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Massive black holes are key ingredients of the assembly and evolution of cosmic structures. Pulsar Timing Arrays (PTAs) currently provide the only means to observe gravitational radiation from massive black hole binary systems with masses…

Cosmology and Nongalactic Astrophysics · Physics 2010-05-27 A. Sesana , A. Vecchio

Even though the sensitivity of direct dark matter search experiments reach the level about $10^{-45}~{\rm cm}^2$, there is no confident signal of dark matter been observed. We point out that, if dark matter is a vector boson, the null…

High Energy Physics - Phenomenology · Physics 2018-05-09 Chuan-Ren Chen , Yu-Kuang Chu , Ho-Chin Tsai

Ultra-light dark matter may consist of axion-like particles with masses below 10^(-19) eV. Two-photon interactions of these particles affect the polarization of radiation propagating through the dark matter. Coherent oscillations of the…

Cosmology and Nongalactic Astrophysics · Physics 2019-03-04 M. M. Ivanov , Y. Y. Kovalev , M. L. Lister , A. G. Panin , A. B. Pushkarev , T. Savolainen , S. V. Troitsky

The dark-matter candidates of particle physics invariably possess electromagnetic interactions, if only via quantum fluctuations. Taken en masse, dark matter can thus engender an index of refraction which deviates from its vacuum value. Its…

High Energy Physics - Phenomenology · Physics 2014-11-18 S. Gardner , D. C. Latimer

Observations of low-frequency gravitational waves will require the highest possible timing precision from an array of the most spin-stable pulsars. We can improve the sensitivity of a pulsar timing array (PTA) to different…

High Energy Astrophysical Phenomena · Physics 2018-11-28 M. T. Lam

One of the open questions of modern cosmology is the nature and properties of the Dark Matter halo and its substructures. In this work we study the gravitational effect of dark matter substructures on pulsar timing observations. Since…

Cosmology and Nongalactic Astrophysics · Physics 2015-03-18 Shant Baghram , Niayesh Afshordi , Kathryn M. Zurek

In this research we consider a $U(1)_X$ gauge boson acting as a dark matter candidate. The vector dark matter (DM) gets mass when a complex singlet scalar breaks the gauge symmetry spontaneously, adding a second Higgs boson to the spectra.…

High Energy Physics - Phenomenology · Physics 2023-08-15 Amir Amiri , Bastián Díaz Sáez , Karim Ghorbani

The nanohertz gravitational wave background (GWB) is expected to be an aggregate signal of an ensemble of gravitational waves emitted predominantly by a large population of coalescing supermassive black hole binaries in the centres of…

We investigate the capability of pulsar timing arrays (PTAs) as a probe of primordial black holes (PBHs), which might constitute the Galactic dark matter. A PBH passing nearby the Earth or a pulsar gives an impulse acceleration and induces…

Cosmology and Nongalactic Astrophysics · Physics 2015-06-11 Kazumi. Kashiyama , Naoki. Seto

We present the results of the search for an isotropic stochastic gravitational wave background (GWB) at nanohertz frequencies using the second data release of the European Pulsar Timing Array (EPTA) for 25 millisecond pulsars and a…

We study the secular effects that an oscillating background ultralight (fuzzy) cosmological vector field has on the dynamics of binary systems; such effects appear when the field and the binary are in resonance. We first consider the…

Cosmology and Nongalactic Astrophysics · Physics 2018-10-31 Diana López Nacir , Federico R. Urban

Supermassive black hole binary mergers serve as prominent sources of the stochastic gravitational wave background (SGWB), detectable by pulsar timing arrays (PTAs). If dark matter-induced friction is present in the vicinity of these…

High Energy Physics - Phenomenology · Physics 2025-04-29 Pratick Sarkar

Direct detection of low-frequency gravitational waves ($10^{-9} - 10^{-8}$ Hz) is the main goal of pulsar timing array (PTA) projects. One of the main targets for the PTAs is to measure the stochastic background of gravitational waves (GWB)…

In fuzzy dark matter (FDM) cosmologies, the dark matter consists of ultralight bosons ($m\lesssim10^{-20}$ eV). The astrophysically large de Broglie wavelengths of such particles hinder the formation of low-mass dark matter halos. This…

Cosmology and Nongalactic Astrophysics · Physics 2025-02-20 Jackson Sipple , Adam Lidz , Daniel Grin , Guochao Sun

