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dc.identifier.uri http://dx.doi.org/10.15488/15167
dc.identifier.uri https://www.repo.uni-hannover.de/handle/123456789/15286
dc.contributor.author Meyer-Hoppe, Bernd eng
dc.date.accessioned 2023-11-09T12:36:40Z
dc.date.available 2023-11-09T12:36:40Z
dc.date.issued 2023
dc.identifier.citation Meyer-Hoppe, Bernd: Quantum Dynamics in a Ferromagnetic Atomic Gas. Hannover : Gottfried Wilhelm Leibniz Universität, Diss., 2023, ix, 122 S., DOI: https://doi.org/10.15488/15167 eng
dc.description.abstract Bose-Einstein condensates (BECs) provide an extraordinary system to study many-body quantum effects with a high degree of control. Using such ultra-cold gases, microscopic quantum effects become visible on a macroscopic scale as thermal fluctuations are negligible. In particular, quantum phase transitions can be observed. These phase transitions can be indicated by an order parameter that abruptly changes at the critical value of a certain control parameter. Throughout this work, a spin-1 BEC with ferromagnetic interactions and zero magnetization is considered. This system exhibits three ground-state quantum phases that can be controlled by an effective magnetic field. These phases have been explored both theoretically and experimentally in the last two decades. Quantum phase transitions are by definition only applicable to the ground state of a system. However, this powerful concept can be extended to states with non-zero energy. Such excited-state quantum phase transitions (ESQPTs) can be driven by a conventional control parameter, but, interestingly, also by a variation of the excitation energy only. ESQPTs have been studied theoretically and their existence itself has been revealed, e.g., in molecular spectra. However, a thorough investigation by an order parameter and in particular the experimental mapping of the corresponding phase diagram remain an open challenge in any physical system. In this thesis, an interferometric order parameter is employed to experimentally map out an excited-state quantum phase diagram. This order parameter is based on dynamical behavior of coherent states that resemble the mean-field phase-space trajectories of excited-state phases. While a ferromagnetic spin-1 BEC with zero magnetization serves as an exemplary platform, the findings can be applied to other quantum systems with similar Hamiltonians. Importantly, the distinction of excited-state quantum phases utilizes the excitation energy as a second control parameter, which presents a key feature of ESQPTs. Our experiments therefore extend the powerful concept of quantum phases and quantum phase transitions to the entire Hilbert space of the spin-1 BEC. eng
dc.language.iso eng eng
dc.publisher Hannover : Institutionelles Repositorium der Leibniz Universität Hannover
dc.rights CC BY 3.0 DE eng
dc.rights.uri http://creativecommons.org/licenses/by/3.0/de/ eng
dc.subject spinor Bose-Einstein condensate eng
dc.subject spin-changing collisions eng
dc.subject ferromagnetic interaction eng
dc.subject phase diagrams eng
dc.subject quantum phase transitions eng
dc.subject excited-state quantum phase transitions eng
dc.subject Spinor-Bose-Einstein-Kondensat ger
dc.subject spinändernde Stöße ger
dc.subject ferromagnetische Wechselwirkung ger
dc.subject Phasendiagramme ger
dc.subject Quantenphasenübergänge ger
dc.subject Quantenphasenübergänge angeregter Zustände ger
dc.subject.ddc 530 | Physik eng
dc.title Quantum Dynamics in a Ferromagnetic Atomic Gas eng
dc.type DoctoralThesis eng
dc.type Text eng
dc.description.version publishedVersion eng
tib.accessRights frei zug�nglich eng


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