phenomenon

wormhole resonance

Wormhole resonance refers to gravitational wave signatures from hypothetical traversable wormholes.
70 related articles · 2 formulas

Description

Wormhole resonance refers to the characteristic gravitational wave signals that would be emitted by a traversable wormhole, as opposed to a black hole. When a compact object like a neutron star falls into a wormhole, or when the wormhole itself is perturbed, it would ring at specific frequencies, similar to how a bell rings. However, the 'ringdown' of a wormhole would differ from that of a black hole due to the absence of an event horizon and the presence of a throat, which can cause echoes in the gravitational wave signal. These echoes are a key observational signature that could distinguish a wormhole from a black hole.

History

The idea of using gravitational wave echoes to test wormholes was proposed in the 2010s, following the first detections of gravitational waves by LIGO. Theoretical work by Cardoso, Pani, and others showed that exotic compact objects, including wormholes, would produce echoes in the ringdown signal. The concept gained attention as a way to probe quantum gravity effects near the horizon.

How it works

In general relativity, a wormhole's throat acts as a reflective boundary for gravitational waves. When a perturbation hits the throat, part of the wave is transmitted and part is reflected, creating a series of echoes with decreasing amplitude. The time delay between echoes depends on the wormhole's geometry, specifically the length of its throat. The resonance frequencies are determined by the wormhole's mass and spin, and can be computed using perturbation theory. Detecting these echoes in gravitational wave data would provide strong evidence for the existence of wormholes.

In practice

Wormhole resonance is a target for current and future gravitational wave detectors, including LIGO, Virgo, and LISA. Analyzing the ringdown of binary mergers for echoes could reveal the existence of wormholes or other exotic compact objects, providing a test of general relativity and quantum gravity.

Fun fact

If wormholes exist, they would be 'black hole mimickers'—their gravitational wave signal would look almost identical to a black hole for the first few milliseconds, but then differ by a series of repeating echoes, like a cosmic 'tail' that gives them away.

Concept graph →

Formulas

$$ds^2 = -e^{2\Phi(r)} dt^2 + \left(1 - \frac{b(r)}{r}\right)^{-1} dr^2 + r^2 d\Omega^2$$
A static wormhole metric with shape function b(r) and redshift function Φ(r).
What is in the formula
ds^2variableSpacetime interval squared — spacetime interval metre squared
\Phi(r)variableRedshift function — redshift function
b(r)variableShape function — shape function metre
rvariableRadial coordinate — radial coordinate metre
tvariableTime coordinate — time coordinate second
d\Omega^2variableSolid angle element squared — solid angle element
doperatorExterior derivative — differential operator
ds^2=-(1-\frac{2m}{\sqrt{r^2+\ell^2}})dt^2+(1-\frac{2m}{\sqrt{r^2+\ell^2}})^{-1}dr^2+r^2dω^2 · 2605.04631v1
$$\frac{d^2 r}{dz^2} = \frac{b - r b'}{2b^2} > 0$$
Geometric condition for wormhole throat existence violating null energy condition.
What is in the formula
rvariableradial coordinate of the throat — radial coordinate metre
zvariableproper distance along the throat — proper distance metre
bvariableshape function of the wormhole — shape function metre
d/dzoperatorderivative with respect to proper distance — ordinary derivative
d/droperatorderivative with respect to radial coordinate — ordinary derivative
\frac{d^2r}{dz^2}=\frac{b-rb'}{2b^2}>0 · 2605.14027v1

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