TY - BOOK

T1 - Dynamics of ion Coulomb crystals

AU - Timm, Lars

PY - 2023

Y1 - 2023

N2 - The field of quantum simulations has achieved a remarkable success through the development of highly controllable and accessible quantum platforms, which pro- vide insights into the microscopic properties of complex large-scale systems that are otherwise difficult to analyze. Many of the platforms utilized in this pursuit are derived from the field of atomic, molecular, and optical physics. One particularly popular candidate is provided by trapped ions, whose vibrational and electronic degrees of freedom can be effectively combined through laser pulses to engineer desired model Hamiltonians or quantum circuits. Trapped ions constitute as well the basis for modern atomic clocks, the most precise frequency standards currently available. They find further applications in metrology, geodesy, and fundamental physics experiments. In this Thesis, we investigate the dynamics of vibrational modes in trapped ion crystals, utilizing them as a versatile platform to explore various many-body phenomena. We first focus on the expansion dynamics of local excitations and on heat transport within ion crystals hosting structural defects that undergo a sliding- to-pinned transition. We observe a significant reduction in conductivity when the crystal symmetry is spontaneously broken during the transition, and show that resonances between crystal eigenmodes lead to distinct softening signatures associated with energy localization. We then delve into the effects of thermal and quantum fluctuations on the vibrational modes of ion crystals near two distinct structural transitions. We observe the emergence of a prolonged symmetric phase stabilized by thermal and quantum fluctuations, and develop effective theories that reduce the degrees of freedom to the modes that drive the transitions. Finally, we discuss how to engineer spin-orbit coupling and on-site interaction energies for vibrational quantum excitations using two different external driving schemes. While the simulation of spin models with ions typically involves the use of two electronic states, we propose interpreting the two local oscillation modes in an ion crystal as a pseudospin. We show how using Floquet engineering ideas allows for spin flips in Coulomb-induced vibron hopping, resulting in a non-trivial coupling between spatial motion and spin evolution, that results in a markedly non-Abelian dynamics. Subsequently, we explore the simulation of Hubbard models in trapped ions by coupling the vibrational Fock states to an internal level system. Our findings include the observation of bound states in the strong interaction limit of the resulting Jaynes-Cummings-Hubbard model. By investigating these topics, we aim to contribute to the understanding of vibrational dynamics in trapped ion crystals, and shed light on their potential for simulating condensed matter systems, offering insights into phenomena that are otherwise challenging to explore.

AB - The field of quantum simulations has achieved a remarkable success through the development of highly controllable and accessible quantum platforms, which pro- vide insights into the microscopic properties of complex large-scale systems that are otherwise difficult to analyze. Many of the platforms utilized in this pursuit are derived from the field of atomic, molecular, and optical physics. One particularly popular candidate is provided by trapped ions, whose vibrational and electronic degrees of freedom can be effectively combined through laser pulses to engineer desired model Hamiltonians or quantum circuits. Trapped ions constitute as well the basis for modern atomic clocks, the most precise frequency standards currently available. They find further applications in metrology, geodesy, and fundamental physics experiments. In this Thesis, we investigate the dynamics of vibrational modes in trapped ion crystals, utilizing them as a versatile platform to explore various many-body phenomena. We first focus on the expansion dynamics of local excitations and on heat transport within ion crystals hosting structural defects that undergo a sliding- to-pinned transition. We observe a significant reduction in conductivity when the crystal symmetry is spontaneously broken during the transition, and show that resonances between crystal eigenmodes lead to distinct softening signatures associated with energy localization. We then delve into the effects of thermal and quantum fluctuations on the vibrational modes of ion crystals near two distinct structural transitions. We observe the emergence of a prolonged symmetric phase stabilized by thermal and quantum fluctuations, and develop effective theories that reduce the degrees of freedom to the modes that drive the transitions. Finally, we discuss how to engineer spin-orbit coupling and on-site interaction energies for vibrational quantum excitations using two different external driving schemes. While the simulation of spin models with ions typically involves the use of two electronic states, we propose interpreting the two local oscillation modes in an ion crystal as a pseudospin. We show how using Floquet engineering ideas allows for spin flips in Coulomb-induced vibron hopping, resulting in a non-trivial coupling between spatial motion and spin evolution, that results in a markedly non-Abelian dynamics. Subsequently, we explore the simulation of Hubbard models in trapped ions by coupling the vibrational Fock states to an internal level system. Our findings include the observation of bound states in the strong interaction limit of the resulting Jaynes-Cummings-Hubbard model. By investigating these topics, we aim to contribute to the understanding of vibrational dynamics in trapped ion crystals, and shed light on their potential for simulating condensed matter systems, offering insights into phenomena that are otherwise challenging to explore.

U2 - 10.15488/16052

DO - 10.15488/16052

M3 - Doctoral thesis

CY - Hannover

ER -