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Related Concept Videos

Potential Due to a Polarized Object01:29

Potential Due to a Polarized Object

A neutral atom consists of a positively charged nucleus surrounded by a negatively charged electron cloud. When placed in an external electric field, the external electric force pulls the electrons and nucleus apart, opposite to the intrinsic attraction between the nucleus and the electrons. The opposing forces balance each other with a slight shift between the center of masses of the nucleus and the electron cloud, resulting in a polarized atom. On the other hand, a few molecules, like water,...
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The electrical signals recorded on an electrocardiogram (ECG) occur before the mechanical processes of contraction and relaxation during the cardiac cycle.
A cardiac action potential originates in the SA node and spreads throughout the atria and the AV node in approximately 0.03 seconds. This results in the P wave in an ECG and triggers atrial contraction. The action potential is then briefly slowed at the AV node, allowing the atria to contract and fill the ventricles with blood before...
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Cardiac action potentials are essential for proper heart function, enabling the rhythmic contractions needed for adequate blood circulation. Nodal cells and Purkinje fibers, specialized for electrical conduction, generate these action potentials.
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Standing Electromagnetic Waves01:15

Standing Electromagnetic Waves

Electromagnetic waves can be reflected; the surface of a conductor or a dielectric can act as a reflector. As electric and magnetic fields obey the superposition principle, so do electromagnetic waves. The superposition of an incident wave and a reflected electromagnetic wave produces a standing wave analogous to the standing waves created on a stretched string.
Suppose a sheet of a perfect conductor is placed in the yz-plane, and a linearly polarized electromagnetic wave traveling in the...
Dielectric Polarization in a Capacitor01:31

Dielectric Polarization in a Capacitor

The presence of a dielectric medium in a capacitor not only changes the voltage and capacitance but also affects the electric field. In general, dielectrics can be of two types: polar and nonpolar. In a polar dielectric, the positive and negative charges in the molecules are separated by a distance and hence have a permanent dipole moment. In contrast, no such charge separation exists in a nonpolar dielectric, however the nonpolar molecules get polarized in the presence of an external electric...
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Electrocardiogram Fundamentals

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A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference
07:56

A Photonic System for Generating Unconditional Polarization-Entangled Photons Based on Multiple Quantum Interference

Published on: September 5, 2019

p-Wave polaron.

Jesper Levinsen1, Pietro Massignan, Frédéric Chevy

  • 1T.C.M. Group, Cavendish Laboratory, Cambridge, United Kingdom. jfl36@cam.ac.uk

Physical Review Letters
|September 26, 2012
PubMed
Summary
This summary is machine-generated.

We studied a single impurity in a Fermi sea near a p-wave Feshbach resonance. A magnetic field induced anisotropic impurity dispersion and a third polaron branch, offering tunable effective masses.

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Area of Science:

  • Quantum physics
  • Ultracold atomic gases

Background:

  • Interactions between atoms and impurities are crucial in quantum systems.
  • Feshbach resonances allow tuning of these interactions.
  • Polarons describe quasiparticles formed by an impurity interacting with a quantum medium.

Purpose of the Study:

  • Investigate the behavior of a single impurity in a Fermi sea near a p-wave Feshbach resonance.
  • Analyze the impurity's dispersion and spectral response under magnetic field influence.
  • Explore novel phenomena arising from dipolar interactions and magnetic fields.

Main Methods:

  • Theoretical calculation of impurity dispersion and spectral response.
  • Analysis of a single impurity in a Fermi sea.
  • Consideration of interspecies p-wave Feshbach resonance and magnetic fields.

Main Results:

  • Observed a third polaron branch in the excitation spectrum, beyond attractive and repulsive polarons.
  • Discovered anisotropic impurity dispersion with distinct effective masses parallel and perpendicular to the magnetic field.
  • Demonstrated tunability of anisotropy and effective masses by magnetic field strength.

Conclusions:

  • Dipolar interactions in a magnetic field lead to unique polaron properties.
  • Anisotropic effective masses can be tuned and even exhibit opposite signs or be smaller than the bare mass.
  • This system provides a novel platform for exploring quantum many-body physics and polaron physics.