Conveners
Quantumsimulation
- Hans Michel (Universität Hamburg)
Quantumsimulation
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Magnus Michael Rusch (Universität Tübingen)06/10/2026, 11:45Talk
We present the current status of our experimental setup for imaging ${}^6$Li atoms in near-resonant optical tweezers.
The tweezers are generated using light at a wavelength of $674.6 \text{ nm}$, close to the ${}^6$Li $D$-line resonance at $671 \text{ nm}$. This configuration provides a promising platform for combination with an optical lattice operating at $841 \text{ nm}$. The chosen...
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David Gopalan (RPTU Kaiserslautern-Landau)06/10/2026, 12:00Talk
Ultracold quantum gases are versatile model systems for quantum simulation, since both the quantum gas itself and its surrounding potential landscape can be controlled with high precision [1].
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The generation of nearly arbitrary optical potentials is made possible through Digital Micromirror Devices (DMDs), which consist of arrays of individually tiltable micrometer-sized mirrors.
Here, I... -
Om Pote (Johannes Gutenberg Universität-Mainz)06/10/2026, 12:15Talk
Abstract
The preparation of excited many-body eigenstates is a central challenge in quantum simulation. In the Fermi–Hubbard model, the double well constitutes a local building block of a many body extended system. In this thesis, a controlled scheme for preparing two-particle eigenstates of a repulsively interacting fermions in a double-well system is developed and experimentally...
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Vicente Yael Baca Montero (RPTU Kaiserslautern Landau)07/10/2026, 11:30Talk
In recent years, radio-frequency (RF) magnetic fields have become increasingly important tools in ultracold-atom and quantum-gas experiments. Because many of these experiments rely on glass-cell vacuum chambers, where stable ultra-high vacuum (UHV) is critical, it is essential to verify that the presence of an RF coil (or any source of time-dependent magnetic fields) does not compromise vacuum...
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Juan Antonio Luna Gutierrez (RPTU Kaiserslautern and University of Hamburg)07/10/2026, 11:45Talk
The superradiant phase transition takes place when an ensemble of ultracold atoms collectively coupled to a single-mode cavity is transversally driven by a classical coherent pump. Above a critical drive strength, the system transitions from a normal to a superradiant phase, building up a non-zero cavity field while the atoms form a crystalline pattern. In this work, we extend this standard...
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