Related Experiment Video
Updated: May 13, 2025

05:39
Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
9.5K
The open driven two-level system at conical intersections of quasienergies
1Instituto de Ciencia de Materiales de Madrid, CSIC, E-28049 Madrid, Spain.
The Journal of Chemical Physics
|April 15, 2025
Summary
This study explores ac-driven two-level systems interacting with a fermionic environment. It reveals a temperature-dependent crossover in system state, shifting from a Floquet-Gibbs-like behavior to a mean-energy dominated state.
Area of Science:
- Quantum mechanics
- Condensed matter physics
- Statistical mechanics
Background:
- Investigating the stationary state of quantum systems is crucial for understanding their long-term behavior.
- Two-level systems are fundamental models in quantum physics, with applications in quantum computing and spectroscopy.
- Particle exchange with an environment introduces dissipation and decoherence, significantly altering system dynamics.
Purpose of the Study:
- To determine if Floquet state populations are governed by quasienergies or mean energies in an ac-driven two-level system.
- To explore the behavior near conical intersections of quasienergies where these energy definitions diverge.
- To identify temperature-driven transitions in the system's stationary state.
Main Methods:
- Theoretical analysis of an ac-driven two-level system coupled to a fermionic bath.
- Focus on parameter regimes near conical intersections of quasienergies.
- Numerical calculations to validate analytical estimates.
Main Results:
- A crossover is observed in the system's stationary state as a function of temperature.
- At low temperatures, the system exhibits a Floquet-Gibbs-like state.
- At intermediate temperatures, the system transitions to a state dominated by mean energy.
Conclusions:
- The system's stationary state is not solely determined by quasienergies or mean energies but exhibits a temperature-dependent crossover.
- The vicinity of conical intersections is key to observing distinct behaviors related to quasienergies and mean energies.
- Findings provide insights into thermalization and energy dynamics in open quantum systems.
Related Concept Videos
One-Degree-of-Freedom System
440
In mechanical engineering, one-degree-of-freedom systems form the basis of a wide range of electrical and mechanical components. Using these models, engineers can predict the behavior of various parts in a larger system, which gives them insight into how different forces interact with each other.
A one-degree-of-freedom system is defined by an independent variable that determines its state and behavior. One example of a one-degree-of-freedom system is a simple harmonic oscillator, such as a...
A one-degree-of-freedom system is defined by an independent variable that determines its state and behavior. One example of a one-degree-of-freedom system is a simple harmonic oscillator, such as a...
440
Conservation of Energy in Control Volume
410
Consider a turbine operating under steady-flow conditions. The control volume is drawn around the turbine, with fluid entering at one point and exiting at another. The turbine extracts energy from the fluid, which performs mechanical work (shaft work).
For steady flow systems, the time derivative of the stored energy becomes zero since there is no energy accumulation within the control volume. This simplifies the energy equation to:
For steady flow systems, the time derivative of the stored energy becomes zero since there is no energy accumulation within the control volume. This simplifies the energy equation to:
410
Second Order systems II
69
In an underdamped second-order system, where the damping ratio ζ is between 0 and 1, a unit-step input results in a transfer function that, when transformed using the inverse Laplace method, reveals the output response. The output exhibits a damped sinusoidal oscillation, and the difference between the input and output is termed the error signal. This error signal also demonstrates damped oscillatory behavior. Eventually, as the system reaches a steady state, the error diminishes to zero.
69
Energy Conservation and Bernoulli's Equation
7.6K
Applying the conservation of energy principle or the work-energy theorem to an incompressible, inviscid fluid in laminar, steady, irrotational flow leads to Bernoulli's equation. It states that the sum of the fluid pressure, potential, and kinetic energy per unit volume is constant along a streamline.
All the terms in the equation have the dimension of energy per unit volume. The kinetic energy per unit volume is called the kinetic energy density, and the potential energy per unit volume is...
All the terms in the equation have the dimension of energy per unit volume. The kinetic energy per unit volume is called the kinetic energy density, and the potential energy per unit volume is...
7.6K
Energy Diagrams - II
4.6K
Energy diagrams are important to understand the dynamics of a system. The topology of an energy diagram helps illustrate the equilibrium points of the system.
The point in the energy diagram at which the system’s potential energy is the lowest is known as the local minima. The system tends to stay in this position indefinitely unless acted upon by a net force. The slope of the potential energy diagram at the local minima is zero, indicating that zero net force is acting on the system. The...
The point in the energy diagram at which the system’s potential energy is the lowest is known as the local minima. The system tends to stay in this position indefinitely unless acted upon by a net force. The slope of the potential energy diagram at the local minima is zero, indicating that zero net force is acting on the system. The...
4.6K
Second Order systems I
119
A servo system exemplifies a second-order system, featuring a proportional controller and load elements that ensure the output position aligns with the input position. The relationship between these components is described by a second-order differential equation. Applying the Laplace transform under zero initial conditions yields the transfer function, showing how inputs are converted to outputs in the system.
By reinterpreting the system, one can derive the closed-loop transfer function, which...
By reinterpreting the system, one can derive the closed-loop transfer function, which...
119

