Stephan Haas
Current Organizations / Institutes
The organizations/institutes from the scholar's latest article
Previous Organizations / Institutes
The organizations / institutes from the scholar's other articles in the past ten years
Research Subjects
Stephan Haas has a total of 63 co-authors. Here are the top co-authors by number of shared publications:
- Stefan Kettemann
Max Planck Institute for the Physics of Complex Systems
6 shared publications - George Courcoubetis
Convergent Science Institute in Cancer, Michelson Center for Convergent Bioscience, University of Southern California, Los Angeles, CA 90089, USA
3 shared publications - Hyun-Yong Lee
Korea University
3 shared publications - Javad Vahedi
Department of Physics and Earth Sciences, Jacobs University Bremen, Bremen 28759, Germany
3 shared publications - N. Moure
Department of Physics and Astronomy University of Southern California, Los Angeles, California 90089-0484, USA
3 shared publications - Youcef Mohdeb
Department of Physics and Earth Sciences, Jacobs University Bremen, Bremen 28759, Germany
3 shared publications
Latest Publications
- 21 August 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (10) , 105132
Geometric decoherence time in Lindbladian dynamics
The onset of decoherence in open many-body systems lacks a dynamical timescale grounded in the loss of bipartite entanglement. Here, we introduce the geometric decoherence time, defined as the earliest moment the monotone relation between logarithmic negativity and R\'enyi-$\frac{1}{2}$ entropy---exactly equal across any bipartition for pure states---breaks down under open-system evolution, signaling entropy growth without accompanying entanglement growth. We establish this criterion in both single-particle Gaussian dynamics and many-body Lindbladian evolution. We show that quantum mutual information provides a complementary long-time diagnostic: Its asymptotic vanishing is equivalent to factorization of the steady state across the bipartition, a condition strictly stronger than separability, and whenever a product steady state is approached exponentially in trace norm, negativity and mutual information share the same decay rate. In the presence of a strong symmetry, this tracking can fail---residual classical correlations can survive after entanglement has vanished. In the Kitaev chain with balanced gain and loss, we derive a closed-form solution and show that the topological phase sustains longer coherence times than the trivial phase at identical dissipation, with a local minimum at the chiral-symmetric point. In the interacting XXZ chain, exact many-body evolution shows that local $Z$ dephasing preserves residual classical correlations, whereas gain and loss restore the mutual-information tracking of negativity. Our results establish the geometric decoherence time as a dynamical scale tracking the onset of decoherence.- 21 August 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 114 (10) , 105132
Geometric decoherence time in Lindbladian dynamics
The onset of decoherence in open many-body systems lacks a dynamical timescale grounded in the loss of bipartite entanglement. Here, we introduce the geometric decoherence time, defined as the earliest moment the monotone relation between logarithmic negativity and R\'enyi-$\frac{1}{2}$ entropy---exactly equal across any bipartition for pure states---breaks down under open-system evolution, signaling entropy growth without accompanying entanglement growth. We establish this criterion in both single-particle Gaussian dynamics and many-body Lindbladian evolution. We show that quantum mutual information provides a complementary long-time diagnostic: Its asymptotic vanishing is equivalent to factorization of the steady state across the bipartition, a condition strictly stronger than separability, and whenever a product steady state is approached exponentially in trace norm, negativity and mutual information share the same decay rate. In the presence of a strong symmetry, this tracking can fail---residual classical correlations can survive after entanglement has vanished. In the Kitaev chain with balanced gain and loss, we derive a closed-form solution and show that the topological phase sustains longer coherence times than the trivial phase at identical dissipation, with a local minimum at the chiral-symmetric point. In the interacting XXZ chain, exact many-body evolution shows that local $Z$ dephasing preserves residual classical correlations, whereas gain and loss restore the mutual-information tracking of negativity. Our results establish the geometric decoherence time as a dynamical scale tracking the onset of decoherence.- 24 June 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (23)
Dynamics of Majorana fermions on a quantum computer
- 24 June 2026
- Published by American Physical Society (APS) in Physical Review B
- Vol. 113 (23)
Dynamics of Majorana fermions on a quantum computer
- 16 December 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 112 (24)
Topological phase diagram of generalized Su-Schrieffer-Heeger models with interactions
- 16 December 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 112 (24)
Topological phase diagram of generalized Su-Schrieffer-Heeger models with interactions
