Axion-Like Particles and Their Cosmological Consequences
Ziqian Yu
a
University of California, Santa Barbara, 585 Sweet Rain Place, Goleta, U.S.A.
Keywords: Axion-Like Particles, Cosmology, Dark Matter, Particle Physics, Beyond Standard Model Physics.
Abstract: Axion-like particles (ALPs) are hypothetical particles that have garnered significant attention in both particle
physics and cosmology due to their potential roles in addressing unresolved issues such as the strong CP
problem, dark matter, and dark energy. This paper provides a comprehensive overview of ALPs, starting with
their theoretical foundations and production mechanisms in the early universe. The paper will explore their
interactions with standard model (SM) particles and their influence on cosmological phenomena, including
Big Bang nucleosynthesis, the cosmic microwave background, and structure formation. Furthermore, the
paper will examine the viability of ALPs as dark matter candidates and their potential contributions to the
dynamics of dark energy. Current experimental efforts, including direct detection methods like haloscopes
and helioscopes, along with indirect detection strategies through astrophysical observations, are reviewed.
The challenges and open questions in ALP research are discussed, highlighting the need for future theoretical
and experimental advancements to unveil the mysteries surrounding these elusive particles.
1 INTRODUCTION
As research into axions, a theoretical particle
introduced to address the strong CP problem in
quantum chromodynamics (QCD), progressed, it
became clear that a broader class of particles, now
known as axion-like particles (ALPs), could arise
from a variety of theoretical models beyond the
original scope of the QCD axion. These models often
emerge from extensions of the Standard Model,
including string theory and other high-energy
frameworks that propose additional dimensions or
symmetries. Unlike the QCD axion, ALPs are not
strictly bound to the strong CP problem, and their
properties—such as mass and coupling constants—
can vary widely depending on the specific model.
This flexibility makes ALPs a versatile tool for
exploring new physics beyond the Standard Model,
particularly in areas where existing theories fall short.
ALPs and axion have been extensively studied as
promising candidates for dark matter. Their weak
interactions with other standard model particles and
their potential to account for different astrophysical
and cosmological observations make them a
significant focus in contemporary physics research.
a
https://orcid.org/0000-0002-3721-6468
One of the most intriguing aspects of ALPs is
their potential role as dark matter candidates. Dark
matter is a foundational element of modern
cosmology, making up close to one third of the
universe's mass-energy content (much larger than that
of baryons), yet it remains elusive, interacting
primarily through gravity. Traditional dark matter
candidates, like weakly interacting massive particles
(WIMPs), have not yet been detected, prompting
researchers to explore alternatives, including ALPs.
ALPs are particularly interesting because their weak
interactions with Standard Model particles allow
them to avoid many of the constraints that have
excluded other dark matter candidates. Additionally,
their ability to form cold dark matter, depending on
the production mechanisms involved, aligns well
with observations of large-scale cosmic structures.
Beyond their role as dark matter, ALPs may also
influence cosmic evolution. The interactions between
ALPs and particles like photons and nucleons could
affect key events in the early universe, such as Big
Bang nucleosynthesis (BBN) and the buildup of the
cosmic microwave background (CMB). For instance,
ALPs might alter the photon-to-baryon ratio, thereby
impacting the synthesis of light elements and the
Yu, Z.
Axion-Like Particles and Their Cosmological Consequences.
DOI: 10.5220/0013075800004601
Paper published under CC license (CC BY-NC-ND 4.0)
In Proceedings of the 1st International Conference on Innovations in Applied Mathematics, Physics and Astronomy (IAMPA 2024), pages 321-329
ISBN: 978-989-758-722-1
Proceedings Copyright © 2024 by SCITEPRESS Science and Technology Publications, Lda.
321
variation of temperature observed in the CMB. While
these effects may be subtle, they are significant
enough to make the study of ALPs an important
avenue for testing cosmological models and
understanding early universe conditions.
Furthermore, ALPs are also being considered as
potential drivers of dark energy, an enigmatic force
driving the universe's accelerated expansion. In
certain theoretical models, ALPs are considered
scalar fields with characteristics that enable them to
imitate the behavior of a cosmological constant or
various types of dynamic dark energy. These models
suggest that ALPs could contribute to a slowly
varying energy density that drives cosmic
acceleration, offering a potential explanation for
observations that challenge the standard ΛCDM
model. Including ALPs in dark energy theories not
only broadens our understanding of the universe's
expansion history but also introduces new
observational signatures that could be detected
through high-precision cosmological surveys.
The ongoing search for ALPs extends across
multiple experimental and observational frontiers.
