Related Experiment Video
Updated: Dec 25, 2025

05:39
Scalable Quantum Integrated Circuits on Superconducting Two-Dimensional Electron Gas Platform
Published on: August 2, 2019
10.2K
Scaling and Diabatic Effects in Quantum Annealing with a D-Wave Device
Phillip Weinberg1, Marek Tylutki2,3, Jami M Rönkkö4
1Department of Physics, Boston University, 590 Commonwealth Avenue, Boston, Massachusetts 02215, USA.
Physical Review Letters
|March 24, 2020
Summary
We found an optimal annealing rate for quantum annealing on D-Wave systems, balancing quantum effects and noise to minimize errors. This rate is longer than individual qubit coherence times.
Area of Science:
- Quantum Computing
- Condensed Matter Physics
- Computational Physics
Background:
- Quantum annealing is a metaheuristic optimization algorithm.
- The transverse-field Ising model is a fundamental model in statistical mechanics and quantum computing.
- D-Wave systems are specialized quantum processors designed for quantum annealing.
Purpose of the Study:
- To investigate the optimal annealing rate for the 2D transverse-field Ising model on a D-Wave quantum annealer.
- To understand the interplay between quantum fluctuations and noise during the annealing process.
- To develop a model that explains the observed scaling of performance with annealing rate and lattice size.
Main Methods:
- Quantum annealing simulations on a D-Wave device with L×L lattices (L≤32).
- Analysis of residual energy and deviation from maximal magnetization in the final classical state.
- Development and validation of a phenomenological model to describe the results.
- Numerical solutions of the transverse-field Ising model with noise sources.
Main Results:
- An optimal annealing rate (v) was identified, dependent on lattice size (L), that minimizes residual energy and magnetization deviation.
- The optimal rate balances reduced quantum fluctuations (Kibble-Zurek mechanism evidence) against increasing noise impact at lower rates.
- A phenomenological model with specific power-law dependencies on v and L-dependent prefactors accurately describes the experimental and numerical results.
- The optimal annealing time exceeds individual qubit coherence times, explained by the model.
Conclusions:
- The performance of quantum annealing on the 2D transverse-field Ising model is sensitive to the annealing rate.
- A balance between quantum effects and noise is crucial for optimal performance.
- The observed scaling phenomena can be explained by a model incorporating competing effects and noise.
- The study provides insights into optimizing quantum annealing protocols and understanding their limitations.
Related Concept Videos
Ampere-Maxwell's Law: Problem-Solving
1.0K
A parallel-plate capacitor with capacitance C, whose plates have area A and separation distance d, is connected to a resistor R and a battery of voltage V. The current starts to flow at t = 0. What is the displacement current between the capacitor plates at time t? From the properties of the capacitor, what is the corresponding real current?
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
To solve the problem, we can use the equations from the analysis of an RC circuit and Maxwell's version of Ampère's law.
For the first part of the...
1.0K
Ampere's Law: Problem-Solving
4.2K
Ampere's law states that for any closed looped path, the line integral of the magnetic field along the path equals the vacuum permeability times the current enclosed in the loop. If the fingers of the right hand curl along the direction of the integration path, the current in the direction of the thumb is considered positive. The current opposite to the thumb direction is considered negative.
Specific steps need to be considered while calculating the symmetric magnetic field distribution...
Specific steps need to be considered while calculating the symmetric magnetic field distribution...
4.2K
Small-signal Diode Model
1.4K
In analyzing the behavior of diodes in circuits, the relationship between the current through a diode and the voltage across it is of particular interest, especially when considering the effect of a direct current (DC) bias voltage. When applied, this DC bias influences the diode's operating point, known as the Q point, around which the current-voltage (I-V) characteristic of the diode exhibits exponential behavior. Introducing a small, time-varying signal on top of this bias aids in examining...
1.4K
π Electron Effects on Chemical Shift: Overview
1.5K
An applied magnetic field causes loosely bound π-electrons in organic molecules to circulate, producing a local or induced diamagnetic field over a large spatial volume. As the molecules tumble in solution, the field generated by π-electrons in spherical substituents results in a zero net field. However, the net field generated by π-electrons in non-spherical substituents is not zero. The effect of this induced field depends on the orientation of the molecule with respect to B0,...
1.5K
Fermi Level Dynamics
578
The vacuum level denotes the energy threshold required for an electron to escape from a material surface. It is usually positioned above the conduction band of a semiconductor and acts as a benchmark for comparing electron energies within various materials.
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
Electron affinity in semiconductors refers to the energy gap between the minimum of its conduction band and the vacuum level and it is a critical parameter in determining how easily a semiconductor can accept additional electrons.
The work...
578
Types of Damping
7.4K
If the amount of damping in a system is gradually increased, the period and frequency start to become affected because damping opposes, and hence slows, the back and forth motion (the net force is smaller in both directions). If there is a very large amount of damping, the system does not even oscillate; instead, it slowly moves toward equilibrium. In brief, an overdamped system moves slowly towards equilibrium, whereas an underdamped system moves quickly to equilibrium but will oscillate about...
7.4K

