method

axion detection neutron stars

Axion detection from neutron stars involves observing electromagnetic signals from axion conversions in strong magnetic fields.
35 related articles · 4 formulas

Description

Axions are hypothetical elementary particles that could explain dark matter and solve a long-standing puzzle in particle physics known as the strong CP problem. They are predicted to interact extremely weakly with ordinary matter, making them notoriously difficult to detect. Neutron stars, however, offer a unique natural laboratory: their intense magnetic fields — the strongest known in the universe — can convert axions into detectable electromagnetic radiation, typically in the radio or X-ray band.

History

The axion was proposed in 1977 by Roberto Peccei and Helen Quinn to explain why the strong nuclear force preserves CP symmetry, with the particle itself named by Frank Wilczek and Steven Weinberg. The idea of using neutron stars for axion detection gained traction in the 2010s, with detailed predictions published by researchers such as Christopher Dessert and Benjamin Safdi.

How it works

In the presence of a strong magnetic field, an axion can convert into a photon (and vice versa) through a process called the Primakoff effect. Near a neutron star, axions produced in the star's core or in the surrounding magnetosphere would traverse the magnetic field, and a fraction would convert into photons. These photons would emerge with energies matching the axion mass, creating a narrow spectral line that telescopes can search for. The conversion probability depends on the field strength and the path length, which is why neutron stars — with fields up to 10^15 gauss — are prime targets.

In practice

Searches for axion-induced radio signals from neutron stars are ongoing using observatories like the Green Bank Telescope and the Effelsberg Telescope, aiming to detect dark matter axions or axions produced in stellar interiors.

Fun fact

If axions exist, they would be so light that a single cubic centimeter of dark matter axions would contain roughly 10^14 particles, yet their combined mass would be only about 10^-18 grams.

Concept graph →

Formulas

$$P_{a\to\gamma} \propto (g_{a\gamma\gamma} B L)^2$$
Probability of axion converting to photon scales with magnetic field and distance squared.
What is in the formula
P_{a\to\gamma}variableprobability of axion-photon conversion — probability
g_{a\gamma\gamma}variableaxion-photon coupling constant — coupling constant reciprocal gev
Bvariablemagnetic field strength — magnetic flux density tesla
Lvariablepath length through the magnetic field — length metre
\proptooperatorindicates proportionality, not equality — proportional to
p_{a\toγ}\approx\frac{(g_{aγγ}bl)^2}{4} · 2607.23140v1
$$g_{a\gamma} \sim \text{constant}$$
The axion-photon coupling constant sets the conversion probability.
What is in the formula
g_{a\gamma}variableAxion-photon coupling constant — coupling constant
\simoperatorIndicates the left side is of the order of the right side — approximate equality
g/m\sim10^{-22}{gev}^{-1} · 2510.27416
$$\nu \propto m_a$$
Axion-photon conversion frequency is proportional to axion mass.
What is in the formula
νvariableFrequency of the converted photon — frequency hertz
m_avariableAxion mass — mass kilogram
∝operatorIndicates that the left side scales linearly with the right side — proportionality
ν\simeq242{мгц}(\frac{m_a}{μ{эв}}) · 2606.04304v1
$$E_c \propto \frac{|m_a^2 - \omega_{\rm pl}^2|}{B_\perp g_{a\gamma}}$$
Critical energy where axion-photon oscillations become energy-independent.
What is in the formula
E_cvariableCritical energy — energy joule
m_avariableAxion mass — mass kilogram
ω_plvariablePlasma frequency — angular frequency radian per second
B_perpvariablePerpendicular magnetic field strength — magnetic field strength tesla
g_aγvariableAxion-photon coupling constant — coupling constant inverse gev
e_c\simeq2.5{гэв}(\frac{|m_a^2-ω_{\rmpl}^2|}{1{\rmнэв}})(\frac{b_\perp}{μ{г}})^{-1}(\frac{g_{aγ}}{10^{-11}{гэв}^{-1}})^{-1} · 2607.07158

