Related Experiment Video
Updated: Dec 31, 2025

10:26
Fabrication and Characterization of Superconducting Resonators
Published on: May 21, 2016
11.8K
Ultrastrong Parametric Coupling between a Superconducting Cavity and a Mechanical Resonator
G A Peterson1,2, S Kotler1,2, F Lecocq1,2
1National Institute of Standards and Technology, 325 Broadway, Boulder, Colorado 80305, USA.
Physical Review Letters
|January 11, 2020
Summary
We developed a novel optomechanical device demonstrating ultrastrong parametric coupling in superconducting cavities. This breakthrough enables enhanced frequency splitting and opens doors for ultrafast quantum applications.
Area of Science:
- Quantum physics
- Optomechanics
- Superconducting circuits
Background:
- Optomechanical systems couple mechanical motion to light.
- Superconducting circuits are vital for quantum technologies.
- Ultrastrong coupling regimes are sought for advanced quantum phenomena.
Purpose of the Study:
- To introduce a new optomechanical device architecture.
- To achieve and characterize ultrastrong parametric coupling.
- To explore potential applications in quantum information processing.
Main Methods:
- Fabrication of a micromechanical membrane coupled to a 3D superconducting cavity.
- Experimental realization of parametric coupling exceeding system dissipation and mechanical frequency.
- Measurement of hybridized normal mode frequency splitting.
Main Results:
- Achieved ultrastrong parametric coupling in the optomechanical device.
- Observed a frequency splitting of 88% of the bare mechanical frequency.
- Demonstrated coupling rates surpassing mechanical thermal decoherence.
Conclusions:
- The developed device enables ultrastrong coupling in an optomechanical system.
- The observed effects pave the way for ultrafast quantum state transfer.
- Potential for generating entanglement in superconducting circuits is highlighted.
Related Concept Videos
Sound Waves: Resonance
3.1K
Resonance is produced depending on the boundary conditions imposed on a wave. Resonance can be produced in a string under tension with symmetrical boundary conditions (i.e., has a node at each end). A node is defined as a fixed point where the string does not move. The symmetrical boundary conditions result in some frequencies resonating and producing standing waves, while other frequencies interfere destructively. Sound waves can resonate in a hollow tube, and the frequencies of the sound...
3.1K
Magnetic Damping
963
Eddy currents can produce significant drag on motion, called magnetic damping. For instance, when a metallic pendulum bob swings between the poles of a strong magnet, significant drag acts on the bob as it enters and leaves the field, quickly damping the motion.
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
If, however, the bob is a slotted metal plate, the magnet produces a much smaller effect. When a slotted metal plate enters the field, an emf is induced by the change in flux; however, it is less effective because the slots limit the...
963
Standing Waves in a Cavity
1.4K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.4K
Double Resonance Techniques: Overview
633
Double resonance techniques in Nuclear Magnetic Resonance (NMR) spectroscopy involve the simultaneous application of two different frequencies or radiofrequency pulses to manipulate and observe two distinct nuclear spins. One important application of double resonance is spin decoupling, which selectively suppresses coupling with one type of nucleus while observing the NMR signal from another nucleus, simplifying the spectrum and enhancing resolution.
Spin decoupling is usually achieved by...
Spin decoupling is usually achieved by...
633
Spin–Spin Coupling Constant: Overview
1.4K
In bromoethane, the three methyl protons are coupled to the two methylene protons that are three bonds away. In accordance with the n+1 rule, the signal from the methyl protons is split into three peaks with 1:2:1 relative intensities. The methylene protons appear as a quartet, with the relative intensities of 1:3:3:1.
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
Qualitatively, any spin plus-half nucleus polarizes the spins of its electrons to the minus-half state. Consequently, the paired electron in the hydrogen–carbon bond must...
1.4K
Parallel Resonance
460
The parallel RLC circuit is an arrangement where the resistor (R), inductor (L), and capacitor (C) are all connected to the same nodes and, as a result, share the same voltage across them. The parallel RLC circuit is analyzed in terms of admittance (Y), which reflects the ease with which current can flow. The admittance is given by:
460

