substance

ultralight dark matter

Hypothetical dark matter particles with extremely low mass, such as axions.
38 related articles · 3 formulas

Description

Ultralight dark matter refers to hypothetical particles with masses far smaller than the electron, often around 10^-22 eV, such as axions. Unlike heavy dark matter candidates like WIMPs, these particles behave more like waves than particles due to their enormous de Broglie wavelength, which can be as large as a galaxy. This wave-like behavior could leave distinct imprints on cosmic structures, such as suppressing small-scale clumping or creating solitonic cores in dark matter halos.

History

The axion was first proposed in 1977 by Roberto Peccei and Helen Quinn to solve the strong CP problem in quantum chromodynamics, and later recognized as a dark matter candidate. The ultralight scalar field dark matter idea gained traction in the 2000s with models like fuzzy dark matter.

How it works

Because of their tiny mass, ultralight dark matter particles are produced in huge numbers and form a coherent quantum state, like a Bose-Einstein condensate. Their wave interference can create patterns of density fluctuations, and they can form stable, oscillating configurations called solitons. Detection strategies often rely on their coupling to photons or other particles, using resonant cavities or atomic magnetometers to pick up faint signals from axion-photon conversion.

In practice

Ultralight dark matter searches drive the development of ultra-sensitive detectors, such as the Axion Dark Matter Experiment (ADMX), which uses a tunable microwave cavity to detect axion signals.

Fun fact

If dark matter is made of ultralight particles, a single 'particle' could have a wavelength spanning thousands of kilometers, making it behave more like a wave than a bullet.

Concept graph →

Formulas

$$v_{\mathrm{min}} = \frac{1}{\sqrt{2 m_N E_R}} \left( \frac{E_R m_N}{\mu} + \delta \right)$$
Minimum DM speed to excite nuclear recoil.
What is in the formula
v_minvariableMinimum dark matter speed — velocity metre per second
m_NvariableMass of the target nucleus — mass kilogram
E_RvariableRecoil energy of the nucleus — energy joule
μvariableReduced mass of the dark matter-nucleus system — reduced mass kilogram
δvariableMass splitting between dark matter states (energy gap) — energy joule
v_{χ}^{({min})}\approx\frac{1}{\sqrt{2m_ne_r}}(\frac{e_rm_n}{μ_{χn}}+δ) · 2606.30724
$$m_{\text{crit}} \sim \frac{3 k_B T}{v^2}$$
Dark matter particles above this mass heat stars; below it, they cool.
What is in the formula
m_critvariablecritical dark matter mass — mass kilogram
k_BvariableBoltzmann constant — boltzmann constant joule per kelvin
Tvariabletemperature — temperature kelvin
vvariablevelocity — velocity metre per second
m_{{crit}}\sim\frac{3k_bt}{v_*^2} · 2607.00840
m_{\rmcrit}\approx\frac{3k_bt}{v_{\star}^2} · 2607.00840v2
$$\lambda_{\mathrm{Edd}} = \frac{L_{\mathrm{bol}}}{L_{\mathrm{Edd}}}}$$
Ratio of bolometric luminosity to Eddington luminosity limit.
What is in the formula
\lambda_{\mathrm{EddvariableEddington luminosity ratio — eddington luminosity ratio
L_{\mathrm{bol}}variableBolometric luminosity — luminosity watt
L_{\mathrm{Edd}}variableEddington luminosity — luminosity watt
λ_{{edd}}=\frac{l_{{bol}}}{l_{{edd}}} · 2607.05246v1

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