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

Maxwell-Boltzmann Distribution: Problem Solving01:20

Maxwell-Boltzmann Distribution: Problem Solving

1.6K
Individual molecules in a gas move in random directions, but a gas containing numerous molecules has a predictable distribution of molecular speeds, which is known as the Maxwell-Boltzmann distribution, f(v).
This distribution function f(v) is defined by saying that the expected number N (v1,v2) of particles with speeds between v1 and v2 is given by
1.6K
Propagation of Uncertainty from Random Error00:59

Propagation of Uncertainty from Random Error

732
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...
732
Probability Distributions01:32

Probability Distributions

7.3K
 The probability of a random variable x  is the likelihood of its occurrence. A probability distribution represents the probabilities of a random variable using a formula, graph, or table. There are two types of probability distribution– discrete probability distribution and continuous probability distribution.
A discrete probability distribution is a probability distribution of discrete random variables. It can be categorized into binomial probability distribution and Poisson...
7.3K
Propagation of Uncertainty from Systematic Error01:10

Propagation of Uncertainty from Systematic Error

557
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...
557
The Quantum-Mechanical Model of an Atom02:45

The Quantum-Mechanical Model of an Atom

42.5K
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.
42.5K
The Pauli Exclusion Principle03:06

The Pauli Exclusion Principle

40.0K
The arrangement of electrons in the orbitals of an atom is called its electron configuration. We describe an electron configuration with a symbol that contains three pieces of information:
40.0K

You might also read

Related Articles

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

Sort by
Same author

Double-Bracket Quantum Algorithms for Quantum Imaginary-Time Evolution.

Physical review letters·2026
Same author

Classically Estimating Observables of Noiseless Quantum Circuits.

Physical review letters·2025
Same author

Quantum learning advantage on a scalable photonic platform.

Science (New York, N.Y.)·2025
Same author

Does provable absence of barren plateaus imply classical simulability?

Nature communications·2025
Same author

Quantum Simulation of Molecular Dynamics Processes─A Benchmark Study Using a Classical Simulator and Present-Day Quantum Hardware.

The journal of physical chemistry. A·2025
Same author

Random unitaries in extremely low depth.

Science (New York, N.Y.)·2025
Same journal

Demonstration of a quantum C-NOT gate in a time-multiplexed fully reconfigurable photonic processor.

Nature communications·2026
Same journal

Nonlinear quantum light source with van der Waals ferroelectric NbOX<sub>2</sub> (X = Br, I).

Nature communications·2026
Same journal

Antagonistic histone H2A variants and autonomous heterochromatin formation shape epigenomic patterns in Arabidopsis.

Nature communications·2026
Same journal

The long tail of nitrate pollution in groundwater challenges governance of global water quality.

Nature communications·2026
Same journal

Select microbial metabolites promote tau aggregation in a murine tauopathy model.

Nature communications·2026
Same journal

Warming climate has lengthened global intense tropical cyclone seasons.

Nature communications·2026
See all related articles

Related Experiment Video

Updated: Jul 24, 2025

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

607

Out-of-distribution generalization for learning quantum dynamics.

Matthias C Caro1,2,3,4, Hsin-Yuan Huang5,6, Nicholas Ezzell7,8

  • 1Department of Mathematics, Technical University of Munich, Garching, Germany. matthias.caro@fu-berlin.de.

Nature Communications
|July 5, 2023
PubMed
Summary
This summary is machine-generated.

Quantum machine learning (QML) models can now generalize beyond their training data distribution. This study proves out-of-distribution generalization for learning unknown unitaries, even when training on simple product states.

More Related Videos

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
Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

12.9K

Related Experiment Videos

Last Updated: Jul 24, 2025

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

607
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
Gradient Echo Quantum Memory in Warm Atomic Vapor
10:00

Gradient Echo Quantum Memory in Warm Atomic Vapor

Published on: November 11, 2013

12.9K

Area of Science:

  • Quantum Machine Learning
  • Quantum Computing Theory
  • Generalization Bounds

Background:

  • Generalization bounds are crucial for understanding data needs in Quantum Machine Learning (QML).
  • Existing QML research guarantees in-distribution generalization for quantum neural networks (QNNs).
  • Out-of-distribution (OOD) generalization in QML remains an open challenge, limiting model applicability to unseen data distributions.

Purpose of the Study:

  • To establish theoretical guarantees for out-of-distribution generalization in Quantum Machine Learning.
  • To demonstrate the ability to learn unknown quantum unitaries from data generated from different distributions.
  • To explore the implications for near-term quantum hardware and quantum circuit compilation.

Main Methods:

  • Theoretical analysis of generalization bounds for quantum models.
  • Proving out-of-distribution generalization for the specific task of learning an unknown unitary.
  • Utilizing product states for training and evaluating generalization on entangled states.

Main Results:

  • The study proves out-of-distribution generalization for learning an unknown unitary in QML.
  • It is demonstrated that a quantum model trained on product states can learn the action of a unitary on entangled states.
  • This theoretical advancement is achieved without requiring training data from the target distribution.

Conclusions:

  • This work bridges the gap in understanding OOD generalization for QML.
  • The findings suggest that learning quantum dynamics is feasible on near-term quantum hardware using simpler training states.
  • The results offer new avenues for classical and quantum circuit compilation strategies.