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Related Concept Videos

Standing Waves in a Cavity01:28

Standing Waves in a Cavity

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:
IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration01:16

IR Spectroscopy: Hooke's Law Approximation of Molecular Vibration

A covalently bonded heteronuclear diatomic molecule can be modeled as two vibrating masses connected by a spring. The vibrational frequency of the bond can be expressed using an equation derived from Hooke's law, which describes how the force applied to stretch or compress a spring is proportional to the displacement of the spring. In this case, the atoms behave like masses, and the bond acts like a spring.
According to Hooke's law, the vibrational frequency is directly proportional to the...
Flexural Stress01:16

Flexural Stress

When analyzing bending in symmetric members, it's crucial to understand how stresses distribute when subjected to bending moments. This stress distribution is effectively described by applying fundamental mechanics and material science principles, particularly Hooke's Law for elastic materials.
Hooke's Law states that within the material's elastic limits, stress is directly proportional to strain. In a member experiencing a bending moment, the strain at any point is relative to its distance...
Electric Field at the Surface of a Conductor01:26

Electric Field at the Surface of a Conductor

Consider a conductor in electrostatic equilibrium. The net electric field inside a conductor vanishes, and extra charges on the conductor reside on its outer surface, regardless of where they originate.
In the 19th century, Michael Faraday conducted the famous ice pail experiment to prove that the charges always reside on the surface of a conductor. The experimental set-up consists of a conducting uncharged container mounted on an insulating stand. The outer surface of the container is...
Modes of Standing Waves: II01:04

Modes of Standing Waves: II

The starting point for expressing the modes of standing waves is understanding the boundary conditions that the waves must follow. The boundary conditions are derived from the physical understanding of how the standing waves are sustained, that is, how the vibrating particles of the medium behave at the boundaries imposed on them.
For a tube open at one end and closed at the other filled with air, the modes are such that there is always an antinode at the open end and a node at the closed end.
Unsymmetric Bending01:18

Unsymmetric Bending

Unsymmetrical bending occurs when the bending moment applied to a structural member does not align with its principal axis. This misalignment leads to complex stress distributions and deflection patterns that differ from those in symmetrical bending, and are essential for designing structures to withstand different loading conditions. In unsymmetrical bending, the neutral axis—where stress is zero—does not necessarily align with the geometric axes of the cross-section. The orientation of the...

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Fabrication of Three-Dimensional Graphene-Based Polyhedrons via Origami-Like Self-Folding
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Flexural phonons in free-standing graphene.

Eros Mariani1, Felix von Oppen

  • 1Institut für Theoretische Physik, Freie Universität Berlin, Arnimallee 14, 14195 Berlin, Germany.

Physical Review Letters
|March 21, 2008
PubMed
Summary

Flexural phonons in graphene membranes exhibit quadratic dispersion, leading to an anomalous T(5/2)lnT resistivity dependence below a crossover temperature. This behavior arises from coupled bending and stretching in the membrane.

Area of Science:

  • Condensed Matter Physics
  • Materials Science
  • Nanotechnology

Background:

  • Freestanding graphene membranes possess unique phononic properties due to their 2D structure.
  • Understanding phonon behavior is crucial for predicting electronic properties like electrical resistivity.
  • Symmetries in graphene dictate the nature of phonon dispersion relations.

Purpose of the Study:

  • To investigate the role of out-of-plane (flexural) phonons in the electrical resistivity of graphene membranes.
  • To determine the temperature dependence of resistivity arising from flexural phonon interactions.
  • To elucidate the microscopic origins of anomalous temperature dependencies in graphene's electrical transport.

Main Methods:

  • Theoretical analysis of flexural phonon dispersion relations in freestanding graphene membranes, considering rotation and reflection symmetries.

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  • Calculation of the phonon contribution to electrical resistivity (rho) by analyzing phonon-charge carrier interactions.
  • Investigation of the coupling between bending and stretching degrees of freedom and its effect on phonon renormalization.
  • Main Results:

    • Flexural phonons exhibit quadratic dispersion at long wavelengths, consistent with symmetry constraints.
    • Charge carriers excite flexural phonons in pairs, influencing their contribution to resistivity.
    • An anomalous temperature dependence, rho proportional to T(5/2)lnT, is observed below a crossover temperature T(x).
    • The logarithmic factor in resistivity arises from the renormalization of flexural phonon dispersion due to coupled in-plane and out-of-plane motions.

    Conclusions:

    • Flexural phonons are the dominant contributors to resistivity in graphene membranes below T(x).
    • The observed anomalous temperature dependence provides insight into electron-phonon coupling mechanisms in 2D materials.
    • The coupling between bending and stretching modes significantly modifies phonon properties and electron transport in graphene.