Related Experiment Video
Updated: Jun 9, 2025

07:03
Measuring Magnetically-Tuned Ferroelectric Polarization in Liquid Crystals
Published on: August 15, 2018
8.7K
Circularly polarized radiation to control the superconducting states: stability analysis
M D Croitoru1,2, A I Buzdin1,3
1University of Bordeaux, LOMA UMR-CNRS 5798, F-33405 Talence, France.
Summary
Switching quantum states in superconducting nanorings using circularly polarized radiation is feasible. Numerical simulations confirm the method
Area of Science:
- Condensed matter physics
- Quantum optics
- Superconducting devices
Background:
- Circularly polarized radiation offers potential for on-demand quantum state switching in superconducting nanorings.
- The stability of this switching mechanism against environmental and material variations is a critical concern for experimental realization.
Purpose of the Study:
- To investigate the robustness of quantum state switching in superconducting nanorings under realistic conditions.
- To assess the impact of local variations in superconducting properties and magnetic flux fluctuations on the switching behavior.
Main Methods:
- Numerical simulations employing the time-dependent Ginzburg-Landau equation.
- Analysis of switching dynamics under simulated perturbations.
Main Results:
- The quantum state switching phenomena in superconducting nanorings demonstrate remarkable robustness.
- Local variations and flux fluctuations do not significantly impede the switching behavior.
Conclusions:
- The proposed method for quantum state switching using circularly polarized radiation is experimentally viable.
- The inherent stability of the system provides confidence for future experimental validation and applications.
Keywords:
Helicity-controlled switching of superconducting statescircularly polarized radiationdefectsinverse Faraday effectMore Related Videos
Related Concept Videos
Pole and System Stability
252
The transfer function is a fundamental concept representing the ratio of two polynomials. The numerator and denominator encapsulate the system's dynamics. The zeros and poles of this transfer function are critical in determining the system's behavior and stability.
Simple poles are unique roots of the denominator polynomial. Each simple pole corresponds to a distinct solution to the system's characteristic equation, typically resulting in exponential decay terms in the system's...
Simple poles are unique roots of the denominator polynomial. Each simple pole corresponds to a distinct solution to the system's characteristic equation, typically resulting in exponential decay terms in the system's...
252
Atomic Nuclei: Nuclear Relaxation Processes
632
In the absence of an external magnetic field, nuclear spin states are degenerate and randomly oriented. When a magnetic field is applied, the spins begin to precess and orient themselves along (lower energy) or against (higher energy) the direction of the field. At equilibrium, a slight excess population of spins exists in the lower energy state. Because the direction of the magnetic field is fixed as the z-axis, the precessing magnetic moments are randomly oriented around the z-axis.
632
Stability
93
The time response of a linear time-invariant (LTI) system can be divided into transient and steady-state responses. The transient response represents the system's initial reaction to a change in input and diminishes to zero over time. In contrast, the steady-state response is the behavior that persists after the transient effects have faded.
The stability of an LTI system is determined by the roots of its characteristic equation, known as poles. A system is stable if it produces a bounded...
The stability of an LTI system is determined by the roots of its characteristic equation, known as poles. A system is stable if it produces a bounded...
93
Potential Due to a Polarized Object
367
A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
367
Standing Electromagnetic Waves
1.5K
Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
1.5K
Types Of Superconductors
944
A superconductor is a substance that offers zero resistance to the electric current when it drops below a critical temperature. Zero resistance is not the only interesting phenomenon as materials reach their transition temperatures. A second effect is the exclusion of magnetic fields. This is known as the Meissner effect. A light, permanent magnet placed over a superconducting sample will levitate in a stable position above the superconductor. High-speed trains that levitate on strong...
944