Related articles · 35

The Invisible Conductor of a Pulsar: How an Axion Mane Makes a Dying Star Sing
The orchestra plays, though no one sees the conductor. The musicians are charged particles in the pulsar's magnetosphere, and the score is the electric and magnetic fields generated by the spinning superdense star.
Lensless Camera Counts Antiprotons by Annihilation Sparks
The antiproton beam hits the plate, and each impact bursts into a shower of charged particles. In the GBAR experiment at CERN, this picture is captured not by a sophisticated detector but by an ordinary industrial camera without a lens, pressed against the vacuum window from the outside.
HEP Phenomenology2026-08-162 minarXiv:2608.15699express
Hunting Solar Axions in Liquid Xenon
Inside the Sun, reactions can produce light, almost undetectable particles called axions. One such reaction yields axions with an energy of 5.49 MeV, as if each one carried the energy of a tennis ball moving at 100 km/h. These particles pass freely through Earth, but occasionally they might collide with a xenon atom.
Atomic Physics2026-08-051 minarXiv:2608.05067express
How to Catch an Invisible Electron
An extra electron in a molecule is like a passenger barely hanging onto the step of a departing train. Such a 'passenger' turns the particle into an anion — a negative ion. Studying it is tough: the bond is weak, the electron cloud is diffuse, and any jolt can knock the electron off.
HEP Phenomenology2026-08-052 minarXiv:2608.05279express
A Heavy Rock and a Sea of Particles
The early Universe resembles a boiling cauldron, where particles and antiparticles are born and die in equal numbers. But today, all around us is only matter — stars, planets, ourselves. How did a tiny excess of one part in a billion emerge from the initial equality? One answer hides in the oscillations of a heavy field, like a rock that the tide alternately submerges and exposes.
High Energy2026-08-032 minarXiv:2608.02269express
X-ray Beacons Spawn Ghost Particles
In the distant Cigar Galaxy, there is an unusual beacon. It doesn't shine in the usual sense: its rays are born in a scorching cloud around a black hole that is devouring matter from a companion star. Such objects are called ultraluminous X-ray sources. Their X-ray brilliance is so intense that it outshines entire galaxies. This cloud, the corona, is like a boiling cauldron.
The Shadow Breath of a Neutron Star: Axions and the X-ray Puzzle
Some 123 parsecs from Earth, in the constellation Corona Australis, drifts the neutron star RX J1856.5-3754. Its diameter is about 12 kilometers, smaller than Moscow's Ring Road, but its surface temperature reaches 460 000 kelvin. The star emits a slow, almost inaudible exhalation.
HEP Experiment2026-07-232 minarXiv:2607.21363express
Archaeological Lead Catches Solar Axions
Deep underground, in the silence of a cryostat (a cooled container), lie crystals of lead that once belonged to an ancient Roman ship. This material barely emits background radiation — over two thousand years, unstable isotopes have decayed, leaving it perfectly clean for hunting the rarest events.
High Energy2026-07-212 minarXiv:2607.18647express
Starlight Betrays Elusive Particles
A lighthouse at sea doesn't just rotate: its lamp itself dims and brightens on its own. Magnetic white dwarfs, the ultra-dense remnants of stars like our Sun, behave in much the same way. Their powerful magnetic fields can convert light into axions — hypothetical particles that could explain the Universe's hidden mass.
Nuclear Theory2026-07-212 minarXiv:2607.19220express
How Quarks Help Neutron Stars Avoid Collapsing
A handful of sand in your fist: the grains press against each other, and your hand can't squeeze any further. Ordinary matter behaves similarly. But in a neutron star, compression is billions of times stronger — atoms are crushed, electrons are squeezed into protons, and nearly all space is filled with neutrons.
High Energy2026-07-202 minarXiv:2607.18124express
Neutron Star Twins: When Precision Changes the Picture
A neutron star is the collapsed core of a massive star, squeezed to the size of a city. A teaspoon of its material weighs as much as a mountain. But inside this superdense sphere, a surprise may lurk: under unimaginable pressure, neutrons break apart into quarks, giving the star a new, more compact core.
