Probing molecular spectral functions and unconventional pairing using Raman spectroscopy

被引:2
|
作者
Diessel, Oriana K. [1 ,2 ,3 ,4 ]
von Milczewski, Jonas [1 ,2 ,4 ,5 ]
Christianen, Arthur [1 ,2 ]
Schmidt, Richard [1 ,2 ,5 ,6 ]
机构
[1] Max Planck Inst Quantum Opt, Hans Kopfermann Str 1, D-85748 Garching, Germany
[2] Munich Ctr Quantum Sci & Technol MCQST, Schellingstr 4, D-80799 Munich, Germany
[3] Harvard & Smithsonian, Ctr Astrophys, ITAMP, Cambridge, MA 02138 USA
[4] Harvard Univ, Dept Phys, Cambridge, MA 02138 USA
[5] Heidelberg Univ, Inst Theoret Phys, Philosophenweg 16, D-69120 Heidelberg, Germany
[6] Aarhus Univ, Ctr Complex Quantum Syst, Dept Phys & Astron, DK-8000 Aarhus C, Denmark
来源
PHYSICAL REVIEW RESEARCH | 2024年 / 6卷 / 02期
基金
新加坡国家研究基金会;
关键词
NUMEROV METHOD; SUPERCONDUCTIVITY; CONDENSATION;
D O I
10.1103/PhysRevResearch.6.023239
中图分类号
O4 [物理学];
学科分类号
0702 ;
摘要
An impurity interacting with an ultracold Fermi gas can form either a polaron state or a dressed molecular state, the molaron, in which the impurity forms a bound state with one gas particle. This molaron state features rich physics, including a negative effective mass around unitarity and a first-order transition to the polaron state. However, these features have remained so far experimentally inaccessible. In this work we show theoretically how the molaron state can be directly prepared experimentally even in its excited states using Raman spectroscopy techniques. Initializing the system in the ultrastrong coupling limit, where the binding energy of the molaron is much larger than the Fermi energy, our protocol maps out the momentum-dependent spectral function of the molecule. Using a diagrammatic approach we furthermore show that the molecular spectral function serves as a direct precursor of the elusive Fulde-Ferell-Larkin-Ovchinnikov phase, which is realized for a finite density of fermionic impurity particles. Our results pave the way to a systematic understanding of how composite particles form in quantum many-body environments and provide a basis to develop new schemes for the observation of exotic phases of quantum many-body systems.
引用
收藏
页数:10
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