Direct detection efforts, such as those conducted by
haloscopes and helioscopes, aim to observe ALPs
interacting with strong magnetic fields or being
produced in astrophysical environments like the Sun.
Indirect searches focus on astrophysical phenomena,
such as the cooling rates of stars, gamma-ray
observations, and the polarization of the CMB, which
could reveal the presence of ALPs through their
interactions with other particles. Despite the
challenges associated with detecting such weakly
interacting particles, advances in technology and
experimental techniques continue to expand the limits
of possibility, moving us nearer to the potential
discovery of these elusive particles.
This paper aims to delve into the cosmological
consequences of ALPs by first providing a thorough
introduction to their theoretical foundations and
production mechanisms. The paper will then explore
their possible roles in dark matter, dark energy, and
the formation of cosmic structures. By reviewing
current theoretical models, experimental efforts, and
observational evidence, the paper aim to highlight the
significant challenges and open questions that remain
in the field. Ultimately, this paper seeks to provide a
comprehensive overview of how ALPs could reshape
our comprehension of the universe and the
fundamental forces that regulate it. As the paper move
forward, the study of ALPs promises to be a key area
of research with significant consequences for both
particle physics and cosmology.
2 THEORETICAL
FRAMEWORKS OF AXION-
LIKE PARTICLES
2.1 Origin and Properties of ALPs
The Peccei-Quinn (PQ) mechanism, introduced in the
late 1970s, was suggested as a solution to the strong
CP problem, which explains why QCD appears not to
violate CP symmetry as one would anticipate. CP
symmetry involves the combination of charge (C)
conjugation and parity (P) symmetries.
The strong CP problem arises because the QCD
Lagrangian includes a term that could potentially
break CP symmetry, yet experimental results have
shown that such a violation is extremely rare.
The Peccei-Quinn mechanism introduces a new
global U(1) symmetry, called Peccei-Quinn (PQ)
symmetry, which is spontaneously broken, resulting
in the appearance of a new pseudoscalar particle
known as the axion.
The axion field can dynamically eliminate the CP-
violating term, effectively setting 𝜃

=0, thus
resolving the strong CP problem.
2.2 ALPs in Particle Physics Models
Axion-like particles (ALPs) are theoretical entities
resembling axions, but they aren't necessarily linked
to solving the strong CP problem. Unlike the QCD
axion, ALPs can have a wide range of masses and
coupling constants. Their mass tends to be
considerably smaller than that of standard model
particles, and they can arise through various
mechanisms, such as explicit PQ symmetry breaking.
ALPs have very weak interactions with standard
model particles, meaning their effects on gravity are
notable, making them strong dark matter candidates.
The interaction strengths between ALPs and standard
model particles are typically described by coupling
constants, which influence their interactions with
photons, fermions, and gluons. These interactions are
typically modeled using effective Lagrangians.
In string theory, ALPs can naturally arise as
pseudo-Nambu-Goldstone bosons due to the
spontaneous breaking of global symmetries. These
particles may stem from higher-dimensional gauge
symmetries that become apparent after
compactification. Within various string theory
IAMPA 2024 - International Conference on Innovations in Applied Mathematics, Physics and Astronomy
322
scenarios, ALPs can exhibit a wide array of masses
and coupling constants, offering a fertile ground for
theoretical physics exploration.
Beyond string theory, ALPs also feature in other
beyond the Standard Model (BSM) theories. These
include models that extend the Higgs sector, grand
unified theories (GUTs), and other standard model
extensions aimed at addressing the hierarchy
problem, dark matter, and baryogenesis.
3 PRODUCTION MECHANISMS
OF ALPS IN THE EARLY
UNIVERSE
3.1 Thermal Production mechanisms
3.1.1 ALP Thermal Production in Early
Universe
In the early universe, axion-like particles (ALPs) can
be thermally produced through various interactions.
The production typically involves scattering and
decay processes that occur at high temperatures, often
before or during the epoch of BBN. The rate that ALP
produces depends on their coupling to photons,
electrons, nucleons and other standard model
particles.
Moreover, ALPs decouple when their interaction
rate becomes slower than the rate of cosmic
expansion. (Carenza et al., 2021). However, in low-
reheating cosmological scenarios, where the
reheating temperature can be significantly lower
(even down to a few MeV), the expansion rate of the
universe is quicker than predicted by the standard
model. This accelerated expansion causes the ALPs
to decouple earlier at higher temperatures, leading to
a suppression in their thermal relic abundance.
Consequently, this scenario allows for the possibility
of heavier ALPs, as the cosmological mass bounds
are relaxed in such low-reheating environments.
