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

Speed of Sound in Solids and Liquids00:51

Speed of Sound in Solids and Liquids

3.1K
Most solids and liquids are incompressible—their densities remain constant throughout. In the presence of an external force, the molecules tend to restore to their original positions, which is only possible because the constituents interact. The interactions help the constituents pass on information about external disturbances, like sound waves. Therefore, sound waves travel faster through these media. Compared to solids, the constituents in a liquid are less tightly bound. Thus, sound...
3.1K
Deriving the Speed of Sound in a Liquid01:09

Deriving the Speed of Sound in a Liquid

588
As with waves on a string, the speed of sound or a mechanical wave in a fluid depends on the fluid's elastic modulus and inertia. The two relevant physical quantities are the bulk modulus and the density of the material. Indeed, it turns out that the relationship between speed and the bulk modulus and density in fluids is the same as that between the speed and the Young's modulus and density in solids.
The speed of sound in fluids can be derived by considering a mechanical wave...
588
Speed of Sound in Gases01:08

Speed of Sound in Gases

3.1K
The speed of sound in a gaseous medium depends on various factors. Since gases constitute molecules that are free to move, they are highly compressible. Hence, sound waves travel slowly through gases. Thermodynamics helps us understand the relationship between pressure, volume, and temperature of gases, thus, the speed of sound in an ideal gas can be determined using the laws of thermodynamics. At the same time, Newton's laws of motion and the continuity equation of fluid dynamics also come...
3.1K
Shock Waves01:16

Shock Waves

2.2K
While deriving the Doppler formula for the observed frequency of a sound wave, it is assumed that the speed of sound in the medium is greater than the source's speed through it. When this condition is breached, a shock wave occurs.
When the source's speed approaches the speed of sound, constructive interference between successive wavefronts emitted by the source occurs immediately behind it. Initially, scientists believed that this constructive interference would result in such high...
2.2K
Propagation Speed of Electromagnetic Waves01:30

Propagation Speed of Electromagnetic Waves

3.8K
Electromagnetic waves are consistent with Ampere's law. Assuming there is no conduction current Ampere's law is given as:
3.8K
Mechanisms of Heat Transfer II01:20

Mechanisms of Heat Transfer II

3.4K
In convection, thermal energy is carried by the large-scale flow of matter. Ocean currents and large-scale atmospheric circulation, which result from the buoyancy of warm air and water, transfer hot air from the tropics toward the poles and cold air from the poles toward the tropics. The Earth’s rotation interacts with those flows, causing the observed eastward flow of air in the temperate zones. Convection dominates heat transfer by air, and the amount of available space for the airflow...
3.4K

You might also read

Related Articles

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

Sort by
Same author

A quantum-coherent photon-emitter interface in the original telecom band.

Nature nanotechnology·2026
Same author

Electrostatic comb-drive actuators for nanoelectromechanical photonics: theory, design, fabrication, and characterization.

Nanotechnology·2026
Same author

Unraveling Structure-Strain-Defect Relationships in Thermopower Modulation of Epitaxial Double Perovskite Oxide.

ACS omega·2026
Same author

Rough Fabry-Perot cavity: a vastly multi-scale numerical problem.

Nanophotonics (Berlin, Germany)·2025
Same author

A self-assembled two-dimensional hypersonic phononic insulator.

Nanophotonics (Berlin, Germany)·2025
Same author

Far-Field Radiative Thermal Rectification Based on Asymmetric Emissivity.

ACS applied optical materials·2024
Same journal

Near-exceptional point degeneracy enables multilevel optical memory.

Nature nanotechnology·2026
Same journal

Monolithic manufacturing of an electrically addressable quasi-suspended nanophotonic aperture.

Nature nanotechnology·2026
Same journal

Halide-site-substituting spacer creates quasi-two-dimensional perovskites for vapour-deposited light-emitting diodes.

Nature nanotechnology·2026
Same journal

Nanoscale amorphization of poly(triarylamine) for efficient and stable inverted perovskite photovoltaics.

Nature nanotechnology·2026
Same journal

Bridging nanotechnology and mechanobiology.

Nature nanotechnology·2026
Same journal

Coherent 2D/3D van der Waals epitaxy enables single-crystal perovskite heterostructures.

Nature nanotechnology·2026
See all related articles

Related Experiment Video

Updated: Sep 2, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.6K

Engineering nanoscale hypersonic phonon transport.

O Florez1,2, G Arregui3, M Albrechtsen4

  • 1Catalan Institute of Nanoscience and Nanotechnology (ICN2), CSIC and BIST, Campus UAB, Barcelona, Spain. omar.florez@icn2.cat.

Nature Nanotechnology
|August 8, 2022
PubMed
Summary
This summary is machine-generated.

Researchers eliminated thermal vibrations in a silicon membrane at room temperature, creating a phononic stop band. This breakthrough enables precise phonon manipulation for quantum technologies and signal processing.

More Related Videos

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

5.9K
Characterization of Thermal Transport in One-dimensional Solid Materials
05:20

Characterization of Thermal Transport in One-dimensional Solid Materials

Published on: January 26, 2014

17.5K

Related Experiment Videos

Last Updated: Sep 2, 2025

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids
11:03

An Analog Macroscopic Technique for Studying Molecular Hydrodynamic Processes in Dense Gases and Liquids

Published on: December 4, 2017

8.6K
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

5.9K
Characterization of Thermal Transport in One-dimensional Solid Materials
05:20

Characterization of Thermal Transport in One-dimensional Solid Materials

Published on: January 26, 2014

17.5K

Area of Science:

  • Solid-state physics
  • Nanotechnology
  • Acoustics

Background:

  • Controlling vibrations in solids is key for tuning elastic properties and light interactions.
  • Thermal vibrations cause noise and dephasing in quantum processes.
  • Phononic stop bands eliminate specific elastic wave frequencies, suppressing vibrations.

Purpose of the Study:

  • To demonstrate the complete absence of thermal vibrations in a nanostructured silicon membrane.
  • To create and characterize a broad phononic bandgap at room temperature.
  • To explore the potential of this platform for phonon manipulation.

Main Methods:

  • Fabrication of a nanostructured silicon membrane with a shamrock crystal geometry.
  • Utilizing Brillouin light scattering spectroscopy to measure guided phonon modes.
  • Creating a line-defect waveguide to guide elastic waves.

Main Results:

  • Complete absence of thermal vibrations observed in the silicon membrane at room temperature.
  • A 5.3-GHz-wide phononic bandgap was achieved, centered at 8.4 GHz.
  • Gigahertz guided modes were directly measured in the waveguide without external excitation.

Conclusions:

  • The shamrock crystal geometry provides an effective platform for phonon control.
  • This research opens possibilities for applications in optomechanics and signal processing transduction.
  • Demonstrated absence of thermal vibrations advances solid-state quantum device development.