Related Experiment Video
Updated: Feb 7, 2026

07:56
A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
Published on: September 5, 2019
9.0K
Efficient entanglement generation between exciton-polaritons using shortcuts to adiabaticity
Optics Letters
|July 14, 2018
Summary
Shortcuts to adiabaticity efficiently generate entanglement between exciton-polaritons in semiconductor microcavities. This method surpasses previous techniques by utilizing time-dependent nonlinearity for enhanced quantum dynamics.
Area of Science:
- Quantum optics
- Condensed matter physics
- Nonlinear dynamics
Background:
- Exciton-polaritons are quasiparticles formed from the coupling of excitons and photons in semiconductor microcavities.
- Generating entanglement between these quasiparticles is crucial for quantum information processing.
- Adiabatic quantum dynamics is a standard method for controlling quantum systems, but can be slow.
Purpose of the Study:
- To develop an efficient method for generating entanglement between exciton-polaritons.
- To improve upon existing methods for enhancing nonlinearity in coupled microcavity systems.
- To explore the application of shortcuts to adiabaticity in quantum optics.
Main Methods:
- Utilizing shortcuts to adiabaticity to accelerate quantum dynamics.
- Implementing a time-dependent nonlinearity in coupled semiconductor microcavities.
- Comparing the entanglement generation efficiency with a conventional method using constant nonlinearity.
Main Results:
- Achieved efficient generation of entanglement between exciton-polaritons.
- Demonstrated substantial improvement over a recently proposed method.
- Showcased the advantage of time-dependent nonlinearity exceeding Josephson coupling.
Conclusions:
- Shortcuts to adiabaticity provide an efficient route for exciton-polariton entanglement.
- Time-dependent nonlinearity offers superior control compared to constant nonlinearity.
- The proposed method has potential applications in other areas of nonlinear optics.
Related Concept Videos
Work Done in an Adiabatic Process
4.3K
Consider the adiabatic compression of an ideal gas in the cylinder of an automobile diesel engine. The gasoline vapor is injected into the cylinder of an automobile engine when the piston is in its expanded position. The temperature, pressure, and volume of the resulting gas-air mixture are 20 °C, 1.00 x 105 N/m2, and 240 cm3 , respectively. The mixture is then compressed adiabatically to a volume of 40 cm3. Note that, in the actual operation of an automobile engine, the compression is not...
4.3K
Adiabatic Processes for an Ideal Gas
4.1K
When an ideal gas is compressed adiabatically, that is, without adding heat, work is done on it, and its temperature increases. In an adiabatic expansion, the gas does work, and its temperature drops. Adiabatic compressions actually occur in the cylinders of a car, where the compressions of the gas-air mixture take place so quickly that there is no time for the mixture to exchange heat with its environment. Nevertheless, because work is done on the mixture during the compression, its...
4.1K
Pressure and Volume in an Adiabatic Process
3.5K
Free expansion of a gas is an adiabatic process. However, there are few differences between free expansion and adiabatic expansion. During free expansion, no work is done, and there is no change in internal energy. But, for an adiabatic expansion, work is done, and there is a change in internal energy. During an adiabatic process, the relation between the pressure and volume is obtained from the condition for the adiabatic process, that is,
3.5K
Production Efficiency
18.4K
Net production efficiency (NPE) is the efficiency at which organisms assimilate energy into biomass for the next trophic level. Due to low metabolic rates and less energy spent on thermoregulatory processes, the NPE of ectotherms (cold-blooded animals) is 10 times higher than endotherms (warm-blooded animals).
18.4K
Trophic Efficiency
25.2K
Trophic level transfer efficiency (TLTE) is a measure of the total energy transfer from one trophic level to the next. Due to extensive energy loss as metabolic heat, an average of only 10% of the original energy obtained is passed on to the next level. This pattern of energy loss severely limits the possible number of trophic levels in a food chain.
25.2K
Efficiency of The Carnot Cycle
3.7K
The hypothetical Carnot cycle consists of an ideal gas subjected to two isothermal and two adiabatic processes. Since the internal energy of an ideal gas depends only on its temperature, which is the same before and after the completion of the Carnot cycle, there is no change in its internal energy. Hence, using the first law of thermodynamics, the total heat exchanged by the ideal gas equals the total work done. Thus, we can quantify the efficiency of the Carnot cycle via the heat exchanged...
3.7K