3.1.2 Impact of ALP Interactions with
Photons, Electrons, and Nucleons
The interactions between ALPs and standard model
particles such as photons, electrons, and nucleons
play a crucial role in shaping the thermal evolution of
ALPs and the overall history of the universe.
For instance, the interaction of ALPs with photons
(resonant photon-ALP conversion) could influence
the cosmic microwave background (CMB) by
modifying photon distribution, leading to distortions
in the black-body spectrum of the CMB, causing a
reduction in the number of photons, and,
consequently, an apparent decrease in the CMB
temperature in the direction of the affected galaxy
clusters.
ALPs coupled to nucleons can be efficiently
produced in the core of supernovae through the
nucleon-nucleon bremsstrahlung process. This
mechanism is significant because it allows for the
prolific production of ALPs in the supernova core,
where large densities and high temperatures are
present. The produced ALPs can escape the
supernova, contributing to a large flux of ALPs.
3.2 Non-Thermal Production
Mechanisms of ALPs
3.2.1 Misalignment Mechanism
The misalignment mechanism is a non-thermal
process through which axions are produced in the
early universe. This happens when the axion field
starts off "misaligned" from the minimum of its
potential, rather than starting at the minimum. This
misalignment continues because, in the early
universe, the Hubble expansion rate is much higher
than the axion field's mass. As the universe continues
to expand and cool, the Hubble parameter decreases,
eventually enabling the axion field to eventually
oscillate around the minimum of its potential.
The
oscillations resemble cold dark matter, with the
axion's energy density depending on the initial angle
of misalignment (axion field's initial displacement)
and the axion mass.
For axion-like particles (ALPs), energy density
generated by the misalignment mechanism is
influenced by factors like the initial misalignment
angle, the ALP mass, and the PQ scale. This
mechanism is particularly intriguing because it does
not depend on thermal processes and can produce a
cold dark matter component that is independent of the
universe's thermal history.
3.2.2 Decay of Topological Defects
Topological defects, which include structures like
cosmic strings and domain walls, arise when the
universe undergoes symmetry-breaking phase
transitions. These defects are particularly important
because their decay can lead to the production of
ALPs, which contribute to the cold dark matter
density in space.
As PQ symmetry break at high energies, Cosmic
strings form as line-like defects where the axion field
Axion-Like Particles and Their Cosmological Consequences
323
winds around a vacuum expectation value. As the
universe continues to cool and experiences additional
phase transitions, especially the QCD phase
transition, these strings may become connected to
domain walls if the domain wall number exceeds one
(Chang, S., 1998). The resulting ALPs are often
relativistic and could contribute to the dark radiation
or act as a warm dark matter component depending
on their mass and coupling constants.
Domain walls, formed by two-dimensional
defects when the PQ symmetry breaking leads to
discrete degeneracies in the vacuum state, are causing
series result in cosmology because they can dictate
the energy density of the cosmos, leading to conflicts
with observed cosmological data (Saikawa, 2017).
However, if these walls decay before they dominate,
they are able to produce a large amount of ALPs. The
ALPs produced this way is typically linked to the
scale of PQ symmetry breaking.
The decay of these topological defects is affected
by several aspects, such as the coupling between
ALPs and other particle fields, the dynamics of the
defects themselves, and the presence of any external
fields that might interact with the defects.
4 ALPS AND COSMIC
EVOLUTION
4.1 Influence on Big Bang
Nucleosynthesis (BBN)
BBN, which involves the formation of light elements
such as hydrogen, helium, and lithium within the first
few minutes after the Big Bang, is extremely sensitive
to the conditions present in the early universe. Key
factors include the density of baryons, the rate of
cosmic expansion, and interactions between particles.
Axion-Like Particles (ALPs), which are hypothetical
particles, could interact with Standard Model
particles such as photons, nucleons, and leptons,
potentially affecting these crucial conditions.
One of the primary ways ALPs can affect BBN is
through their interactions with photons or nucleons.
For instance, if ALPs are produced in sufficient
quantities, have the potential to modify the baryon-to-
photon ratio (η) as well as the effective number of
relativistic degrees of freedom (𝑁

), which could
impact the expansion rate of the universe,
subsequently affecting the production of light
elements like deuterium (
2
H) and helium-4 (
4
He). The
combined observations from BBN and the CMB
place tight limits on the parameter space of ALPs,
particularly ruling out regions where ALPs would
lead to significant deviations in light element
abundances (Millea et al., 2015).
4.2 Indication From Cosmic
Microwave Background
The CMB is the remnant radiation from the Big Bang,
offering a glimpse into the universe roughly 380,000
years after the Big Bang. The CMB carries imprints
of the physics of the early universe, including
potential interactions between ALPs and photons. As
a fundamental observable of cosmology, the CMB
serves as a critical tool for probing the early universe
and any new physics, such as the existence of ALPs.
