Jove
Visualize
Contact Us
JoVE
x logofacebook logolinkedin logoyoutube logo
ABOUT JoVE
OverviewLeadershipBlogJoVE Help Center
AUTHORS
Publishing ProcessEditorial BoardScope & PoliciesPeer ReviewFAQSubmit
LIBRARIANS
TestimonialsSubscriptionsAccessResourcesLibrary Advisory BoardFAQ
RESEARCH
JoVE JournalMethods CollectionsJoVE Encyclopedia of ExperimentsArchive
EDUCATION
JoVE CoreJoVE BusinessJoVE Science EducationJoVE Lab ManualFaculty Resource CenterFaculty Site
Terms & Conditions of Use
Privacy Policy
Policies

Related Concept Videos

The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.7K
Shortly after de Broglie published his ideas that the electron in a hydrogen atom could be better thought of as being a circular standing wave instead of a particle moving in quantized circular orbits, Erwin Schrödinger extended de Broglie’s work by deriving what is now known as the Schrödinger equation. When Schrödinger applied his equation to hydrogen-like atoms, he was able to reproduce Bohr’s expression for the energy and, thus, the Rydberg formula governing hydrogen spectra.
42.7K
Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

757
An experiment often consists of more than a single step. In this case, measurements at each step give rise to uncertainty. Because the measurements occur in successive steps, the uncertainty in one step necessarily contributes to that in the subsequent step. As we perform statistical analysis on these types of experiments, we must learn to account for the propagation of uncertainty from one step to the next. The propagation of uncertainty depends on the type of arithmetic operation performed on...
757
The de Broglie Wavelength02:32

The de Broglie Wavelength

26.1K
In the macroscopic world, objects that are large enough to be seen by the naked eye follow the rules of classical physics. A billiard ball moving on a table will behave like a particle; it will continue traveling in a straight line unless it collides with another ball, or it is acted on by some other force, such as friction. The ball has a well-defined position and velocity or well-defined momentum, p = mv, which is defined by mass m and velocity v at any given moment. This is the typical...
26.1K
Propagation of Uncertainty from Systematic Error01:10

Propagation of Uncertainty from Systematic Error

580
The atomic mass of an element varies due to the relative ratio of its isotopes. A sample's relative proportion of oxygen isotopes influences its average atomic mass. For instance, if we were to measure the atomic mass of oxygen from a sample, the mass would be a weighted average of the isotopic masses of oxygen in that sample. Since a single sample is not likely to perfectly reflect the true atomic mass of oxygen for all the molecules of oxygen on Earth, the mass we obtain from this...
580
Randomized Experiments01:13

Randomized Experiments

7.1K
The randomization process involves assigning study participants randomly to experimental or control groups based on their probability of being equally assigned. Randomization is meant to eliminate selection bias and balance known and unknown confounding factors so that the control group is similar to the treatment group as much as possible. A computer program and a random number generator can be used to assign participants to groups in a way that minimizes bias.
Simple randomization
Simple...
7.1K
Propagation of Action Potentials01:23

Propagation of Action Potentials

6.2K
The propagation of an action potential refers to the process by which a nerve impulse, or "action potential," travels along a neuron.
Neurons (nerve cells) have a resting membrane potential, with a slightly negative charge inside compared to outside. This is maintained by ion channels, such as sodium (Na+) and potassium (K+) channels, which control the flow of ions. When a stimulus, like a touch or a signal from another neuron, triggers the neuron, sodium channels open, allowing sodium ions to...
6.2K

You might also read

Related Articles

Articles linked to this work by shared authors, journal, and citation graph.

Sort by
Same author

High-Fidelity Controlled-Phase Gate for Binomial Codes via Geometric Phase Engineering.

Physical review letters·2026
Same author

Magnetic-Free Optical Mode Degeneracy Lifting in Lithium Niobate Microring Resonators.

Physical review letters·2026
Same author

Experimental Demonstration of Entanglement Pumping with Bosonic Logical Qubits.

