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Related papers: Cosmological constraints on ultra-light axion fiel…

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Axion-like particles (ALPs) can oscillate to photons and vice versa in electromagnetic fields. The photon-ALP oscillation provides an attractive solution to the apparent transparency of the Universe to TeV photons. The allowed parameter…

High Energy Physics - Phenomenology · Physics 2019-06-26 Yun-Feng Liang , Cun Zhang , Zi-Qing Xia , Lei Feng , Qiang Yuan , Yi-Zhong Fan

As one of the fundamental unknowns of our Universe, the mass of dark matter remains to be a topic of great interest. We consider the possibility of a time-variation of the dark matter mass. We study the cosmological constraints on a model…

Cosmology and Nongalactic Astrophysics · Physics 2025-04-01 Amlan Chakraborty , Anirban Das , Subinoy Das , Shiv K. Sethi

We study cosmological solutions of (pseudo)scalar theories with periodic potentials, in the presence of arbitrary cosmological fluids -- including a cosmological constant of either sign. Independently of the initial misalignment angle and…

Cosmology and Nongalactic Astrophysics · Physics 2026-04-13 Gary Shiu , Flavio Tonioni , Hung V. Tran

We present a realistic scenario of tracking of scalar fields with varying equation of state. The astrophysical constraints on the evolution of scalar fields in the physical universe are discussed. The nucleosynthesis and the galaxy…

Astrophysics · Physics 2011-07-19 Vinod B. Johri

Scenarios with axion-like particles of variable masses, from the milli-eV range to ultralight, can be generated in a natural way in the context of effective field theory models with anomalous $U(1)$ gauge symmetries. They include…

High Energy Physics - Phenomenology · Physics 2020-05-06 Claudio Corianò , Matteo Maria Maglio , Alessandro Tatullo , Dimosthenis Theofilopoulos

The mass of ultralight axions is determined in order to get the explicit U(1)$_A$ symmetry breaking scale $ \Lambda $ at a Peccei-Quinn scale of the magnitude of the Planck mass. It is assumed that the dominant contribution to the mass of a…

High Energy Physics - Phenomenology · Physics 2021-08-06 Janning Meinert

Recent DESI results indicate a strong preference for dynamical dark energy (DE) when baryon acoustic oscillation (BAO) measurements are combined with supernovae (SNe) and cosmic microwave background (CMB) data using the…

Cosmology and Nongalactic Astrophysics · Physics 2026-01-26 Shubham Barua , Shantanu Desai

If axions exist, they are copiously produced in hot and dense plasmas, carrying away energy directly from the interior of stars. Various astronomical observables constrain the operation of such anomalous stellar energy-loss channels and…

High Energy Physics - Phenomenology · Physics 2009-10-31 G. Raffelt

New light particles produced in supernovae can lead to additional energy loss and a consequent deficit in neutrino production in conflict with the neutrinos observed from Supernova 1987A (SN1987A). Contrary to the majority of previous…

High Energy Physics - Phenomenology · Physics 2021-02-03 Djuna Croon , Gilly Elor , Rebecca K. Leane , Samuel D. McDermott

Ultra-light dark matter (ULDM) is currently one of the most popular classes of cosmological dark matter. The most important advantage is that ULDM with mass $m \sim 10^{-22}$ eV can account for the small-scale problems encountered in the…

Astrophysics of Galaxies · Physics 2021-09-27 Man Ho Chan , Chu Fai Yeung

Cosmological variation of the fine structure constant $\alpha$ due to the evolution of a spatially homogeneous ultra-light scalar field ($m \sim H_0$) during the matter and $\Lambda$ dominated eras is analyzed. Agreement of $\Delta…

Astrophysics · Physics 2009-11-07 Carl L. Gardner

The highly populated, low-energy excitations of a scalar field of mass $m_a\sim 10^{-22}\,\textrm{eV}$ can represent the full dark matter content of the universe and alleviate some tensions in the standard cosmological scenario on…

High Energy Physics - Phenomenology · Physics 2017-02-08 Alberto Diez-Tejedor , David J. E. Marsh

The natural environment of the Earth can act as a sensitive detector for dark matter in ultralight axions. When axions with masses between $1\times10^{-15}\,{\rm eV}$ and $1\times10^{-13}\,{\rm eV}$ pass through the Earth, they interact…

High Energy Physics - Phenomenology · Physics 2025-04-23 Atsushi Nishizawa , Atsushi Taruya , Yoshiaki Himemoto

Most ultraluminous X-ray sources (ULXs) display a typical set of properties not seen in Galactic stellar-mass black holes (BHs): higher luminosity Lx > 3 10^39 erg/s, unusually soft X-ray components (kT < 0.3 keV) and a characteristic…

High Energy Astrophysical Phenomena · Physics 2015-06-23 C. Motch , M. W. Pakull , R. Soria , F. Grisé , G. Pietrzyński

We consider a very simple toy model for a spatially varying `cosmological constant', where we are inside a spherical bubble (with a given set of cosmological parameters) that is surrounded by a larger region where these parameters are…

