arXiv subjects

Rachid Ouyed

Publications and source records attributed to Rachid Ouyed.

At least 19 recordsLinked to original sources

arXiv2026

Beyond Spin: QCD Magnetars

We present a unified framework in which anomalous X-ray pulsars (AXPs), soft gamma-ray repeaters (SGRs), superluminous supernovae (SLSNe-I), luminous fast blue optical transients (LFBOTs), and fast radio bursts (FRBs) originate from quark deconfinement in the core of a massive neutron star (NS). Spontaneous ferromagnetism in the deconfined phase generates ~10^18 G core fields, producing a highly magnetized hybrid star (HS) - the "QCD magnetar" - whose surface field is set by NS mass, not birth spin. The Quark-Nova (QN) that forms the HS ejects ~0.01M_sun of neutron-rich outer layers, powering a kilonova and leaving the HS crustless for centuries. During this phase, magnetic instabilities at the hadron-quark interface release rising flux ropes that power X-ray-quiet FRBs; as the crust reforms, the source evolves into an X-ray-loud AXP&SGR. Two parameters govern the model: a critical mass M_dec triggering deconfinement, and a critical period P_fast separating fast and slow rotators. Fast rotators inject spin-down energy into the QN ejecta, producing an LFBOT - directly observable once the SN ejecta is optically thin, or via binary accretion with no preceding SN; otherwise the LFBOT is reprocessed by the SN ejecta into an SLSN-I. A Bayesian Monte Carlo population synthesis reproduces the observed rates of AXPs&SGRs, SLSNe-I, and LFBOTs with M_dec ~2.1M_sun and P_fast ~5.5 ms, and predicts non-merger r-process signatures and kilonovae from isolated NSs, with or without an LFBOT. The QN ejecta also carries its own DM and RM, independent of environment, predicted to appear as excess dispersion and rotation measure in FRBs once Galactic, host, and intergalactic contributions are removed. These provide direct observational tests of the hadron-quark phase transition and ferromagnetic ordering in dense quark matter.

astro-ph.HE↗

arXiv2026

Optical Flares in the Luminous Fast Blue Optical Transient AT2022tsd ("Tasmanian Devil")

We propose that luminous fast blue optical transients (LFBOTs) signal the delayed conversion of a massive neutron star (NS; M_NS > ~1.8 Msun) into a highly magnetized hybrid star (HS) with B_HS ~10^15 G surface field; a QCD magnetar. This is the partial conversion channel in the Quark-Nona (QN) model where the core of the NS enters a quark phase with spontaneous generation of extreme (i.e., up to > 10^18 G) magnetic field independent of the NS spin. The process ejects ~0.01 Msun of the NS outermost layers at ~0.1c (the QN ejecta) with a photon diffusion timescale of a few days. The powering of the QN ejecta by spin-down of a rapidly rotating HS (inherited from the parent NS) yields the LFBOT. The fragmentation of the QN ejecta allows optical flares to arise from clumps that become optically thin, releasing stored radiation energy (with luminosities comparable to the LFBOT peak) on light-crossing timescales of tens of minutes. X-rays from the relativistic HS spin-down wind escaping through optically thin gaps in the QN ejecta, and radio from QN ejecta-medium interaction arise self-consistently from a single physical engine. This framework reproduces key features of AT2022tsd, AT2020xnd, AT2020mrf, and AT2018cow. The neutron-rich, r-process-producing QN ejecta predicts kilonova-like emission associated with LFBOTs in environments that do not host neutron star mergers.

astro-ph.HE↗

arXiv2026

Late-Onset Energy Injection in Type Ic SNe and W-Shaped O II Absorption in SLSNe-I

We show that delayed (weeks-months) energy injection into expanding Type Ic supernova (SN) ejecta can reproduce the luminosity and spectral evolution of hydrogen-poor superluminous SNe (SLSNe-I). Late-time reheating sets the radiation temperature and density needed for the W-shaped OII absorption near peak, explaining its disappearance as the ejecta cools without extra excitation mechanisms. In our model, the neutron star (NS) undergoes a core phase transition to deconfined quark matter at time t_QN, triggering rapid magnetic field amplification and forming a hybrid star (HS; a QCD-magnetar). This Quark-Nova (QN) resets the central engine, weeks to months after the SN, by converting the NS rotational energy into renewed energy injection, producing two powering epochs separated by a delay determined by hadron-to-quark microphysics. The model reproduces photometric and spectroscopic evolution of SLSNe-I such as iPTF13ajg, SN2010gx, PTF09cnd, and PTF09atu. We predict a systematic offset between spectroscopic and photometric ages when pre-QN emission is below detection limits, and discuss observational signatures distinguishing QCD-magnetars from standard magnetars. Double-peaked SLSNe-I may probe the hadron-quark transition, constraining quark-matter parameters like deconfinement density and surface tension.