Stellar2026-07-082 minarXiv:2607.07781
Cosmic Brake: How to Catch Aliens by the Spin of Stars
For decades, SETI has hunted for Dyson spheres — hypothetical shells that capture a star's light stars and re-radiate it in the infrared. But the cosmos remains silent. Perhaps an alien intelligence operates more elegantly: instead of collecting light, it tames the rotation of a sun, like a giant flywheel.
Dark Core or Pearlescent Layer: Metamorphoses of Neutron Stars
Neutron stars — remnants of supernovae — are among the densest objects in the Universe. Their central density exceeds nuclear density many times over, and gravity is surpassed only by black holes.
Message from the Invisible World: FAST Listens to Axions
The story began with a puzzle: in the 1930s, Fritz Zwicky noticed that clusters of galaxies behave as if an enormous invisible mass is hidden within them. Half a century later, Vera Rubin confirmed that stars on the outskirts of galaxies rotate too fast to be held by visible matter alone.
Nuclear Theory2026-06-041 minarXiv:2606.06378express
Neutron Stars: Frozen on the Verge of a Phase Change
Neutron stars are cosmic 'ice cubes' of unimaginable density: a tablespoon of their material would outweigh Mount Everest. It was a mystery what lay in their cores: ordinary neutron matter (a giant atomic nucleus) or exotic quark matter, where particles are not bound into neutrons.
The Universe's Radio Concert: How 30 Seconds of Silence Are Changing Physics
Listening to the cosmos requires patience and a finely tuned ear. Astronomers chose the most sensitive low-frequency instrument for this: the OVRO–LWA antenna array — 352 dipole antennas scattered across two and a half kilometers of California desert.
Plateau and Dip: The Music of Cosmic Strings
The Universe doesn't just expand — it resonates. After the Big Bang, stretched strings remained in its fabric — thin as a proton, yet heavy as a mountain range. Their oscillations give birth to gravitational waves, and in this radiation, like in a musical score, the history of fundamental symmetries is encoded.
Nuclear Theory2026-06-021 minarXiv:2606.03993express
The shape of the xenon nucleus is no longer a mystery
Atomic nuclei are not always like billiard balls. Some are elongated, like cigars, others are flattened. But xenon-129 resembles a potato — a bumpy triaxial ellipsoid.
Cosmology2026-05-252 minarXiv:2605.26265express
How Solar X-rays Catch Invisible Particles
Tiny invisible bullets pass straight through the Sun, barely noticing its matter. These are axions — hypothetical particles so light and elusive that they are often compared to ghosts.
HEP Phenomenology2026-04-292 minarXiv:2604.26860express
Why Gravitational Waves Whisper About a Hundred Mega-Electronvolts
In a vast hall, a hundred tuning forks are set out. Each one is a pulsar — an ultra-dense stellar remnant spinning at a furious rate, sending out radio pulses more precisely than any clock. When a low-frequency sound wave sweeps through the hall, all the tuning forks start to go slightly out of tune at the same moment.
Nuclear Experiment2026-04-282 minarXiv:2604.25107express
Tin Nucleus Reveals Its Size
Two tin nuclei collide at about two-thirds the speed of light. For an instant, a hot, dense cloud forms, and protons fly out in all directions. If you catch pairs of protons and measure how often they fly off in the same direction, you can work out the size of that cloud. This method is called femtoscopy: it works like a microscope for nuclear scales.
HEP Phenomenology2026-04-282 minarXiv:2604.26004express
A Window for Invisible Particles: Axions Are Back
In 1987, astronomers saw a supernova flare up in a neighboring galaxy — the Large Magellanic Cloud. It was a rare gift: the explosion was close enough to catch not just light but also neutrinos, those nearly undetectable particles that pass straight through Earth.
HEP Phenomenology2026-04-222 minarXiv:2604.21077express
Listening for the Unseen: Hunting Axions in Stellar Cataclysms
Imagine a tiny coin hidden inside a perfect safe, but the walls are so thin that the coin sometimes slips right through, leaving a barely audible sound. Axions are like those coins — except instead of metal, they're particles, and instead of a safe, they're ordinary matter. They barely notice obstacles, making them incredibly hard to catch directly.