ALPs can interact with photons through resonant
conversion processes, particularly in the presence of
magnetic fields within galaxy clusters. These
interactions can lead to observable polarized
distortions in the CMB, such as changes in the
anisotropy spectrum or polarization patterns, which
would manifest differently from other well-known
CMB signals like those caused by gravitational
lensing. The presence of ALPs could also result in
additional temperature fluctuations at high
multipoles, distinct from the standard CMB spectrum.
These temperature fluctuations, if detected, would
offer further evidence supporting the existence of
ALPs, highlighting the importance of high-resolution
CMB observations.
Moreover, spectral distortions in the CMB, which
can arise from processes such as energy injection or
non-thermal effects, could also provide indirect
evidence for ALPs. These distortions are highly
sensitive to the thermal history of the universe and
any new particles or interactions that could alter this
history. As such, analyzing spectral distortions allows
cosmologists to explore the thermal processes in the
early universe, where ALPs could play a significant
role.
Future CMB experiments with improved
capabilities are expected to significantly tighten these
constraints, offering a more comprehensive picture of
ALPs' impact on the universe.
4.3 Role in Structure Formation
Axion-like particles (ALPs) also plays a crucial role
in the formation of cosmic structures such as galaxies,
clusters, and large-scale filaments in the universe.
Unlike traditional cold dark matter (CDM), ALPs can
have different properties, exhibiting wave-like effects
on certain scales where these effects dominate over
self-gravity and a smaller mass or interactions with
IAMPA 2024 - International Conference on Innovations in Applied Mathematics, Physics and Astronomy
324
other particles, which can lead to distinct signatures
in structure formation.
ALPs can form a form of dark matter that is
slightly warmer than CDM, sometimes referred to as
"fuzzy dark matter" (Shen et al., 2023) or "ultralight
dark matter." The quantum mechanical effects due to
the small mass of ALPs can cause a reduction in the
formation of structures at smaller scales.
This suppression occurs because the de Broglie
wavelength of ALPs, which is inversely proportional
to their mass, can become comparable to or larger
than the size of small-scale structures, leading to a
phenomenon known as "quantum pressure" or "wave-
like behavior". This effect can prevent the formation
of scale of diminutive structures. For example, dwarf
galaxies, which would be abundant in a purely CDM
scenario. Moreover, such suppression is related to the
quantum pressure that counteracts gravitational
collapse on small scales, resulting in a cutoff in the
linear matter power spectrum.
Moreover, ALP dark matter can influence the
formation of cosmic structures by affecting the
collapse of dark matter halos, the building blocks of
galaxies and larger structures. In scenarios involving
fuzzy dark matter, halos can form solitonic cores —
dense, stable regions at the centers of dark matter
halos. These cores are surrounded by more diffuse
outer regions, creating a unique structure that can be
contrasted with predictions from standard denser
CDM models.
5 ALPS AND DARK MATTER
5.1 ALPs as Dark Matter Candidates
Just like what the previous section 2 passage indicate,
ALPs are considered strong contenders for dark
matter due to their distinct properties, including weak
interactions with standard model particles and the
potential to make up a significant portion, or even all,
of dark matter.
ALPs as a weak coupling dark matter can arise in
various theoretical frameworks, including string
theory and other beyond the Standard Model (BSM)
scenarios. Depending on their mass and coupling
constants, ALPs can manifest as cold dark matter,
similar to the canonical WIMP (Weakly Interacting
Massive Particle) models. ALPs are also being
regards as the substance of "Fuzzy dark matter"
models, where they have ultralight masses, suppress
small-scale structures due to quantum mechanical
effects, providing a potential answer to some of the
small-scale issues encountered with CDM.
The characteristics of ALPs as potential dark
matter contenders are constrained by various
astrophysical observations and experimental
searches. Astrophysical observations, such as the
CMB, can serve to limit or define the characteristics
of ALPs.
Overall, while ALPs remain a reasonable
contender for dark matter, their exact role depends on
further observational and experimental evidence,
which will help to narrow down the range of allowed
properties and clarify their contribution to the
composition of dark matter present in the universe.
5.2 Direct and Indirect Detection
Methods
5.2.1 Laboratory Searches for ALPs
Haloscopes and helioscopes are two of the primary
laboratory-based techniques used to look for ALPs.
To detect ALPs that could comprise the dark
matter halo over our galaxy, various experiments
focus on the interaction between the axion field and
photons in the presence of a strong magnetic field,
which facilitates the conversion of ALPs into
detectable photons. The most prominent haloscope
experiment is ADMX (Axion Dark Matter
eXperiment), which has established significant
constraints on ALP masses and couplings within the
microwave frequency range (Khatiwada et al., 2021).