astro-ph.HE↗

arXiv2025

Modeling the Light Curve and Spectra of SN 2023aew

We propose that the delayed conversion of a neutron star (NS) into either a quark star (QS) or a hybrid star (HS), occurring approximately 105-109 days after the supernova (SN) explosion, injects ~ 2e49 erg of thermal energy into the expanded SN ejecta. This energy, delivered over ~ 40 days via a quark-nova (QN) shock or the spin-down power of the HS, can reproduce the photometric and spectral features observed in SN 2023aew. In this model, the first light curve peak corresponds to the 56Ni-powered SN resulting from a stripped-envelope progenitor with a zero-age main sequence mass of at least ~ (15-16)M_sun. The plateau between the two peaks may result from interaction between the SN ejecta and circumstellar material (CSM). Alternatively, it could be explained by the spin-down power of the NS prior to its conversion into a highly magnetized HS, which is responsible for powering the second bump. A scenario involving two phases of spin-down power - first from the NS and later from the HS - is compelling and supports the hypothesis that some magnetars are, in fact, HSs. These HSs acquire their ultra-strong magnetic fields through a quark matter phase capable of sustaining core fields on the order of ~ 1e18 G. In our model, the spin-down energy of the HS powers the QN ejecta - the outermost layers of the NS - before this energy is transferred to the expanded SN ejecta. This process produces luminous fast blue optical transients (LFBOTs). The model establishes a potential connection between superluminous SNe (SLSNe) and LFBOTs, with significant implications for high-energy astrophysics and the r-process nucleosynthesis of heavy elements. Potential consequences for Quantum Chromodynamics (QCD) are also discussed.

astro-ph.HE↗

arXiv2025

The Quark-Nova model for FRBs: model comparison with observational data

We utilize the Quark-Novae (QN) model for Fast Radio Bursts (FRBs; Ouyed et al. 2021; arXiv:2005.09793) to evaluate its performance in reproducing the distribution and statistical properties of key observations. These include frequency, duration, fluence, dispersion measure (DM), and other relevant features such as repetition, periodic activity window, and the sad trombone effect. In our model, FRBs are attributed to coherent synchrotron emission (CSE) originating from collisionless QN chunks that traverse ionized media both within and outside their host galaxies. By considering burst repetition from a single chunk and accounting for the intrinsic DM of the chunks, we find agreement between our model and the observed properties of FRBs. This agreement enhances our confidence in the model's effectiveness for interpreting FRB observations. Our model generates testable predictions, allowing for future experiments and observations to validate and further refine our understanding of FRBs.

astro-ph.HE↗

arXiv2024

Quark clusters, QCD vacuum and the cosmological 7Li, Dark Matter and Dark Energy problems

We propose a non-exotic electromagnetic solution (within the standard model of particle physics) to the cosmological 7Li problem based upon a narrow 2 MeV photo-emission line from the decay of light Glueballs (LGBs). These LGBs form within color superconducting, tens of Fermi in size, quark clusters (SQCs) in the radiation-dominated post-BBN epoch. The mono-chromatic line from the LGB -> gamma+gamma decay reduces Big-Bang nucleosynthesis (BBN) 7Be by 2/3 without affecting other abundances or CMB physics, provided the combined mass of the SQCs is greater than the total baryonic mass in the Universe. Following the LGB emission, the in-SQC Quantum-ChromoDynamics (QCD) vacuum becomes unstable and "leaks" (via quantum tunnelling) into the external space-time (trivial) vacuum inducing a decoupling of SQCs from hadrons. In seeking a solution to the 7Li problem, we uncovered a solution which also addresses the dark energy (DE) and dark matter (DM) problem making these critical problems intertwined in our model. Being colorless, charge neutral, optically thin and transparent to hadrons, SQCs interact only gravitationally making them a viable CDM candidate. The quantum tunnelling of the in-SQC QCD vacuum to the trivial vacuum offers an explanation of DE in our model and allows for a cosmology which evolves into a LambdaCDM universe at low redshift with a possible resolution of the Hubble tension. Our model distinguishes itself by proposing that the QCD vacuum within SQCs possesses the ability to tunnel into the exterior trivial vacuum, resulting in the generation of DE. This implies the possibility that DM and hadrons might represent distinct phases of quark matter within QCD, characterized by different vacuum properties. We discuss SQC formation in heavy-ion collision experiments at moderate temperatures and the possibility of detection of MeV photons from LGB -> gamma+gamma.