HEP Experiment2026-04-172 minarXiv:2604.16602express
Axion Radio: How to Hear the Invisible
In a noisy city, you try to hear a cricket. It's quiet, and cars are humming all around. To catch its chirp, you set up a sensitive microphone and hit the noise-cancellation button. That's roughly how physicists hunt for axions — hypothetical particles that could be the very dark matter holding galaxies together.
HEP Phenomenology2026-04-011 minarXiv:2604.01277express
Cosmic Invisibles: Axions and Supernova Light
When a massive star dies, a supernova explosion occurs, so powerful that a single flash outshines an entire galaxy. In this fire, billions of axions are born — invisible particles that leave almost no trace. Every second, trillions of these tiny things fly right through each of us, completely unnoticed.
HEP Phenomenology2026-03-292 minarXiv:2603.28826express
Axions at Neutron Star Poles: A Key to Dark Matter
Neutron stars are the compressed cores of dead stars — city-sized objects with staggering density. Some of these stars become pulsars, cosmic lighthouses emitting strictly periodic radiation pulses.
How to Tell a Pion from a Kaon in a Fireball
In collisions of heavy nuclei, a fireball of thousands of particles is born. Among them are pions and kaons, two kinds of light particles that look very much alike. To understand what happens in this fireball, physicists need to know exactly how many of each particle flew out.
HEP Experiment2026-02-161 minarXiv:2602.14538express
Argon catches dark matter
In the dark chamber of the detector, argon waits. When an invisible particle (say, a dark matter candidate) flies through, it gives the argon nucleus a gentle shove. The nucleus is knocked out of place, and charges are born around it. Exactly how many charges is no trivial question: physicists use that number to tell what kind of visitor dropped by.
High Energy2026-01-161 minarXiv:2601.11718express
Neutron Star's Light Is More Polarized Than Expected
In the binary system Cyg X-2, a neutron star pulls matter from a normal companion star. The infalling gas spirals in, heats up to millions of degrees, and shines brightly in X-rays. Astronomers pointed two space telescopes, IXPE and NuSTAR, at this object and, for the first time, measured in detail how polarized that light is.
HEP Phenomenology2026-01-131 minarXiv:2601.08567express
Ghost Particle: How Scientists Caught a Hint of a New Force
At Hungary's Institute for Nuclear Research, ATOMKI, physicists noticed something odd: in the decays of excited atomic nuclei, pairs of electrons and positrons sometimes fly apart at an unusual angle. It's as if an invisible mediator particle briefly appears and disappears between them.
High Energy2026-01-101 minarXiv:2601.06409express
Ice detectors listen to the radio voices of cosmic particles
Neutrinos are ghost particles: predicted by the Standard Model, they barely interact with matter. Catching them is like trying to hear a whisper in the roar of a waterfall.
Nuclear Theory2026-01-091 minarXiv:2601.05999express
How to Peer Inside a Neutron Star
Inside a neutron star, matter is squeezed so tightly that a teaspoon of its material would weigh as much as a mountain. We can't directly see what happens to particles under such conditions, but stars tell us about themselves through gravitational waves and light when two such stars merge.
HEP Phenomenology2025-10-131 minarXiv:2510.11879express
Microscopic Black Holes: Aftermath of Cosmic Catastrophes
Cosmic rays are elementary particles carrying colossal energy that pierce the intergalactic void. When two such particles smash head-on, the energy density at the point of impact could be enough to collapse into a black hole the size of an atomic nucleus.
Fingerprints in the Spectrum: Pulsars vs. Dark Matter
The cosmic electron spectrum is like fingerprints at a crime scene. Particles arriving from the depths of the Galaxy carry in their energies the traces of those that produced them. For a long time, the picture was blurred: instruments with wide energy bins, like out-of-focus photographs, did not reveal details.