wave function trapped in a tight lattice that exhibits a width below 30 nm.
In this work, we experimentally observe for the first time nanoscale plasmonic enhanced Electromagnetically Induced Transparency (EIT) and Velocity Selective Optical Pumping (VSOP) effects in miniaturized Integrated Quantum Plasmonic Device (IQPD) for D 2 transitions in rubidium (Rb). Our device consists of a vapor cell integrated on top of a prism coated with a thin layer of metal. This configuration is known to allow efficient excitation of Surface Plasmon Resonance (SPR). The evanescent field of the surface plasmon mode interacts with the atomic media in close vicinity to the metal. In spite of the limited interaction length between SPR and Rb atoms, the signature of EIT along with VSOP signals could be clearly observed in our miniaturized IQPD under proper conditions of pump and probe intensities. A gradual decrease in the contrast of the plasmonic enhanced EIT and VSOP signals was observed as the excitation was detuned from the SPR critical angle, due to reduction in electromagnetic field enhancement, leading to a reduced interaction of the evanescent field with the atomic vapor media. Following the demonstration of these effects, we also present a detailed model revealing the mechanisms and the origin of plasmonic enhanced EIT and VSOP effects in our system. The model, which is based on the Bloch equations, is in good agreement with the observed experimental results. The obtained results are regarded as an important step in the quest for the realization of nanoscale quantum plasmonic effects and devices.
Atoms with narrow-line resonances play a major role in high precision measurements like magnetometry and atomic clocks. Due to their long inherent coherence time, atoms can serve as quantum memories as well. Moreover, as they possess well-defined electronic levels, coherent interactions with the photon fields can be used to manipulate their quantum states very precisely. Besides, the capability of the optical excitation and read out, increase the spatial resolution of the atomic sensors. Within the last couple of decades interfacing atoms with engineered confined light fields has been a proper playground for investigating various quantum-electrodynamical effects. So far different strategies have been utilized successfully to integrate atoms with a confined light field, for example in high-finesse optical cavities, hollow core fibers, and tapered nanofibers. While cold atom setups provide ideal conditions and controllability to explore different coupling regimes, the large setups required to cool and trap the atoms have hindered their scalability for any realistic quantum networks. Thermal vapors, on the other hand, allow for less precision and control, but their low technical complexity and suitable compatibility with miniaturization and integration make them a promising candidate for realizing scalable networks.
Techniques to controllably interface atoms with quantum optical fields form the basis for many applications in quantum information science. For example, photons are convenient to relay information over large quantum networks, while atoms naturally are physical systems that can process and store this information. Thus far, the available techniques to efficiently couple single photons with atomic media fall into one of the following, mostly independent, categories: i) cavity quantum electrodynamics (QED), where atomic interactions with light are enhanced via a high-finesse cavity, ii) coherent coupling with atomic ensembles exhibiting large optical depths, and iii) the use of fields tightly focused to dimensions smaller than or approaching the scattering cross-section of a single atom. Although remarkable achievements have been made with all of these approaches, a robust, scalable technique remains elusive. Recently, several groups have successfully demonstrated that cold atoms can be trapped near and interfaced with nanophotonic systems, such as hollow-core photonic crystal fibers [1] and tapered nanofibers [2–4]. The traps are well-characterized [2, 3, 5], and the nearly diffraction-limited transverse confinement of optical fields enables ∼ 10% coupling efficiency of a single atom to the fiber [2, 3]. This has already led to remarkable observations of strong light-matter interactions using relatively few atoms and low powers [1]. It has also been proposed that such techniques can be extended to highly configurable photonic crystal waveguides [6]. Together, these efforts raise the intriguing possibility for future nanophotonic systems with tremendous figures of merit, wherein atom-light interactions can be tailored nearly at will. Here, we discuss recent efforts to develop novel techniques to realize strong, controllable atom-photon and photon-photon interactions, which take full advantage of the parameter space afforded by nanophotonic interfaces and are not based upon the extension of existing techniques. As a specific example, we discuss a protocol to achieve “all-atomic” cavity QED [7], as briefly described below. First, we show that although the single-atom coupling to guided modes of a nanophotonic waveguide might be relatively weak, there exist collective modes of a trapped atomic ensemble whose coupling to light is enhanced by the square root of the atom number, √ NA. While collective effects are generally well-known, special consequences emerge in the nanofiber system when the atoms are trapped in a lattice. In particular, collective effects cause such a lattice to act as a near-perfect mirror for an incident field close to resonance. In analogy to cavity QED, we then demonstrate that two sets of atomic mirrors can form an effective cavity, which can greatly enhance the coupling of a single, specially chosen “impurity” atom (or a few impurity atoms) positioned inside. We introduce a novel quantum spin model to describe the atom-light coupling, which allows one to exactly map the atom-nanofiber interface onto the simple and elegant Jaynes-Cummings model of cavity QED [8]. A unique feature of our atomic mirrors compared to conventional cavities is that they have long relaxation times and are highly dispersive. Remarkably, even with very low mirror finesse (F ∼ 10 2 ), this property allows one to attain the “strong coupling” regime of cavity QED, where vacuum Rabi oscillations [9–12] occur between an excited impurity atom and a single “photon” stored in the cavity (or more precisely, in the atomic mirrors). Furthermore, as quantum mechanical objects, these atom mirrors can be used to store quantum information and transfer this information into propagating waveguide modes. These various features can be combined to realize all of the building blocks for scalable quantum information processing.
Attempting to implement quantum information related applications utilizing atoms and photons, as they naturally form quantum systems supporting superposition states, hybrid quantum plasmonic systems emerged in the past as a platform to study and engineer light-matter interaction. This platform combines the unrivaled electromagnetic field localization of surface plasmon polaritons, boosting the light-matter coupling rate, with the tremendous integration potential of truly nanoscale structures, and both the significant emission rates of nanoantennas and photonic transmission velocities. In this work, a classical description of surface plasmon polaritons is combined with a light-matter interaction model based on a cavity quantum electrodynamical formalism. The resulting composite semi-classical method, introduced and described in this thesis, provides efficient and versatile means to simulate the dynamical behavior of radiative atomic transitions coupled to plasmonic cavity modes in the weak incoherent coupling regime. Both the emission into the far field and various dissipation mechanisms are included by expanding the model to an open quantum system. The variety of light-matter interaction applications that can be modeled with the outlined method is indicated by the four different exemplary scenarios detailed in the application chapter of this thesis. The classical description of localized surface plasmon polaritons is benchmarked by reproducing the experimental measurements of the molecular fluorescence manipulation through optical nanoantennas in a collaborative effort with experimental partners. Furthermore, in the weak light-matter coupling regime, the potential of achieving a higher nanoantenna functionality and simultaneously realizing more elaborate quantum dynamics is revealed by the three remaining applications. Each pivotally involving a bimodal nanoantenna and demonstrating different quantum optical phenomena, the implementation of cavity radiation mode conversion, non-classical cavity emission statistics, and non-classical cavity emission properties is shown and described in the application chapter.