Other methods like Helioscopes are telescopes
designed to detect ALPs produced in the Sun. The
best helioscope here is CAST (CERN Axion Solar
Telescope), which detects potential axions generated
in the Sun by observing the effect produced by their
conversion into photons under a strong magnetic field
(Barth et al., 2013). The experiment has progressed
through several stages, employing a decommissioned
LHC dipole magnet to track movement of the Sun and
convert the generated axions into discernible X-ray
photons via axion-photon interactions. This help
narrow down the parameter space where ALPs could
exist.
5.2.2 Indirect Detection through
Astrophysical Signals
Indirect detection includes gamma ray observations.
For gamma-ray observations, ALPs can interact with
photons when exposed to external magnetic fields,
which allows for photon-ALP conversions. This
conversion is facilitated by the two-photon vertex
interaction described in the context of ALPs, where
high-energy gamma rays from astrophysical sources
Axion-Like Particles and Their Cosmological Consequences
325
can convert into ALPs and vice versa when they pass
through regions with strong magnetic fields (Hooper
& Serpico, 2007). For example, gamma rays from
distant astrophysical sources could convert into ALPs
when subjected to B fields, leading to irregularities in
the detected high-energy photon flux. Observatories
like the Fermi Gamma-ray Space Telescope have
been used to search for such signatures, providing
constraints on ALP properties.
Gamma-ray telescopes, both space-based (like the
GLAST satellite) and ground-based (such as HESS,
MAGIC, and VERITAS), can potentially detect the
signature of ALP-photon conversions by observing
distortions in the gamma-ray spectra. The detection
strategy involves looking for spectral features that
deviate from the expected power-law behavior due to
the depletion of gamma rays converted into ALPs.
Other methods include Stellar Cooling: ALPs
could be produced in the cores of stars and
subsequently escape, carrying away energy and
affecting the cooling rates of stars (Zhang et al.,
2024). Observations of white dwarfs, red giants, and
other stellar remnants provide constraints on ALP
couplings based on how well these stars' cooling
behaviors match theoretical predictions. The faster-
than-expected cooling of certain stars has been
proposed as indirect evidence for ALPs, although
alternative explanations also exist.
6 ALPS AND DARK ENERGY
6.1 ALPs as a Source of Dark Energy
6.1.1 Theoretical Models Linking ALPs to
Dark Energy
In some theoretical models, ALPs are introduced as
scalar fields with properties that allow them to
influence the large-scale dynamics of the universe.
These models often draw from ideas in string theory
and other extensions of the Standard Model.
One of the primary mechanisms through which
ALPs could contribute to dark energy is by acting as
a quintessence field. In these models, ALPs possess a
very light mass and a potential energy that evolves
slowly over time, leading to a negative pressure that
drives cosmic acceleration. The slow roll of the ALP
field down its potential mimics the behavior of a
cosmological constant, but with time-dependent
characteristics that could be observed in the evolution
of the universe's expansion rate.
6.1.2 Cosmological Implications of ALP-
driven Dark Energy
Including ALPs as potential candidates for dark
energy has profound implications for cosmology. A
key prediction of ALP-driven dark energy models is
the development of the equation of state parameter w,
which characterizes the relationship between the
pressure and density of dark energy. Unlike the
cosmological constant, where w = 1, ALP models
can result in a temporally evolving equation of state
w. This variation could be observed through detailed
studies of the CMB, large-scale structure, and
supernovae.
These models also influence the growth of cosmic
structures (Ruchika et al., 2023).
ALP-driven dark energy can modify the rate at
which structures form and evolve, leading to
observable differences in the distribution of galaxies
and clusters. Additionally, the coupling between
ALPs and other fields can lead to new signatures in
gravitational wave observations, providing a unique
way to test these models.
6.2 Observational Signatures
As ALPs are considered a source of dark energy, they
could produce distinctive signatures that may be
detectable through various cosmological
observations.
A possible indication could arise from the
gravitational signatures produced by ALPs with non-
periodic potentials. These particles may undergo
processes such as parametric resonance and field
fragmentation, which can lead to the formation of
dense halos. These halos could result in observable
gravitational phenomena, covering phenomena such
as astrometric lensing, the diffraction of gravitational
waves from black hole mergers, and the photometric
microlensing of stars with extreme magnification
(Chatcrhon et al., 2024). These phenomena could
provide indirect evidence for the presence of ALPs
and their contribution to cosmological processes,
including dark energy.
