concept

dark matter properties

Theoretical and experimental studies of dark matter's composition, annihilation, and interactions with matter.
12 related articles · 3 formulas

Description

Dark matter is the invisible substance that makes up about 27% of the universe's mass-energy content. Unlike ordinary matter, it does not emit, absorb, or reflect light, making it detectable only through its gravitational effects. The study of dark matter's properties focuses on what it is made of, how it interacts with itself and with normal matter, and how it behaves under extreme conditions.

History

The concept of dark matter was first proposed by Fritz Zwicky in 1933, who noticed that galaxies in the Coma cluster were moving too fast to be held together by visible matter alone. Later, Vera Rubin's observations of galaxy rotation curves in the 1970s provided strong evidence for its existence.

How it works

Scientists investigate dark matter through several complementary approaches. Particle physics experiments search for weakly interacting massive particles (WIMPs) that might collide with atomic nuclei in detectors. Astrophysical observations look for signs of dark matter annihilation, where two dark matter particles could produce gamma rays or other particles. Gravitational lensing and galaxy rotation curves provide indirect measurements of dark matter's distribution and density.

In practice

Understanding dark matter properties is crucial for interpreting cosmological observations and for designing experiments to detect it directly, such as those in underground laboratories or space-based detectors.

Fun fact

Dark matter is so diffuse in our solar system that the total amount passing through Earth each year is estimated to be less than a kilogram.

Concept graph →

Formulas

$$\lambda_{\mathrm{FS}} \propto m_{\mathrm{hm}}^{-1/3}$$
Length scale for particle free streaming in dark matter.
What is in the formula
lambda_FSvariablefree streaming length — free streaming length metre
m_hmvariablehalf-mode mass of dark matter — half mode mass kilogram
proptooperatoris proportional to — proportionality
λ_{{fs}}=5.2(\frac{m_{{hm}}}{10^7m_\odot})^{1/3}{кпк} · 2606.05277v1
$$\Omega_{\text{DM}} h^2 \propto \frac{\sqrt{\Gamma M_P}}{m_{\phi}^2}$$
Relic abundance from inflaton decay and mass.
What is in the formula
\Omega_{\text{DM}} hvariableDark matter relic density parameter times squared Hubble constant — density parameter
\GammavariableInflaton decay rate — decay rate per second
M_PvariableReduced Planck mass — mass kilogram
m_{\phi}variableMass of the dark matter particle (or inflaton) — mass kilogram
\proptooperatorIndicates direct proportionality — proportionality
\sqrt{}operatorTakes the square root of the argument — square root
y_0\simeq\frac{9\sqrt{π}b}{2}(\frac{5}{2})^{1/4}\frac{g_*^{3/4}}{g_{*s}}\frac{\sqrt{m_p\gamma_φ}}{m_φ^2} · 2607.23200v1
$$v_{\mathrm{min}} = \frac{1}{\sqrt{2 m_N E_R}} \left( \frac{E_R m_N}{\mu} + \delta \right)$$
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

Related articles · 12

A Crystal Trap for Light Dark Matter
No one has ever seen dark matter, but it should pass through detectors like wind through leaves. Sometimes, very rarely, a dark matter particle bumps into an atomic nucleus, and then the detector must catch that jolt. The trouble is that light dark matter particles can hardly move heavy nuclei: it's like trying to knock down a bowling pin by throwing a feather at it.
High Energy2026-08-072 minarXiv:2608.07234express
Hunting the Invisible at the Heart of the Milky Way
Imagine a huge stadium packed with people dressed in black. You're standing outside, trying to figure out what's happening inside, even though you can't see a single person. But if two people bump into each other and exchange bright T-shirts, you'd spot a flash of color.
Cosmology2026-08-052 minarXiv:2608.04763express
Dark Matter Isn't Quite the Invisible Wallflower
The cosmological standard model is like a recipe for a cake where everything is strictly measured: dark matter is like flour without a single lump (zero pressure), and dark energy is like the perfect leavening agent (equation of state exactly minus one). But what if the flour is a bit damp and the leavening agent has lost its oomph?
HEP Phenomenology2026-06-292 minarXiv:2606.29710express
Dark Matter Gains Strength When Crowded
When two dark matter particles approach each other, they can attract more strongly than expected. This phenomenon is called Sommerfeld enhancement — it works like an invisible spring that compresses before impact. For a long time, it was believed that the spring compresses more strongly the slower the particles approach each other.
HEP Phenomenology2026-06-121 minarXiv:2606.14845express
Dark Matter: When a Hit Leaves No Trace
A billiard ball slams into another. Impact, and the balls scatter. But if the push is not sharp but very gentle, the balls just roll together without bouncing. An atom behaves much the same way when hit by a dark matter particle.
General Relativity2026-04-172 minarXiv:2604.16628express
A Black Hole in a Cloud of Dark Matter
A black hole is not just a void but a massive object that warps the space around it. If it finds itself in a cloud of invisible dark matter, matter that emits no light but makes itself known through gravity, its behavior changes.
General Relativity2026-04-141 minarXiv:2604.12787express
Planet Nine Heats Up with Dark Matter
At the edge of the solar system, far beyond Neptune's orbit, something is knocking icy chunks off their paths. Their orbits are stretched and tilted in the same way, as if an invisible hand arranged them in a pattern.
High Energy2026-01-171 minarXiv:2602.00025express
Dark Matter Reshapes Black Hole Portraits
Although invisible, dark matter’s gravity governs the motion of stars and galaxies. It was first proposed by Fritz Zwicky in the 1930s, and later confirmed by Vera Rubin. Scientists have long suspected it accumulates around black holes, but direct proof was lacking.
HEP Phenomenology2026-01-121 minarXiv:2601.07921express
Dark Matter and Its Taste Preferences
The cosmos is filled with invisible dark matter, which betrays itself only through gravity. Its existence was suspected by Fritz Zwicky and confirmed by Vera Rubin.
Cosmology2026-01-051 minarXiv:2601.02466express
Mysterious Dark Object Challenges Theories
Supermassive bodies warp space, turning into a lens that bends light from distant objects. Such spacetime curvature allows astronomers to see the invisible. Recently, this method helped detect a hidden clump with the mass of a million Suns.
Cosmology2026-01-041 minarXiv:2601.01340express
Dark matter isn’t so cold after all
The enigma of dark matter was already studied by Fritz Zwicky and Vera Rubin. For decades, it was depicted as a cold, listless skeleton that only draws galaxies together.
Cosmology2025-10-081 minarXiv:2510.07382express
Invisible Object Weighing a Million Suns: Gravity Acts as a Magnifying Glass
Astronomers have found an invisible object in the Universe weighing just a million Suns — for cosmic scales, that’s a mere trifle, a hundred times lighter than anything they’ve been able to “weigh” at such distances. The object itself doesn’t shine, but it gave itself away by bending the light from an even more distant galaxy.