astro-ph.CO↗

arXiv2021

Quark-Novae in the outskirts of galaxies: An explanation of the Fast Radio Burst phenomenon

We show that old isolated neutron stars in groups and clusters of galaxies experiencing a Quark-Nova phase (QN: an explosive transition to a quark star) may be the source of FRBs. Each of the millions of fragments of the ultra-relativistic QN ejecta provides a collisionless plasma for which the ambient medium (galactic/halo, the intra-group/intra-cluster medium) acts as a relativistic plasma beam. The Buneman and the Weibel instabilities, successively induced by the beam in the fragment, generate particle bunching and observed coherent emission at GHz frequency with a corresponding fluence in the Jy ms range. The duration, frequency drift and the rate are in agreement with observed properties of FRBs. Repeats (on timescales of minutes to months) are due to seeing multiple fragments each beaming at a different direction and coming in at different times. Single (non-repeating) FRBs, occur when only emission from the primary fragment is within the detector's sensitivity. Key properties of FRB 121102 (its years of activity) and of FRB 180916.J0158+65 (its 16 day period) are recovered. The spatial and temporal coincidence between SGR 1935+2154 and FRB 200428 finds an explanation in our model. We give testable predictions.

astro-ph.HE↗

arXiv2019

A Quark-Nova in the wake of a core-collapse Supernova: a unifying model for long duration Gamma-Ray Bursts and Fast Radio Bursts

[Abridged] By appealing to a Quark-Nova (QN; the explosive transition of a neutron star to a quark star) in the wake of a core-collapse Supernova explosion of a massive star, we develop a unified model for long duration Gamma-ray Bursts (LGRBs) and Fast Radio Bursts (FRBs). The time delay (years to decades) between the SN and the QN and, the fragmented nature (i.e. millions of chunks) of the relativistic QN ejecta are key to yielding a robust LGRB engine. In our model, a LGRB light-curve exhibits the interaction of the fragmented QN ejecta with a turbulent (i.e. filamentary and magnetically saturated) SN ejecta which is shaped by its interaction with an underlying pulsar wind nebula (PWN). The afterglow is due to the interaction of the QN chunks, exiting the SN ejecta, with the surrounding medium. Our model can fit BAT/XRT prompt and afterglow light-curves, simultaneously with their spectra, thus yielding the observed properties of LGRBs (e.g. the Band function and the X-ray flares). We find that the Yonetoku law and the Amati law are not fundamental but phenomenological. FRBs result from coherent synchrotron emission when the QN chunks interact with non-turbulent weakly magnetized PWN-SN ejecta, where conditions are prone to the Weibel instability. Magnetic field amplification induced by the Weibel instability sets the bunching length for electrons and pairs to radiate coherently. The resulting emission frequency, luminosity, duration and dispersion measure in our model are consistent with FRB data. We find a natural unification of high-energy burst phenomena from FRBs to LGRBs including X-ray Flashes and X-ray rich GRBs as well as Super-Luminous SNe. We find a possible connection between Ultra-High Energy Cosmic Rays and FRBs and propose that a QN following a binary neutron star merger can yield a short GRB (SGRB) with fits to BAT/XRT light-curves.

astro-ph.HE↗

arXiv2019

The Structure of the Hadron-Quark Reaction Zone

Hadron-quark combustion in dense matter is a central topic in the study of phases in compact stars and their high-energy astrophysics. We critically review the literature on hadron-quark combustion, dividing them into a "first wave" that treats the problem as a steady-state burning with or without constraints of mechanical equilibrium, and a "second wave" which uses numerical techniques to resolve the burning front and solves the underlying Partial Differential Equations for the chemistry of the burning front under less restrictive conditions. We detail the inaccuracies that the second wave amends over the first wave, and highlight crucial differences between various approaches in the second wave. We also include results from time-dependent simulations of the reaction zone that include a hadronic EOS, neutrinos, and self-consistent thermodynamics without using parameterized shortcuts.

nucl-th↗

arXiv2018

Hadron-Quark Combustion as a Nonlinear, Dynamical System

The hadron-quark combustion front is a system that couples various processes, such as chemical reactions, hydrodynamics, diffusion, and neutrino transport. Previous numerical work has shown that this system is very nonlinear, and can be very sensitive to some of these processes. In these proceedings, we contextualize the hadron-quark combustion as a nonlinear system, subject to dramatic feedback triggered by leptonic weak decays and neutrino transport.

