Related Experiment Video
Updated: Mar 6, 2026

10:00
Gradient Echo Quantum Memory in Warm Atomic Vapor
Published on: November 11, 2013
13.3K
Demonstration of an ac Josephson junction laser
M C Cassidy1, A Bruno1, S Rubbert2
1QuTech, Delft University of Technology, P.O. Box 5046, 2600 GA Delft, Netherlands.
Summary
Researchers demonstrate a superconducting laser using the ac Josephson effect. This device efficiently generates coherent microwave photons on-chip for quantum computing applications.
Area of Science:
- Superconducting electronics
- Quantum optics
- Solid-state physics
Background:
- Superconducting devices offer high speeds and low energy loss, making them promising for computing.
- Demonstrating coherence, such as lasing, is crucial for advancing superconducting technologies.
- The ac Josephson effect is a fundamental property of superconductors with potential for photon generation.
Purpose of the Study:
- To demonstrate a superconducting laser utilizing the ac Josephson effect.
- To achieve efficient on-chip generation of coherent microwave photons at low temperatures.
- To explore the integration of Josephson junction-based lasers with quantum devices.
Main Methods:
- Fabricated a Josephson junction strongly coupled to a superconducting cavity.
- Applied a DC voltage bias across the Josephson junction to generate microwave photons.
- Utilized circuit nonlinearity for down-conversion of Josephson frequencies to the cavity's fundamental mode.
Main Results:
- Successfully demonstrated lasing using a Josephson junction and superconducting cavity.
- Achieved efficient down-conversion of higher-order Josephson frequencies to the cavity's fundamental mode.
- Showcased the potential for on-chip generation of coherent microwave photons.
Conclusions:
- Superconducting lasers based on the ac Josephson effect are feasible.
- This technology enables efficient, low-temperature microwave photon generation for quantum applications.
- The simple design facilitates integration with other quantum electronic devices.
Related Concept Videos
P-N junction
1.5K
A p-n junction is formed when p-type and n-type semiconductor materials are joined together. At the interface of the p-n junction, holes from the p-side and electrons from the n-side begin to diffuse into the opposite sides due to the concentration gradient. This diffusion of carriers leads to a region around the junction where there are no free charge carriers, known as the depletion region. The charge density within the depletion region for the n-side and p-side can be described by the...
1.5K
Photoelectric Effect
40.6K
When light of a particular wavelength strikes a metal surface, electrons are emitted. This is called the photoelectric effect. The minimum frequency of light that can cause such emission of electrons is called the threshold frequency, which is specific to the metal. Light with a frequency lower than the threshold frequency, even if it is of high intensity, cannot initiate the emission of electrons. However, when the frequency is higher than the threshold value, the number of electrons ejected...
40.6K
Confocal Fluorescence Microscopy
21.6K
Confocal microscopy is an advanced microscopic technique. The prime advantage of the confocal microscope over other microscopy techniques is its ability to block the out-of-focus light from the illuminated samples using pinholes. It is widely used with fluorescence optics to obtain high-resolution, sharp contrast images. Unlike optical microscopes, confocal microscopes use a focused beam of light laser to scan the entire sample surface at different z-planes. These microscopes are, therefore,...
21.6K
LC Circuits
3.5K
An LC circuit consists of an inductor and a capacitor, either in series or parallel. Consider a charged capacitor connected with an inductor in series. Before the switch is closed, all the energy of the circuit is stored in the electric field of the capacitor. When the switch is closed, the capacitor begins to discharge, producing a current in the circuit. The current, in turn, creates a magnetic field in the inductor. Because of the induced emf in the inductor, the current cannot change...
3.5K
Biasing of P-N Junction
2.3K
The operation of a p-n junction diode involves various biasing conditions, including forward bias, reverse bias, and equilibrium.
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
In equilibrium, no external voltage is applied across the p-n junction. The depletion region is formed at the junction interface due to the diffusion of carriers, which leaves behind charged dopants, acceptors on the p-side, and donors on the n-side. These immobile charges create an electric field that prevents further diffusion of carriers. The related energy band...
2.3K
Oscillations In An LC Circuit
3.3K
An idealized LC circuit of zero resistance can oscillate without any source of emf by shifting the energy stored in the circuit between the electric and magnetic fields. In such an LC circuit, if the capacitor contains a charge q before the switch is closed, then all the energy of the circuit is initially stored in the electric field of the capacitor. This energy is given by
3.3K

