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

Propagation of Waves01:07

Propagation of Waves

3.4K
When a wave propagates from one medium to another, part of it may get reflected in the first medium, and part of it may get transmitted to the second medium. In such a case, the interface of the two mediums can be considered as a boundary that is neither fixed nor free.
Consider a scenario where a wave propagates from a string of low linear mass density to a string of high linear mass density. In such a case, the reflected wave is out of phase with respect to the incident wave, however the...
3.4K
Generating Electromagnetic Radiations01:10

Generating Electromagnetic Radiations

8.4K
The German physicist Heinrich Hertz (1857–1894) was the first to generate and detect certain types of electromagnetic waves in the laboratory. Starting in 1887, he performed a series of experiments that confirmed the existence of electromagnetic waves and verified that they travel at the speed of light. Hertz used an alternating-current RLC (resistor-inductor-capacitor) circuit that resonated at a known frequency and connected it to a loop of wire. High voltages induced across the gap in...
8.4K
Standing Waves in a Cavity01:28

Standing Waves in a Cavity

1.6K
A household microwave and lasers are examples of standing electromagnetic waves in a cavity. When two conducting metal plates are placed parallel at the nodal planes, it creates a cavity where standing waves are formed. The cavity between the two planes is analogous to a stretched string held at the points x = 0 and x = L. Here, the distance 'L' between the two planes must be an integer multiple of half of the wavelength. The wavelengths that satisfy this condition are given by:
1.6K

You might also read

Related Articles

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

Sort by
Same author

Quantum Critical Dynamics Induced by Topological Zero Modes.

Physical review letters·2026
Same author

Gate-Tunable Orbital Magnetism and Competing Superconductivity in Twisted Trilayer Graphene Josephson Junctions.

ACS applied materials & interfaces·2025
Same author

Effects of Landau Level Mixing on Various Fractional Quantum Hall States in Trilayer Graphene.

Physical review letters·2025
Same author

A sensitive MOKE and optical Hall effect technique at visible wavelengths: insights into the Gilbert damping.

Nature communications·2025
Same author

Revealing quantum geometry in nonlinear quantum materials.

Reports on progress in physics. Physical Society (Great Britain)·2025
Same author

Universality of quantum phase transitions in the integer and fractional quantum Hall regimes.

Nature communications·2024
Same journal

Erratum: Bacterial Turbulence at Compressible Fluid Interfaces [Phys. Rev. Lett. 136, 138301 (2026)].

Physical review letters·2026
Same journal

Unveiling Light-Quark Yukawa Flavor Structure via Dihadron Fragmentation at Lepton Colliders.

Physical review letters·2026
Same journal

Adaptable Route to Fast Coherent State Transport via Bang-Bang-Bang Protocols.

Physical review letters·2026
Same journal

Topological Transition and Emergence of Elasticity of Dislocation in Skyrmion Lattice: Beyond Kittel's Magnetic-Polar Analogy.

Physical review letters·2026
Same journal

Pound-Drever-Hall Method for Superconducting-Qubit Readout.

Physical review letters·2026
Same journal

Coupling a ^{73}Ge Nuclear Spin to an Electrostatically Defined Quantum Dot in Silicon.

Physical review letters·2026
See all related articles

Related Experiment Video

Updated: Mar 29, 2026

Fabrication of Surface Acoustic Wave Devices on Lithium Niobate
07:55

Fabrication of Surface Acoustic Wave Devices on Lithium Niobate

Published on: June 18, 2020

13.3K

Miniband Generation by Surface Acoustic Waves.

Eli Meril1, Unmesh Ghorai1, Tobias Holder1

  • 1Tel Aviv University, School of Physics and Astronomy, Tel Aviv 69978, Israel.

Physical Review Letters
|March 27, 2026
PubMed
Summary
This summary is machine-generated.

Researchers developed a new tunable periodic structure using surface acoustic waves. This acoustoelectric superlattice allows in-situ control over 2D material band structures, creating flat bands and unique topological properties.

More Related Videos

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations
06:51

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations

Published on: August 21, 2018

7.5K
Fabrication of Nanoheight Channels Incorporating Surface Acoustic Wave Actuation via Lithium Niobate for Acoustic Nanofluidics
07:23

Fabrication of Nanoheight Channels Incorporating Surface Acoustic Wave Actuation via Lithium Niobate for Acoustic Nanofluidics

Published on: February 5, 2020

6.3K

Related Experiment Videos

Last Updated: Mar 29, 2026

Fabrication of Surface Acoustic Wave Devices on Lithium Niobate
07:55

Fabrication of Surface Acoustic Wave Devices on Lithium Niobate

Published on: June 18, 2020

13.3K
Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations
06:51

Microparticle Manipulation by Standing Surface Acoustic Waves with Dual-frequency Excitations

Published on: August 21, 2018

7.5K
Fabrication of Nanoheight Channels Incorporating Surface Acoustic Wave Actuation via Lithium Niobate for Acoustic Nanofluidics
07:23

Fabrication of Nanoheight Channels Incorporating Surface Acoustic Wave Actuation via Lithium Niobate for Acoustic Nanofluidics

Published on: February 5, 2020

6.3K

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Acoustics

Background:

  • Periodic structures in 2D materials, such as moiré and optical lattices, are crucial for tuning electronic properties.
  • Existing methods for creating superlattices have limitations in tunability and amplitude control.
  • Surface acoustic waves (SAWs) offer a potential mechanism for dynamic control of material properties.

Purpose of the Study:

  • To introduce a novel class of tunable periodic structures using acoustoelectric effects.
  • To demonstrate the ability to control the periodicity and amplitude of the superlattice potential.
  • To explore the generation of narrow, topologically nontrivial energy bands in 2D materials.

Main Methods:

  • Launching two obliquely propagating surface acoustic waves on a piezoelectric substrate supporting a 2D material.
  • Utilizing the acoustoelectric effect to create a superlattice potential.
  • Employing monolayer graphene as a model system to demonstrate tunability via SAW frequency and power.

Main Results:

  • A widely tunable acoustoelectric superlattice was successfully created, with periodicity tunable between moiré and optical lattice scales.
  • The amplitude of the acoustoelectric potential was externally controlled by adjusting SAW power, unlike fixed amplitudes in moiré systems.
  • In-situ control over the band structure of graphene was achieved, leading to the formation of flat bands and nontrivial valley Chern numbers with localized Berry curvature.

Conclusions:

  • The developed acoustoelectric superlattice provides a powerful new platform for engineering the electronic properties of 2D materials.
  • External tunability of periodicity and amplitude offers unprecedented control over band structure, enabling the exploration of novel quantum phenomena.
  • This technique holds promise for creating designer electronic states and topological devices based on 2D materials.