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

Magnetic Vector Potential01:15

Magnetic Vector Potential

747
In electrostatics, the electric field can be written as the negative gradient of the potential. In magnetostatics, the zero divergence of the magnetic field ensures that the magnetic field can be expressed as the curl of a vector potential. This potential is known as the magnetic vector potential.
Consider an ideal solenoid with n turns per unit length and radius R. If I is the current through the solenoid, the magnetic field inside the solenoid is expressed as the product of vacuum...
747
Magnetostatic Boundary Conditions01:28

Magnetostatic Boundary Conditions

1.1K
An electric field suffers a discontinuity at a surface charge. Similarly, a magnetic field is discontinuous at a surface current. The perpendicular component of a magnetic field is continuous across the interface of two magnetic mediums. In contrast, its parallel component, perpendicular to the current, is discontinuous by the amount equal to the product of the vacuum permeability and the surface current. Like the scalar potential in electrostatics, the vector potential is also continuous...
1.1K
Magnetic Field due to Moving Charges01:23

Magnetic Field due to Moving Charges

9.1K
A stationary charge creates and interacts with the electric field, while a moving charge creates a magnetic field.
Consider a point charge moving with a constant velocity. Like the electric field, the magnetic field at any point is directly proportional to the magnitude of the charge and inversely proportional to the square of the distance between the source point and the field point. However, unlike the electric field, the magnetic field is always perpendicular to the plane containing the line...
9.1K
First Law: Particles in Two-dimensional Equilibrium01:18

First Law: Particles in Two-dimensional Equilibrium

5.2K
Recall that a particle in equilibrium is one for which the external forces are balanced. Static equilibrium involves objects at rest, and dynamic equilibrium involves objects in motion without acceleration; but it is important to remember that these conditions are relative. For instance, an object may be at rest when viewed from one frame of reference, but that same object would appear to be in motion when viewed by someone moving at a constant velocity.
Newton's first law tells us about...
5.2K
Electrostatic Boundary Conditions01:16

Electrostatic Boundary Conditions

565
Consider an external electric field propagating through a homogeneous medium. When the electric field crosses the surface boundary of the medium, it undergoes a discontinuity. The electric field can be resolved into normal and tangential components. The amount by which the field changes at any boundary is given by the difference between the field components above and below the surface boundary.
The surface integral of an electric field is given by Gauss's law in integral form and is related to...
565
First Law: Particles in One-dimensional Equilibrium01:10

First Law: Particles in One-dimensional Equilibrium

7.0K
Newton's first law of motion states that a body at rest remains at rest, or if in motion, remains in motion at constant velocity, unless acted on by a net external force. It also states that there must be a cause for any change in velocity (a change in either magnitude or direction) to occur. This cause is a net external force. For example, consider what happens to an object sliding along a rough horizontal surface. The object quickly grinds to a halt, due to the net force of friction. If...
7.0K

You might also read

Related Articles

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

Sort by
Same author

Primordial-Black-Hole-Based Pathways to Little Red Dots.

Physical review letters·2026
Same author

Scalar Fields around Black Hole Binaries in LIGO-Virgo-KAGRA.

Physical review letters·2026
Same author

Black Hole Quasinormal Mode Resonances.

Physical review letters·2025
Same author

Two-Step Procedure to Detect Cosmological Gravitational Wave Backgrounds with Next-Generation Terrestrial Gravitational-Wave Detectors.

Physical review letters·2025
Same author

Unstable Chords and Destructive Resonant Excitation of Black Hole Quasinormal Modes.

Physical review letters·2025
Same author

Generating synthetic computed tomography for radiotherapy: SynthRAD2023 challenge report.

Medical image analysis·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: Aug 24, 2025

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

9.7K

Ghost Instabilities in Self-Interacting Vector Fields: The Problem with Proca Fields.

Katy Clough1, Thomas Helfer2, Helvi Witek3

  • 1School of Mathematical Sciences, Queen Mary University of London Mile End Road, London E1 4NS, United Kingdom.

Physical Review Letters
|October 21, 2022
PubMed
Summary
This summary is machine-generated.

Self-interacting massive vector fields, described by a modified Proca equation, develop dangerous ghost instabilities. These instabilities grow on a Kerr background, challenging theories of vector dark matter and bosenovae.

More Related Videos

High-speed Particle Image Velocimetry Near Surfaces
11:59

High-speed Particle Image Velocimetry Near Surfaces

Published on: June 24, 2013

33.2K
Quantitative and Qualitative Examination of Particle-particle Interactions Using Colloidal Probe Nanoscopy
13:15

Quantitative and Qualitative Examination of Particle-particle Interactions Using Colloidal Probe Nanoscopy

Published on: July 18, 2014

11.1K

Related Experiment Videos

Last Updated: Aug 24, 2025

Magnetically Induced Rotating Rayleigh-Taylor Instability
06:42

Magnetically Induced Rotating Rayleigh-Taylor Instability

Published on: March 3, 2017

9.7K
High-speed Particle Image Velocimetry Near Surfaces
11:59

High-speed Particle Image Velocimetry Near Surfaces

Published on: June 24, 2013

33.2K
Quantitative and Qualitative Examination of Particle-particle Interactions Using Colloidal Probe Nanoscopy
13:15

Quantitative and Qualitative Examination of Particle-particle Interactions Using Colloidal Probe Nanoscopy

Published on: July 18, 2014

11.1K

Area of Science:

  • Particle Physics
  • Theoretical Physics
  • Cosmology

Background:

  • Massive vector fields are crucial in particle physics, mediating weak interactions, acting as dark matter candidates, and describing photons in plasma.
  • The Proca equation describes massive vector fields, but modifications for self-interactions are explored here.

Purpose of the Study:

  • To investigate the stability of massive vector fields with self-interactions by modifying the Proca equation.
  • To analyze the impact of self-interactions on vector field dynamics, particularly concerning instabilities.
  • To explore the implications for various physical phenomena, including dark matter and astrophysical events.

Main Methods:

  • Replacing the standard mass term in the Proca equation with a general self-interaction potential.
  • Analyzing the emergence of ghost instabilities in this modified theory.
  • Simulating the evolution of a self-interacting Proca field on a Kerr black hole background.

Main Results:

  • Self-interactions in massive vector fields inevitably introduce ghost instabilities, similar to those in modified gravity theories.
  • Nonperturbative dynamics do not prevent these instabilities; instead, superradiant instability on a Kerr background amplifies them.
  • Instabilities are triggered in finite time once self-interaction becomes significant, even if the system initially behaves like a massive field.

Conclusions:

  • The presence of ghost instabilities in self-interacting massive vector fields has significant implications for theoretical models.
  • These findings challenge the viability of certain vector dark matter models and the formation of spin-one bosenovae.
  • The study highlights the importance of considering field self-interactions and their stability in various physical contexts, from particle physics to astrophysics.