This gravitational effect could be observed by
gravitational microlensing phenomenon, where an
axion star and a background star align, causing the
light from the star to be lensed, creating a
characteristic light curve that can be detected by
telescopes.
Additionally, Large-scale structure (LSS)
surveys and supernovae observations are critical tools
for constraining ALP-driven dark energy models
(Ivanov et al., 2020). LSS surveys, which map the
IAMPA 2024 - International Conference on Innovations in Applied Mathematics, Physics and Astronomy
326
distribution of galaxies across vast cosmic volumes,
can reveal how the growth of structures has evolved
over time. Deviations from the expected clustering
patterns in the ΛCDM model could indicate the
presence of ALP-induced modifications to dark
energy.
Supernovae, particularly Type Ia supernovae,
serve as "standard candles," are essential for
measuring cosmic distances. By analyzing the
observed brightness of these supernovae across
various redshifts, astronomers can trace the history of
expansion of the cosmos. Any deviation on the
expected relationship between distance and redshift
could provide evidence for a varying equation of state
driven by ALPs.
These constraints help narrow down the
parameter space where ALPs could play a role as dark
energy and provide essential tests for the validity of
these models.
7 CURRENT AND FUTHER
EXPERIMENTAL EFFORTS
7.1 Existing Experiments and
Observations
Current effort on observation of ALPs (axion-like
particles) includes ADMX and CAST that previous
passage have introduced, and the more advanced
generation helioscope –– IAXO.
Recent findings from ADMX have further
advanced the sensitivity to ALPs. The ADMX Run
1A analysis targeted a specific frequency range (645–
680 MHz), which corresponds to an axion mass range
of 2.66–2.81 μeV, achieving sensitivity at the DFSZ
(Dine-Fischler-Srednicki-Zhitnitsky) level (Boutan et
al., 2023). The experiment did not detect any signals
that would suggest the presence of axions, leading to
exclusion limits on axion-photon couplings at or
below the DFSZ sensitivity, with a confidence level
larger than nine tenth. This effectively excludes
axions as the sole component of dark matter within
the scanned frequency range, assuming a virialization
version of galactic halo model.
Additionally, the recent extended run of CAST,
which included a new Xe-based Micromegas
detector, has set a updated maximum bound on the
axion-photon coupling constant. The new limit here
shows 𝑔

<5.7×10

GeV

at 95% confidence
level (CAST Collaboration et al., 2024), which is the
most stringent experimental limit to date for axion-
photon coupling, particularly in the low-mass range
(for 𝑚
0.02 eV)
With CAST ceasing operations in 2021, these
findings represent the final and most comprehensive
limits from this experiment. The results from this
extended run will remain the most stringent bounds
on solar axions until new data from upcoming
experiments, such as BabyIAXO and IAXO, become
available.
The International Axion Observatory (IAXO) is a
next-generation helioscope experiment designed to
significantly enhance the sensitivity of CAST,
achieving improvements by several orders of
magnitude. It will utilize a much larger magnetic field
volume and advanced X-ray optics to detect ALPs
with greater precision. IAXO is anticipated to provide
new insights into the ALP parameter space,
potentially exploring uncharted regions that could
include ALP dark matter or ALPs linked to other
astrophysical phenomena (Ribas et al., 2015).
Though still in the preparatory phase, IAXO has
been incorporating cutting-edge technologies that are
expected to achieve unparalleled sensitivity to ALPs.
The update highlights the importance of BabyIAXO
in advancing axion research, particularly in the
detection of solar ALPs. BabyIAXO is engineered to
give a significant enhancement on probe’s sensitivity
to axions compared to earlier experiments like CAST.
7.2 Future Prospects and Upcoming
Experiments
Several new experiments are poised to greatly
enhance the search for axion-like particles (ALPs) by
investigating regions of the ALP parameter space that
were previously unexplored.
These efforts aim to identify ALPs across a broad
spectrum of masses and coupling strengths, utilizing
both direct detection methods and astrophysical
observations.
The MADMAX (Magnetized Disk and Mirror
Axion Experiment) project is specifically intended to
detect axions and ALPs within the mass range of
several tens of micro-electronvolts (µeV). This
experiment employs a dielectric haloscope, which
uses a series of dielectric disks placed within a strong
magnetic field to trigger the transformation of ALPs
into detectable photons. This innovative setup
provides a new method for probing ALP dark matter.
Another significant effort is the ALPS II (Any
Light Particle Search II) experiment, an advanced
"light-shining-through-a-wall" setup. It aims to detect
ALPs and other weakly interacting particles with
masses below an electronvolt (sub-eV) by using high-
Axion-Like Particles and Their Cosmological Consequences
327
power lasers and strong magnetic fields to induce
ALP-photon conversion, with the goal of achieving
unprecedented sensitivity to these interactions. If
successful, ALPS II could provide key evidence for
axions or ALPs, which are viewed as promising dark
matter contenders and might also address the strong
CP problem.