nucl-th↗

arXiv2017

Numerical Simulation of the Hydrodynamical Combustion to Strange Quark Matter in the Trapped Neutrino Regime

We simulate and study the microphysics of combustion (flame burning) of two flavored quark matter (u, d) to three flavoured quark matter (u,d,s) in a trapped neutrino regime applicable to conditions prevailing in a hot proto-neutron star. The reaction-diffusion-advection equations for (u,d) to (u,d,s) combustion are coupled with neutrino transport, which is modelled through a flux-limited diffusion scheme. The flame speed is proportional to initial lepton fraction because of the release of electron chemical potential as heat, and reaches a steady-state burning speed of (0.001-0.008)c. We find that the burning speed is ultimately driven by the neutrino pressure gradient, given that the pressure gradient induced by quarks is opposed by the pressure gradients induced by electrons. This suggests, somewhat counter-intuitively, that the pressure gradients that drive the interface are controlled primarily by leptonic weak decays rather than by the quark Equation of State (EOS). In other words, the effects of the leptonic weak interaction, including the corresponding weak decay rates and the EOS of electrons and neutrinos, are at least as important as the uncertainties related to the EOS of high density matter. We find that for baryon number densities nB <= 0.35 fm-3, strong pressure gradients induced by leptonic weak decays drastically slow down the burning speed, which is thereafter controlled by the much slower burning process driven by backflowing downstream matter. We discuss the implications of our findings to proto-neutron stars.

nucl-th↗

arXiv2017

Critical assessment of nuclear sensitivity metrics for the r-process

Any simulation of the r-process is affected by uncertainties in our present knowledge of nuclear physics quantities and astrophysical conditions. It is common to quantify the impact of these uncertainties through a global sensitivity metric, which is then used to identify specific nuclides that would be most worthwhile to measure experimentally. Using descriptive statistics, we assess a set of metrics used in previous sensitivity studies, as well as a new logarithmic measure. For certain neutron-rich nuclides lying near the r-process path for the typical hot-wind scenario, we find opposing conclusions on their relative sensitivity implied by different metrics, although they all generally agree which ones are the most sensitive nuclei. The underlying reason is that sensitivity metrics which simply sum over variations in the r-process distribution depend on the scaling used in the baseline, which often varies between simulations. We show that normalization of the abundances causes changes in the reported sensitivity factors and recommend reporting a minimized F statistic in addition to a scale estimation for rough calibration to be used when comparing tables of sensitivity factors from different studies.

astro-ph.HE↗

arXiv2016

The Superluminous (Type I) Supernova ASASSN-15lh : A case for a Quark-Nova inside an Oxygen-type Wolf-Rayet supernova remnant

We show that a Quark-Nova (QN; the explosive transition of a neutron star to a quark star) occurring a few days following the supernova explosion of an Oxygen-type Wolf-Rayet (WO) star can account for the intriguing features of ASASSN-15lh, including its extreme energetics, its double-peaked light-curve and the evolution of its photospheric radius and temperature. A two-component configuration of the homologously expanding WO remnant (an extended envelope and a compact core) is used to harness the kinetic energy (>10^52 ergs) of the QN ejecta. The delay between the WO SN and the QN yields a large (~ 10^4 Rsun) envelope which when energized by the QN ejecta/shock gives the first peak in our model. As the envelope's photosphere recedes into the slowly expanding, hot and insulated, denser core (initially heated by the QN shock) a second hump emerges. The spectrum in our model should reflect the composition of an WO SN remnant re-heated by a QN going off in its wake.

astro-ph.HE↗

arXiv2016

Nuclear fusion in the deuterated cores of inflated hot Jupiters

Ouyed et al. (1998) proposed Deuterium (DD) fusion at the core-mantle interface of giant planets as a mechanism to explain their observed heat excess. But rather high interior temperatures (~10^5 K) and a stratified D layer are needed, making such a scenario unlikely. In this paper, we re-examine DD fusion, with the addition of screening effects pertinent to a deuterated core containing ice and some heavy elements. This alleviates the extreme temperature constraint and removes the requirement of a stratified D layer. As an application, we propose that, if their core temperatures are a few times 10^4 K and core composition is chemically inhomogeneous, the observed inflated size of some giant exoplanets ("hot Jupiters") may be linked to screened DD fusion occurring deep in the interior. Application of an analytic evolution model suggests that the amount of inflation from this effect can be important if there is sufficient rock-ice in the core, making DD fusion an effective extra internal energy source for radius inflation. The mechanism of screened DD fusion, operating in the above temperature range, is generally consistent with the trend in radius anomaly with planetary equilibrium temperature $T_{\rm eq}$, and also depends on planetary mass. Although we do not consider the effect of incident stellar flux, we expect that a minimum level of irradiation is necessary to trigger core erosion and subsequent DD fusion inside the planet. Since DD fusion is quite sensitive to the screening potential inferred from laboratory experiments, observations of inflated hot Jupiters may help constrain screening effects in the cores of giant planets.

