Abstract:
Synthetic quantum systems are simplified versions of real-world, complex, quantum
many-body systems. They provide a versatile testbed for understanding the complex
phenomenons of condensed matter physics, nuclear physics, high energy physics,
and chemistry. In the context of quantum many-body physics, these systems have
mainly been used to study various spin models and Hubbard-type models. The
major advantage of synthetic quantum systems is the possibility to have control
over system parameters such as dimension, scale, the strength of interaction, and
range of the interaction. The tremendous experimental progress in the area of laser
cooling and trapping has boosted the development of various synthetic quantum
systems based on different architectures. The platforms based on ultracold atoms,
ions, superconducting circuits, photons have emerged in the past two decades and
have succeeded in revealing exotic quantum phenomena. Among all the platforms,
Rydberg atom-based quantum systems stand out because of strong controllable
interaction, single-site addressability, scalability, and large coherence times. These
systems have been used to study both the ground state physics as well as non-equilibrium dynamics of various spin models.
This work is focused on utilizing the properties of Rydberg atoms along with
other tools to achieve control over the interactions, population dynamics, correlations, and entanglement in the system. In three independent setups, we show how
the specific properties of the system along with the properties of Rydberg atoms
can be used to achieve the same. Towards that goal, in Chapter 1, we give a brief
overview of the developments in the field of ultra-cold atoms. We then discuss the
basic properties of Rydberg atoms such as Rydberg blockade, Rydberg dressed interaction, Bose-Hubbard model, photonic crystal waveguides. These properties will
be used in subsequent chapters.
In chapter 2, we calculate the Hubbard parameters for Rydberg-dressed interaction using maximally localized Wannier functions. We show that by varying the external laser parameters we can vary the shape of Rydberg-dressed potential
such that the extended Bose-Hubbard model can be realized. We also identify the
dominant density-assisted tunneling processes for Rydberg-dressed interaction.
In chapter 3, we study a chain of Rydberg atoms in which the detuning is periodically varied in time. We identify the correlated Rabi oscillations emerging due
to Rydberg interaction and study the effect of periodic driving onto the correlation
functions characterizing the correlated Rabi oscillations.
Chapter 4 studies the single excitation dynamics of an atomic excitation coupled
to a photonic crystal waveguide. The coupling of atoms to photonic modes of the
photonic crystal waveguide gives rise to an effective exchange Hamiltonian with a
controllable exchange interaction range. We study the excitation dynamics as a
function of exchange interaction range and characterize the change in the dynamics
using various parameters.
In the final chapter, we introduce one more excitation to the system and study
the effect of that excitation on the dynamics. Firstly, for the non-interacting excitations, we show the anti-bunching dynamics and quasi-localization. Secondly, for the
Rydberg excitations, we take into account the van der Waals interaction and study
its effect on the excitation dynamics. By varying the strength of vdW interaction
we go from anti-bunching dynamics to bound state dynamics. We also investigate
the effect of initial separation on the population dynamics and entanglement.