Overall, these advancements, together with
improvements to existing detectors like ADMX, are
expected to expand our understanding of ALPs
significantly, potentially uncovering new physics
beyond the Standard Model.
8 CHALLENGES AND OPEN
QUESTIONS
8.1 Theoretical Challenges in ALP
Research
Axion-like particles (ALPs) present a rich field of
study with a wide range of theoretical models, but
these models come with significant uncertainties. One
of the primary challenges is the large parameter space
associated with ALPs, including their masses,
couplings, and potential interactions with standard
model particles.
Theories predicting ALPs often emerge from
frameworks like string theory or other beyond the
Standard Model (BSM) physics, leading to a
multitude of possible ALP properties. These
uncertainties complicate efforts to make precise
predictions about ALP behaviours in various
contexts, such as their potential role in dark matter,
dark energy, or their interaction coupling with
photons, nucleons, or other particles. Moreover,
different ALP models can predict vastly different
cosmological and astrophysical phenomena, making
it difficult to design experiments that can
comprehensively test for ALPs.
Given the broad range of possible ALP properties,
there is a pressing need for more precise theoretical
predictions to guide experimental searches. This
requires a better understanding of the underlying
physics that governs ALP interactions and how these
interactions might manifest in observable
phenomena. Since adding all these theoretical
assumptions increase the complexity of the whole
experimental system; thus, it is needed to be selected
carefully for parameters within the theory.
Additionally, advances in computational techniques
and simulations could provide more accurate
predictions of ALP behavior under different
conditions, helping to narrow down the parameter
space and identify the most promising regions for
experimental exploration.
8.2 Observational Challenges in ALP
Research
Current observational techniques for detecting axion-
like particles (ALPs) face challenges, primarily due
to the weak interactions that ALPs are hypothesized
to have with standard model particles. This makes
them incredibly difficult to detect, requiring
extremely sensitive instruments and often relying on
indirect methods.
The main limitation of current detectors, such as
those used in haloscope experiments like ADMX, is
their sensitivity. These detectors must be capable of
detecting extremely faint signals generated by the
conversion of ALPs into photons, a process that is
expected to occur at very low rates, making
distinguishing a potential ALP signal from
background noise very difficult.
Advances in superconducting technologies, such
as the development of quantum amplifiers, could
significantly enhance the sensitivity of detectors used
in haloscope experiments. These amplifiers can
reduce noise levels and increase the signal-to-noise
ratio, making it easier to detect faint ALP signals.
9 CONCLUSIONS
This comprehensive study of axion-like particles
(ALPs) delves into their theoretical foundations,
potential cosmological roles, and the current state of
experimental efforts aimed at detecting these elusive
particles. ALPs have emerged as versatile candidates
for various cosmological phenomena, including dark
matter or energy, and the formation of cosmic
structures.
Weak interactions with SM particles and the
broad parameter space they occupy, underlies the
challenge and intrigue of ALPs, making them
significant subjects for both theoretical and
experimental research.
The exploration of ALPs extends well beyond the
search for a single particle; it opens up new avenues
for understanding the fundamental forces and
particles that shape our universe.
If ALPs are detected, they could offer valuable
insights into high-energy physics, thereby not only
advancing our knowledge of physics beyond the SM
but also providing explanations for dark matter,
contributing to our current knowledge of cosmic
IAMPA 2024 - International Conference on Innovations in Applied Mathematics, Physics and Astronomy
328
structure formation, also influencing the evolution of
dark energy.
Their potential to address significant problems in
both particle physics and cosmology highlights their
importance in these fields.
Ongoing research into ALPs is essential for
advancing our understanding of the universe. As
experimental techniques improve and new theoretical
models are developed, the chances of discovering
ALPs increase. Future experiments like ADMX,
CAST, IAXO, MADMAX, and ALPS II, along with
simulations that bridge particle physics theory and
cosmological observations, will play a critical role in
this pursuit. The implications of ALP research are
profound, with the potential to reshape our
comprehension of the universe and the fundamental
principles that underlie its workings.
Given the challenges and high stakes involved,
ALP research stands at an exciting frontier, promising
insights that could have far-reaching consequences
for both physics and cosmology.
REFERENCES
Saikawa, K. I., 2017. A review of gravitational waves from
cosmic domain walls. Universe, 3(2), 40.
Chang, S., Hagmann, C., & Sikivie, P., 1998. Studies of the
motion and decay of axion walls bounded by strings.