The European Pulsar Timing Array (EPTA) and Indian Pulsar Timing Array (InPTA) collaborations have measured a low-frequency common signal in the combination of their second and first data releases respectively, with the correlation…

Cosmology and Nongalactic Astrophysics · Physics 2024-05-17 J. Antoniadis , P. Arumugam , S. Arumugam , P. Auclair , S. Babak , M. Bagchi , A. -S. Bak Nielsen , E. Barausse , C. G. Bassa , A. Bathula , A. Berthereau , M. Bonetti , E. Bortolas , P. R. Brook , M. Burgay , R. N. Caballero , C. Caprini , A. Chalumeau , D. J. Champion , S. Chanlaridis , S. Chen , I. Cognard , M. Crisostomi , S. Dandapat , D. Deb , S. Desai , G. Desvignes , N. Dhanda-Batra , C. Dwivedi , M. Falxa , F. Fastidio , R. D. Ferdman , A. Franchini , J. R. Gair , B. Goncharov , A. Gopakumar , E. Graikou , J. -M. Grießmeier , A. Gualandris , L. Guillemot , Y. J. Guo , Y. Gupta , S. Hisano , H. Hu , F. Iraci , D. Izquierdo-Villalba , J. Jang , J. Jawor , G. H. Janssen , A. Jessner , B. C. Joshi , F. Kareem , R. Karuppusamy , E. F. Keane , M. J. Keith , D. Kharbanda , T. Khizriev , T. Kikunaga , N. Kolhe , M. Kramer , M. A. Krishnakumar , K. Lackeos , K. J. Lee , K. Liu , Y. Liu , A. G. Lyne , J. W. McKee , Y. Maan , R. A. Main , M. B. Mickaliger , H. Middleton , A. Neronov , I. C. Nitu , K. Nobleson , A. K. Paladi , A. Parthasarathy , B. B. P. Perera , D. Perrodin , A. Petiteau , N. K. Porayko , A. Possenti , T. Prabu , K. Postnov , H. Quelquejay Leclere , P. Rana , A. Roper Pol , A. Samajdar , S. A. Sanidas , D. Semikoz , A. Sesana , G. Shaifullah , J. Singha , C. Smarra , L. Speri , R. Spiewak , A. Srivastava , B. W. Stappers , D. A. Steer , M. Surnis , S. C. Susarla , A. Susobhanan , K. Takahashi , P. Tarafdar , G. Theureau , C. Tiburzi , R. J. Truant , E. van der Wateren , S. Valtolina , A. Vecchio , V. Venkatraman Krishnan , J. P. W. Verbiest , J. Wang , L. Wang , Z. Wu

The first direct detection of gravitational waves may be made through observations of pulsars. The principal aim of pulsar timing array projects being carried out worldwide is to detect ultra-low frequency gravitational waves (f ~ 10^-9 to…

In this work we consider a dark matter candidate described by an ultralight vector field, whose mass is in principle in the range $H_{\rm{eq}}\sim 10^{-28}\rm{eV}\ll m< \rm{eV}$. The homogeneous background vector field is assumed to point…

Cosmology and Nongalactic Astrophysics · Physics 2025-05-22 Tomás Ferreira Chase , Matías Leizerovich , Diana López Nacir , Susana Landau

Ultra-light bosons, naturally appearing in well-motivated extensions to the Standard Model, can constitute all the dark matter. Models with particle mass close to the smallest phenomenologically allowed exhibit coherent field configurations…

High Energy Physics - Phenomenology · Physics 2025-07-11 Diego Blas , Silvia Gasparotto , Rodrigo Vicente

We search for ultra-light axions as dark matter (DM) and dark energy particle candidates, for axion masses $10^{-32}\,\mathrm{eV} \leq m_\mathrm{a} \leq 10^{-24}\,\mathrm{eV}$, by a joint analysis of cosmic microwave background (CMB) and…

Cosmology and Nongalactic Astrophysics · Physics 2023-06-21 Keir K. Rogers , Renée Hložek , Alex Laguë , Mikhail M. Ivanov , Oliver H. E. Philcox , Giovanni Cabass , Kazuyuki Akitsu , David J. E. Marsh

The fuzzy dark matter (FDM) model treats DM as a bosonic field with astrophysically large de Broglie wavelength. A striking feature of this model is $\mathcal{O}(1)$ fluctuations in the dark matter density on time scales which are shorter…

Cosmology and Nongalactic Astrophysics · Physics 2019-08-07 David J. E. Marsh , Jens C. Niemeyer
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