- 24 September 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 112 (10)
Vortex stability in interacting Bose-Einstein condensates
- 24 September 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 112 (10)
Vortex stability in interacting Bose-Einstein condensates
- 25 April 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 111 (13)
SNS junctions along the BCS-BEC crossover
- 25 April 2025
- Published by American Physical Society (APS) in Physical Review B
- Vol. 111 (13)
SNS junctions along the BCS-BEC crossover
- Open Access
Vortex stability in interacting Bose-Einstein condensates
We study the stability of vortices in a binary system of Bose-Einstein condensates, with their wave functions modeled by a set of coupled, time-dependent Gross-Pitaevskii equations. Beginning with an effective two-dimensional system, we identify miscible and immiscible regimes characterized by the inter- and intra-atomic interactions and the initial configuration of the system. We then consider a binary system of Bose-Einstein condensates placed in a rotating harmonic trap and study the single vortex state in this system. We derive an approximate form for the energy of a single vortex in the binary system and the critical angular velocity for the global stability of a vortex at the center of the trap. We also compute the metastability onset angular velocity for the local stability of a vortex at the center of the trap. Numerical solutions to the Gross-Pitaevskii equations support these expressions. These rotational results inform us of a novel subphase within the miscible regime of the binary condensate system. We thus demonstrate the non-trivial aspects of vortex stability in interacting binary Bose-Einstein condensates as a result of their non-linear interactions.
Open AccessVortex stability in interacting Bose-Einstein condensates
We study the stability of vortices in a binary system of Bose-Einstein condensates, with their wave functions modeled by a set of coupled, time-dependent Gross-Pitaevskii equations. Beginning with an effective two-dimensional system, we identify miscible and immiscible regimes characterized by the inter- and intra-atomic interactions and the initial configuration of the system. We then consider a binary system of Bose-Einstein condensates placed in a rotating harmonic trap and study the single vortex state in this system. We derive an approximate form for the energy of a single vortex in the binary system and the critical angular velocity for the global stability of a vortex at the center of the trap. We also compute the metastability onset angular velocity for the local stability of a vortex at the center of the trap. Numerical solutions to the Gross-Pitaevskii equations support these expressions. These rotational results inform us of a novel subphase within the miscible regime of the binary condensate system. We thus demonstrate the non-trivial aspects of vortex stability in interacting binary Bose-Einstein condensates as a result of their non-linear interactions.
- Open Access
- 27 September 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (4) , 36
Collision Dynamics of One-Dimensional Bose–Einstein Condensates
We study the collision dynamics of two Bose–Einstein condensates, with their dynamical wave functions modeled by a set of coupled, time-dependent Gross–Pitaevskii equations. In an effective one-dimensional system, we identify regimes characterized by the relationship between inter- and intra-atomic interactions and the initial configuration of the system, akin to the equilibrium phase diagram of two interacting Bose condensates. We consider a dynamical setup in which two wave packets are initially at rest, with a small separation about the center of an anisotropic harmonic trap. Upon release, we observe a rapid approach to dynamical equilibrium in the limits of very large and very small inter-particle repulsion, characterized by periodic transmission or reflection of the condensates as distinguishable units, whereas the intermediate, critical regime is characterized by extended transient dynamics, density fracturing, and dynamical mixing.
- 27 September 2024
- Published by MDPI AG in Condensed Matter
- Vol. 9 (4) , 36
Open AccessCollision Dynamics of One-Dimensional Bose–Einstein Condensates
We study the collision dynamics of two Bose–Einstein condensates, with their dynamical wave functions modeled by a set of coupled, time-dependent Gross–Pitaevskii equations. In an effective one-dimensional system, we identify regimes characterized by the relationship between inter- and intra-atomic interactions and the initial configuration of the system, akin to the equilibrium phase diagram of two interacting Bose condensates. We consider a dynamical setup in which two wave packets are initially at rest, with a small separation about the center of an anisotropic harmonic trap. Upon release, we observe a rapid approach to dynamical equilibrium in the limits of very large and very small inter-particle repulsion, characterized by periodic transmission or reflection of the condensates as distinguishable units, whereas the intermediate, critical regime is characterized by extended transient dynamics, density fracturing, and dynamical mixing.