Physical Review D, 59(2), 023505.
Barth, K., Belov, A., Beltran, B., Bräuninger, H., Carmona,
J. M., Collar, J. I., Dafni, T., Davenport, M., Lella, L.
D., Eleftheriadis, C., Englhauser, J., Fanourakis, G.,
Ferrer-Ribas, E., Fischer, H., Franz, J., Friedrich, P.,
Galán, J., García, J. A., Geralis, T., … Zioutas, K.,
2013. CAST constraints on the axion-electron coupling.
Journal of Cosmology and Astroparticle Physics,
2013(05), 010–010.
Boutan, C., LaRoque, B. H., Lentz, E., Oblath, N. S.,
Taubman, M. S., Tedeschi, J., Yang, J., Jones, A. M.,
Braine, T., Crisosto, N., Rosenberg, L. J., Rybka, G.,
Will, D., Zhang, D., Kimes, S., Ottens, R., Bartram, C.,
Bowring, D., Cervantes, R., … Hilton, G. C., 2023.
Axion Dark Matter eXperiment: Run 1A Analysis
Details.
Carenza, P., Lattanzi, M., Mirizzi, A., & Forastieri, F.,
2021. Thermal axions with multi-eV masses are
possible in low-reheating scenarios. Journal of
Cosmology and Astroparticle Physics, 2021(07), 031.
CAST Collaboration, Altenmüller, K., Anastassopoulos,
V., Arguedas-Cuendis, S., Aune, S., Baier, J., Barth, K.,
Bräuninger, H., Cantatore, G., Caspers, F., Castel, J. F.,
Çetin, S. A., Christensen, F., Cogollos, C., Dafni, T.,
Davenport, M., Decker, T. A., Desch, K., Díez-Ibáñez,
D., … Zioutas, K., 2024. A new upper limit on the
axion-photon coupling with an extended CAST run with
a Xe-based Micromegas detector.
Chatrchyan, A., Eröncel, C., Koschnitzke, M., & Servant,
G., 2024. Gravitational signatures of ALP dark matter
fragmentation. Proceedings of The European Physical
Society Conference on High Energy Physics —
PoS(EPS-HEP2023), 116.
Hooper, D., & Serpico, P. D., 2007. Detecting Axion-Like
Particles With Gamma Ray Telescopes. Physical
Review Letters, 99(23), 231102.
Ivanov, M. M., McDonough, E., Hill, J. C., Simonović, M.,
Toomey, M. W., Alexander, S., & Zaldarriaga, M.,
2020. Constraining Early Dark Energy with Large-
Scale Structure. Physical Review D, 102(10), 103502.
Khatiwada, R., Bowring, D., Chou, A. S., Sonnenschein,
A., Wester, W., Mitchell, D. V., Braine, T., Bartram, C.,
Cervantes, R., Crisosto, N., Du, N., Kimes, S.,
Rosenberg, L. J., Rybka, G., Yang, J., Will, D., Carosi,
G., Woollett, N., Durham, S., … Hilton, G. C., 2021.
Axion Dark Matter eXperiment: Detailed Design and
Operations. Review of Scientific Instruments, 92(12),
124502.
Millea, M., Knox, L., & Fields, B. D., 2015. New bounds
for axions and axion-like particles with keV-GeV
masses. Physical Review D,
92(2), 023010.
Ribas, E. F., Armengaud, E., Avignone, F. T., Betz, M.,
Brax, P., Brun, P., Cantatore, G., Carmona, J. M.,
Carosi, G. P., Caspers, F., Caspi, S., Cetin, S. A.,
Chelouche, D., Christensen, F. E., Dael, A., Dafni, T.,
Davenport, M., Derbin, A. V., Desch, K., … Zioutas,
K., 2015. The IAXO Helioscope. Journal of Physics:
Conference Series, 650, 012009.
Ruchika, Adil, S. A., Dutta, K., Mukherjee, A., & Sen, A.
A., 2023. Observational constraints on axion(s) dark
energy with a cosmological constant. Physics of the
Dark Universe, 40, 101199.
Shen, X., Borrow, J., Vogelsberger, M., Garaldi, E., Smith,
A., Kannan, R., Tacchella, S., Zavala, J., Hernquist, L.,
Yeh, J. Y.-C., & Zheng, C., 2023. THESAN-HR:
Galaxies in the Epoch of Reionization in warm dark
matter, fuzzy dark matter and interacting dark matter.
Zhang, H.-Y., Hagimoto, R., & Long, A. J., 2024. Neutron
star cooling with lepton-flavor-violating axions.
Physical Review D, 109(10), 103005.
Axion-Like Particles and Their Cosmological Consequences
329