Astrophysics · Physics 2009-11-06 P. P. Avelino , J. P. M. de Carvalho , C. J. A. P. Martins

Dark matter is poorly constrained by direct detection experiments at masses below 1 MeV. This is an important target for the next generation of experiments, and several methods have been proposed to probe this mass range. One class of such…

High Energy Physics - Phenomenology · Physics 2020-07-31 Benjamin V. Lehmann , Stefano Profumo

The combination of multiple observational probes has long been advocated as a powerful technique to constrain cosmological parameters, in particular dark energy. The Dark Energy Survey has measured 207 spectroscopically--confirmed Type Ia…

Cosmology and Nongalactic Astrophysics · Physics 2019-05-07 DES Collaboration , T. M. C. Abbott , A. Alarcon , S. Allam , P. Andersen , F. Andrade-Oliveira , J. Annis , J. Asorey , A. Avelino , S. Avila , D. Bacon , N. Banik , B. A. Bassett , E. Baxter , K. Bechtol , M. R. Becker , G. M. Bernstein , E. Bertin , J. Blazek , S. L. Bridle , D. Brooks , D. Brout , D. L. Burke , J. Calcino , H. Camacho , A. Campos , A. Carnero Rosell , D. Carollo , M. Carrasco Kind , J. Carretero , F. J. Castander , R. Cawthon , P. Challis , K. C. Chan , C. Chang , M. Childress , A. Clocchiatti , M. Crocce , C. E. Cunha , C. B. D'Andrea , L. N. da Costa , C. Davis , T. M. Davis , J. De Vicente , D. L. DePoy , J. DeRose , S. Desai , H. T. Diehl , J. P. Dietrich , S. Dodelson , P. Doel , A. Drlica-Wagner , T. F. Eifler , J. Elvin-Poole , J. Estrada , A. E. Evrard , E. Fernandez , A. V. Filippenko , B. Flaugher , R. J. Foley , P. Fosalba , J. Frieman , L. Galbany , J. García-Bellido , M. Gatti , E. Gaztanaga , D. W. Gerdes , T. Giannantonio , K. Glazebrook , D. A. Goldstein , D. Gruen , R. A. Gruendl , J. Gschwend , G. Gutierrez , W. G. Hartley , S. R. Hinton , D. L. Hollowood , K. Honscheid , J. K. Hoormann , B. Hoyle , D. Huterer , B. Jain , D. J. James , M. Jarvis , T. Jeltema , E. Kasai , S. Kent , R. Kessler , A. G. Kim , R. P. Kirshner , N. Kokron , E. Krause , R. Kron , K. Kuehn , N. Kuropatkin , O. Lahav , J. Lasker , P. Lemos , G. F. Lewis , T. S. Li , C. Lidman , M. Lima , H. Lin , E. Macaulay , N. MacCrann , M. A. G. Maia , K. S. Mandel , M. March , J. Marriner , J. L. Marshall , P. Martini , R. G. McMahon , P. Melchior , F. Menanteau , R. Miquel , J. J. Mohr , E. Morganson , J. Muir , A. Möller , E. Neilsen , R. C. Nichol , B. Nord , R. L. C. Ogando , A. Palmese , Y. -C. Pan , H. V. Peiris , W. J. Percival , A. A. Plazas , A. Porredon , J. Prat , A. K. Romer , A. Roodman , R. Rosenfeld , A. J. Ross , E. S. Rykoff , S. Samuroff , C. Sánchez , E. Sanchez , V. Scarpine , R. Schindler , M. Schubnell , D. Scolnic , L. F. Secco , S. Serrano , I. Sevilla-Noarbe , R. Sharp , E. Sheldon , M. Smith , M. Soares-Santos , F. Sobreira , N. E. Sommer , E. Swann , M. E. C. Swanson , G. Tarle , D. Thomas , R. C. Thomas , M. A. Troxel , B. E. Tucker , S. A. Uddin , P. Vielzeuf , A. R. Walker , M. Wang , N. Weaverdyck , R. H. Wechsler , J. Weller , B. Yanny , B. Zhang , Y. Zhang , J. Zuntz

The sum of cosmic neutrino masses can be measured cosmologically, as the sub-eV particles behave as `hot' dark matter whose main effect is to suppress the clustering of matter compared to a universe with the same amount of purely cold dark…

Cosmology and Nongalactic Astrophysics · Physics 2024-09-05 Helen Shao , Jahmour J. Givans , Jo Dunkley , Mathew Madhavacheril , Frank Qu , Gerrit Farren , Blake Sherwin

Assuming the standard cosmological model as correct, the average linear size of galaxies with the same luminosity is six times smaller at z=3.2 than at z=0, and their average angular size for a given luminosity is approximately proportional…

Cosmology and Nongalactic Astrophysics · Physics 2015-05-18 Martin Lopez-Corredoira

It has been recently suggested by Dvali and Vikman that the superluminal neutrino phenomenology of the OPERA experiment may be due to an environmental feature of the Earth, naturally yielding a long-range fifth force of gravitational origin…

General Relativity and Quantum Cosmology · Physics 2015-03-19 Lorenzo Iorio