Related Experiment Video
Updated: Oct 5, 2025

06:42
Generation and Coherent Control of Pulsed Quantum Frequency Combs
Published on: June 8, 2018
9.1K
Phase-space simulations of feedback coherent Ising machines
Optics Letters
|February 1, 2022
Summary
A novel phase-space simulation technique enables exact quantum computations for the coherent Ising machine. This method allows solving complex optimization problems using quantum feedback devices.
Area of Science:
- Quantum Computing
- Computational Physics
- Optimization
Background:
- The coherent Ising machine (CIM) is a quantum computing architecture with potential for solving complex problems.
- Exact simulations of quantum systems are computationally demanding, limiting the study of devices like the CIM.
- Developing efficient simulation techniques is crucial for advancing quantum computing hardware and applications.
Purpose of the Study:
- To introduce a new, exact positive-P phase-space simulation technique for the coherent Ising machine quantum computer.
- To demonstrate that by designing the coupling matrix, general hard optimization problems can be solved using this technique.
- To validate the technique through computational simulations of a photonic parametric network implementing the CIM.
Main Methods:
- Development of an exact positive-P phase-space algorithm tailored for quantum simulations.
- Design of specific coupling matrices to map general hard optimization problems onto the CIM.
- Implementation of computational quantum simulations using a feedback-type photonic parametric network.
Main Results:
- Successful demonstration of exact positive-P phase-space simulations for the coherent Ising machine.
- Validation of the technique's capability to solve general hard optimization problems.
- Obtained success rate results from scalable quantum simulations of quantum feedback devices.
Conclusions:
- The presented phase-space simulation technique offers an exact and scalable method for studying the coherent Ising machine.
- This approach facilitates the investigation of CIM's potential for solving complex optimization problems.
- The findings pave the way for more efficient quantum simulations of quantum feedback systems.
Related Concept Videos
State Space to Transfer Function
341
The conversion of state-space representation to a transfer function is a fundamental process in system analysis. It provides a method for transitioning from a time-domain description to a frequency-domain representation, which is crucial for simplifying the analysis and design of control systems.
The transformation process begins with the state-space representation, characterized by the state equation and the output equation. These equations are typically represented as:
The transformation process begins with the state-space representation, characterized by the state equation and the output equation. These equations are typically represented as:
341
BIBO stability of continuous and discrete -time systems
565
System stability is a fundamental concept in signal processing, often assessed using convolution. For a system to be considered bounded-input bounded-output (BIBO) stable, any bounded input signal must produce a bounded output signal. A bounded input signal is one where the modulus does not exceed a certain constant at any point in time.
To determine the BIBO stability, the convolution integral is utilized when a bounded continuous-time input is applied to a Linear Time-Invariant (LTI) system....
To determine the BIBO stability, the convolution integral is utilized when a bounded continuous-time input is applied to a Linear Time-Invariant (LTI) system....
565
Simplified Synchronous Machine Model
348
The Synchronous Machine Model is a fundamental tool in analyzing and ensuring the transient stability of power systems. This model simplifies the representation of a synchronous machine under balanced three-phase positive-sequence conditions, assuming constant excitation and ignoring losses and saturation. The model is pivotal for understanding the behavior of synchronous generators connected to a power grid, particularly during transient events.
In this model, each generator is connected to a...
In this model, each generator is connected to a...
348
State Space Representation
320
The frequency-domain technique, commonly used in analyzing and designing feedback control systems, is effective for linear, time-invariant systems. However, it falls short when dealing with nonlinear, time-varying, and multiple-input multiple-output systems. The time-domain or state-space approach addresses these limitations by utilizing state variables to construct simultaneous, first-order differential equations, known as state equations, for an nth-order system.
Consider an RLC circuit, a...
Consider an RLC circuit, a...
320
Transfer Function to State Space
443
State-space representation is a powerful tool for simulating physical systems on digital computers, necessitating the conversion of the transfer function into state-space form. Consider an nth-order linear differential equation with constant coefficients, like those encountered in an RLC circuit. The state variables are selected as the output and its n−1 derivatives. Differentiating these variables and substituting them back into the original equation produces the state equations.
In an...
In an...
443
Fermi Level Dynamics
372
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...
372