- Open Access
- 10 September 2024
- Published by IntechOpen
Hofstadter Butterflies in Topological Insulators
In this chapter, we investigate the energy spectra and the bulk and surface states in a two-dimensional system composed of a coupled stack of one-dimensional dimerized chains in the presence of an external magnetic field. Specifically, we analyze the Hofstadter butterfly patterns that emerge in a 2D stack of coupled 1D Su-Schrieffer-Heeger (SSH) chains subject to an external transverse magnetic field. Depending on the parameter regime, we find that the energy spectra of this hybrid topological system can exhibit topologically non-trivial bulk bands separated by energy gaps. Upon introducing boundaries into the system, we observe topologically protected in-gap surface states, which are protected either by a non-trivial Chern number or by inversion symmetry. We examine the resilience of these surface states against perturbations, confirming their expected stability against local symmetry-preserving perturbations.
- 10 September 2024
- Published by IntechOpen
Open AccessHofstadter Butterflies in Topological Insulators
In this chapter, we investigate the energy spectra and the bulk and surface states in a two-dimensional system composed of a coupled stack of one-dimensional dimerized chains in the presence of an external magnetic field. Specifically, we analyze the Hofstadter butterfly patterns that emerge in a 2D stack of coupled 1D Su-Schrieffer-Heeger (SSH) chains subject to an external transverse magnetic field. Depending on the parameter regime, we find that the energy spectra of this hybrid topological system can exhibit topologically non-trivial bulk bands separated by energy gaps. Upon introducing boundaries into the system, we observe topologically protected in-gap surface states, which are protected either by a non-trivial Chern number or by inversion symmetry. We examine the resilience of these surface states against perturbations, confirming their expected stability against local symmetry-preserving perturbations.
- 8 August 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (7)
Dynamics of symmetry-protected topological matter on a quantum computer
- 8 August 2024
- Published by American Physical Society (APS) in Physical Review B
- Vol. 110 (7)
Dynamics of symmetry-protected topological matter on a quantum computer
- 18 October 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (14) , L140203
Global quench dynamics and the growth of entanglement entropy in disordered spin chains with tunable range interactions
The nonequilibrium dynamics of disordered many-body quantum systems after a quantum quench unveils important insights about the competition between interactions and disorder, yielding, in particular, an interesting perspective toward the understanding of many-body localization. Still, the experimentally relevant effect of bond randomness in long-range interacting spin chains on their dynamical properties have so far not been investigated. In this Letter, we examine the entanglement entropy growth after a global quench in a quantum spin chain with randomly placed spins and long-range tunable interactions decaying with distance with power . Using a dynamical version of the strong disorder renormalization group we find for that the entanglement entropy grows logarithmically with time and becomes smaller with larger as . Here, . We present results of numerical exact diagonalization calculations for system sizes up to spins, in good agreement with the analytical results for sufficiently large . For , we find that the entanglement entropy grows as a power law with time, with a decaying function of the interaction exponent .- 18 October 2023
- Published by American Physical Society (APS) in Physical Review B
- Vol. 108 (14) , L140203
Global quench dynamics and the growth of entanglement entropy in disordered spin chains with tunable range interactions
The nonequilibrium dynamics of disordered many-body quantum systems after a quantum quench unveils important insights about the competition between interactions and disorder, yielding, in particular, an interesting perspective toward the understanding of many-body localization. Still, the experimentally relevant effect of bond randomness in long-range interacting spin chains on their dynamical properties have so far not been investigated. In this Letter, we examine the entanglement entropy growth after a global quench in a quantum spin chain with randomly placed spins and long-range tunable interactions decaying with distance with power . Using a dynamical version of the strong disorder renormalization group we find for that the entanglement entropy grows logarithmically with time and becomes smaller with larger as . Here, . We present results of numerical exact diagonalization calculations for system sizes up to spins, in good agreement with the analytical results for sufficiently large . For , we find that the entanglement entropy grows as a power law with time, with a decaying function of the interaction exponent .