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Axions and axion-like particles vs Primordial Black Holes

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	Axions and axion-like particles Frontier	Primordial Black Holes Frontier
Proposed	1977 / 1983	1974 / 1975
Key figures	Roberto Peccei, Helen Quinn, Steven Weinberg, Frank Wilczek, John Preskill, Pierre Sikivie	Bernard Carr, Stephen Hawking
In one sentence	Very light particles originally proposed to solve a fine-tuning problem in QCD (the strong-CP problem), with a tiny coupling to photons that makes them invisible to most experiments but also makes them a natural cold-dark-matter candidate.	Black holes that formed in the first fraction of a second after the Big Bang, from regions where the matter density was unusually high. They gravitate exactly like dark matter would. Strict constraints from microlensing and gravitational waves allow only a sub-fraction of dark matter to be PBHs in most mass windows.
Predictions	A narrow radio signal from microwave cavity haloscopes (resonant chambers that amplify axion-to-photon conversion in a strong magnetic field), tuned to a frequency set by the unknown axion mass (f = m_a c² / h), with peak power fixed by the axion-photon coupling Stellar cooling anomalies: helium-burning stars and SN1987A would lose energy faster than observed if axion-photon couplings were too strong, bounding the coupling Time-varying signals in precision atomic clocks, NMR experiments, and interferometers from coherent oscillation of an axion dark matter field Spectral features from axion-photon conversion in galactic, stellar, and laboratory magnetic fields	Microlensing events: temporary brightening of background stars as a PBH passes in front, with event rate and timescale set by PBH mass and abundance Gravitational wave signals from PBH-PBH binary mergers, especially in mass gaps where stellar evolution predicts no black holes (~3-5 solar masses, ~50-100 solar masses pair-instability gap) CMB and reionization constraints: gas accretion onto PBHs in the early universe would deposit energy, affecting the CMB temperature and reionization history Diffuse gamma-ray background from [[Hawking radiation]] of very-low-mass PBHs (M < 10^14 g) that would have evaporated by now
Where it breaks	Theoretically well-motivated but the allowed parameter space is vast: several orders of magnitude in mass and in coupling Some axion-production scenarios would leave a patchy imprint in the ancient light of the CMB (an isocurvature signal) that we do not see, so they survive only if the conditions during cosmic inflation are tuned No direct collider or laboratory hint; all motivation is theoretical and cosmological Critics argue axions are easy to 'rescue' with parameter tuning whenever an experiment finds nothing	Microlensing surveys (OGLE, EROS, Subaru HSC) and dynamical limits exclude PBHs as 100% of dark matter across the asteroid-to-solar-mass range almost everywhere Most LIGO/Virgo events have plausible astrophysical alternative explanations (stellar BH binary formation in dense globular clusters or galactic nuclei) Many formation models require fine-tuned primordial power spectra or specific inflationary features The asteroid-mass window is hard to probe directly: no current microlensing experiment is sensitive at that scale, leaving the most-allowed window also the least-tested
Key unresolved problem	The unknown-mass problem: the axion's mass could fall anywhere across a vast range, and no experiment can yet sweep the whole plausible window in any reasonable amount of time.	The untestable window problem: the only mass range where primordial black holes could still be all the dark matter, roughly asteroid-sized, is exactly the one no current star-brightening (microlensing) survey is sensitive enough to check.
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Axions and axion-like particles

1977 / 1983 · Frontier

Primordial Black Holes

1974 / 1975 · Frontier

Proposed

1977 / 1983

1974 / 1975

Key figures

Roberto Peccei, Helen Quinn, Steven Weinberg, Frank Wilczek, John Preskill, Pierre Sikivie

Bernard Carr, Stephen Hawking

In one sentence

Very light particles originally proposed to solve a fine-tuning problem in QCD (the strong-CP problem), with a tiny coupling to photons that makes them invisible to most experiments but also makes them a natural cold-dark-matter candidate.

Black holes that formed in the first fraction of a second after the Big Bang, from regions where the matter density was unusually high. They gravitate exactly like dark matter would. Strict constraints from microlensing and gravitational waves allow only a sub-fraction of dark matter to be PBHs in most mass windows.

Predictions

A narrow radio signal from microwave cavity haloscopes (resonant chambers that amplify axion-to-photon conversion in a strong magnetic field), tuned to a frequency set by the unknown axion mass (f = m_a c² / h), with peak power fixed by the axion-photon coupling
Stellar cooling anomalies: helium-burning stars and SN1987A would lose energy faster than observed if axion-photon couplings were too strong, bounding the coupling
Time-varying signals in precision atomic clocks, NMR experiments, and interferometers from coherent oscillation of an axion dark matter field
Spectral features from axion-photon conversion in galactic, stellar, and laboratory magnetic fields

Microlensing events: temporary brightening of background stars as a PBH passes in front, with event rate and timescale set by PBH mass and abundance
Gravitational wave signals from PBH-PBH binary mergers, especially in mass gaps where stellar evolution predicts no black holes (~3-5 solar masses, ~50-100 solar masses pair-instability gap)
CMB and reionization constraints: gas accretion onto PBHs in the early universe would deposit energy, affecting the CMB temperature and reionization history
Diffuse gamma-ray background from [[Hawking radiation]] of very-low-mass PBHs (M < 10^14 g) that would have evaporated by now

Where it breaks

Theoretically well-motivated but the allowed parameter space is vast: several orders of magnitude in mass and in coupling
Some axion-production scenarios would leave a patchy imprint in the ancient light of the CMB (an isocurvature signal) that we do not see, so they survive only if the conditions during cosmic inflation are tuned
No direct collider or laboratory hint; all motivation is theoretical and cosmological
Critics argue axions are easy to 'rescue' with parameter tuning whenever an experiment finds nothing

Microlensing surveys (OGLE, EROS, Subaru HSC) and dynamical limits exclude PBHs as 100% of dark matter across the asteroid-to-solar-mass range almost everywhere
Most LIGO/Virgo events have plausible astrophysical alternative explanations (stellar BH binary formation in dense globular clusters or galactic nuclei)
Many formation models require fine-tuned primordial power spectra or specific inflationary features
The asteroid-mass window is hard to probe directly: no current microlensing experiment is sensitive at that scale, leaving the most-allowed window also the least-tested

Key unresolved problem

The unknown-mass problem: the axion's mass could fall anywhere across a vast range, and no experiment can yet sweep the whole plausible window in any reasonable amount of time.

The untestable window problem: the only mass range where primordial black holes could still be all the dark matter, roughly asteroid-sized, is exactly the one no current star-brightening (microlensing) survey is sensitive enough to check.

Reader vote

No votes yet