Broadband Lamb shift in an engineered quantum system
The shift of the energy levels of a quantum system owing to broadband electromagnetic vacuum fluctuations—the Lamb shift—has been central for the development of quantum electrodynamics and for the understanding of atomic spectra 1 – 6 . Identifying the origin of small energy shifts is still importan...
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Veröffentlicht in: | Nature physics 2019-06, Vol.15 (6), p.533-537 |
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Sprache: | eng |
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Zusammenfassung: | The shift of the energy levels of a quantum system owing to broadband electromagnetic vacuum fluctuations—the Lamb shift—has been central for the development of quantum electrodynamics and for the understanding of atomic spectra
1
–
6
. Identifying the origin of small energy shifts is still important for engineered quantum systems, in light of the extreme precision required for applications such as quantum computing
7
,
8
. However, it is challenging to resolve the Lamb shift in its original broadband case in the absence of a tuneable environment. Consequently, previous observations
1
–
5
,
9
in non-atomic systems are limited to environments comprising narrowband modes
10
–
12
. Here, we observe a broadband Lamb shift in high-quality superconducting resonators, a scenario also accessing static shifts inaccessible in Lamb’s experiment
1
,
2
. We measure a continuous change of several megahertz in the fundamental resonator frequency by externally tuning the coupling strength to the engineered broadband environment, which is based on hybrid normal-metal–insulator–superconductor tunnel junctions
13
–
15
. Our results may lead to improved control of dissipation in high-quality engineered quantum systems and open new possibilities for studying synthetic open quantum matter
16
–
18
using this hybrid experimental platform.
The measured change in the fundamental frequency of a superconducting resonator coupled to a tunnel junction reveals a broadband constant Lamb shift, which is typically inaccessible in atomic systems. |
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ISSN: | 1745-2473 1745-2481 |
DOI: | 10.1038/s41567-019-0449-0 |