Physical review letters·2026
Same author

Fiber-to-chip grating couplers for lithium niobate on sapphire.

Applied optics·2026
Same author

Fully tunable optical filter based on a thin-film lithium niobate microring resonator.

Optics letters·2026
Same author

Cavity photothermal oscillation spectroscopy generation in an optofluidic microbubble resonator for multi-component mixture solution detection.

Optics letters·2026
Same journal

A 44-min periodic radio transient in a supernova remnant.

Science bulletin·2026
Same journal

Theoretical prediction of semiconductors by data driven light-element substitution in topological materials.

Science bulletin·2026
Same journal

Polymer-regulated crystallization enables scalable, high-performance heterostructured perovskite luminescent optoelectronic fibers.

Science bulletin·2026
Same journal

Global fits and the search for new physics: past, present and future.

Science bulletin·2026
Same journal

Pancancer pro-angiogenic atlas unravels tumor-educated pericyte-augmented anti-angiogenic resistance.

Science bulletin·2026
Same journal

Supramolecular nanomedicine reprogramming calcium ions metabolism for cancer cell PANoptosis and immunotherapy.

Science bulletin·2026
See all related articles

Related Experiment Video

Updated: Aug 11, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

9.1K

Experimental repetitive quantum channel simulation.

Ling Hu1, Xianghao Mu1, Weizhou Cai1

  • 1Center for Quantum Information, Institute for Interdisciplinary Information Sciences, Tsinghua University, Beijing 100084, China.

Science Bulletin
|February 8, 2023
PubMed
Summary
This summary is machine-generated.

Researchers demonstrate the first experimental simulation of arbitrary quantum channels for open quantum systems using a single photonic qubit. This breakthrough enables precise control over quantum noise and decoherence in practical quantum technologies.

Keywords:
Adaptive quantum controlOpen quantum systemQuantum channel simulationSuperconducting quantum computation

More Related Videos

Large Scale Energy Efficient Sensor Network Routing Using a Quantum Processor Unit
05:30

Large Scale Energy Efficient Sensor Network Routing Using a Quantum Processor Unit

Published on: September 8, 2023

628
Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

14.6K

Related Experiment Videos

Last Updated: Aug 11, 2025

Generation and Coherent Control of Pulsed Quantum Frequency Combs
06:42

Generation and Coherent Control of Pulsed Quantum Frequency Combs

Published on: June 8, 2018

9.1K
Large Scale Energy Efficient Sensor Network Routing Using a Quantum Processor Unit
05:30

Large Scale Energy Efficient Sensor Network Routing Using a Quantum Processor Unit

Published on: September 8, 2023

628
Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators
09:23

Quantum State Engineering of Light with Continuous-wave Optical Parametric Oscillators

Published on: May 30, 2014

14.6K

Area of Science:

  • Quantum Information Science
  • Quantum Computing
  • Quantum Optics

Background:

  • Universal control of quantum systems is crucial for quantum information processing.
  • Practical quantum systems are open and influenced by environmental coupling, described by quantum channels.
  • Existing studies often focus on ideally isolated systems.

Purpose of the Study:

  • To experimentally simulate arbitrary quantum channels for an open quantum system.
  • To achieve full control over practical open quantum systems.
  • To provide a testbed for understanding quantum noise and decoherence.

Main Methods:

  • Experimental simulation of arbitrary quantum channels using a single photonic qubit in a superconducting quantum circuit.
  • Utilizing one ancilla qubit and measurement-based adaptive control.
  • Repetitively implementing quantum channel simulation.

Main Results:

  • Successfully simulated arbitrary quantum channels for an open quantum system.
  • Realized an arbitrary Liouvillian for continuous evolution of an open quantum system for the first time.
  • Demonstrated a method with minimal resources (one ancilla qubit).

Conclusions:

  • The experiment provides a powerful tool for full control of practical open quantum systems.
  • Offers a valuable testbed for investigating quantum noise and decoherence.
  • Advances the goal of universal control in quantum information processing.