astro-ph.EP↗

arXiv2016

Quark-Noave in binaries: Observational signatures and implications to astrophysics

The explosive transition of a massive neutron star to a quark star (the Quark-Nova, QN) releases in excess of ~ 10^52 erg in kinetic energy which can drastically impact the surrounding environment of the QN. A QN is triggered when a neutron star gains enough mass to reach the critical value for quark deconfinement to happen in the core. In binaries, a neutron star has access to mass reservoirs (e.g. accretion from a companion or from a Common Envelope, CE). We explain observed light-curves of hydrogen-poor superluminous Supernovae (SLSNe Ia) in the context of a QN occurring in the second CE phase of a massive binary. In particular this model gives good fits to light-curves of SLSNe with double-humped light-curves. Our model suggests the QN as a mechanism for CE ejection and that they be taken into account during binary evolution. In a short period binary with a white dwarf companion, the neutron star can quickly grow in mass and experience a QN event. Part of the QN ejecta collides with the white dwarf, shocking, compressing, and heating it to driving a thermonuclear runaway producing a SN Ia impostor (a QN-Ia). Unlike "normal" Type Ia supernovae where no compact remnant is formed, a QN-Ia produces a quark star undergoing rapid spin-down providing additional power along with the 56Ni decay energy. Type Ia SNe are used as standard candles and contamination of this data by QNe-Ia can infer an incorrect cosmology.

astro-ph.HE↗

arXiv2016

Quark-nova compact remnants: Observational signatures in astronomical data and implications to compact stars

Quark-novae leave behind quark stars with a surrounding metal-rich fall-back (ring-like) material. These compact remnants have high magnetic fields and are misconstrued as magnetars; however, several observational features allow us to distinguish a quark star (left behind by a quark-nova) from a neutron star with high magnetic field. In our model, bursting activity is expected from intermittent accretion events from the surrounding fall-back debris leading to X-ray bursts (in the case of a Keplerian ring) or gamma ray bursts (in the case of a co-rotating shell). The details of the spectra are described by a constant background X-ray luminosity from the expulsion of magnetic flux tubes which will be temporarily buried by bursting events caused by accretion of material onto the quark star surface. These accretion events emit high energy photons and heat up the quark star and surrounding debris leading to hot spots which may be observable as distinct blackbodies. Additionally, we explain observed spectral line features as atomic lines from r-process material and explain an observed anti-glitch in an AXP as the transfer of angular momentum from a surrounding Keplerian disk to the quark star.

astro-ph.HE↗

arXiv2016

Quark-Novae occurring in massive binaries : A universal energy source in superluminous Supernovae with double-peaked light curves

A Quark-Nova (QN, the sudden transition from a neutron star into a quark star) which occurs in the second common envelope (CE) phase of a massive binary (Ouyed et al., 2015a&b), gives excellent fits to super-luminous, hydrogen-poor, Supernovae (SLSNe) with double-peaked light curves including DES13S2cmm, SN 2006oz and LSQ14bdq (http://www.quarknova.ca/LCGallery.html). In our model, the H envelope of the less massive companion is ejected during the first CE phase while the QN occurs deep inside the second, He-rich, CE phase after the CE has expanded in size to a radius of a few tens to a few thousands solar radii, this yields the first peak in our model. The ensuing merging of the quark star with the CO core leads to black hole formation and accretion explaining the second long-lasting peak. We study a sample of 8 SLSNe Ic with double-humped light-curves. Our model provides good fits to all of these with a universal explosive energy of 2x10^52 erg (which is the kinetic energy of the QN ejecta) for the first hump. The late-time emissions seen in iPTF13ehe and LSQ14bdq are fit with a shock interaction between the outgoing He-rich (i.e second) CE and the previously ejected H-rich (i.e first) CE.

astro-ph.HE↗

arXiv2016

Quark Nova Model for Fast Radio Bursts

FRBs are puzzling, millisecond, energetic radio transients with no discernible source; observations show no counterparts in other frequency bands. The birth of a quark star from a parent neutron star experiencing a quark nova - previously thought undetectable when born in isolation - provides a natural explanation for the emission characteristics of FRBs. The generation of unstable r-process elements in the quark nova ejecta provides millisecond exponential injection of electrons into the surrounding strong magnetic field at the parent neutron star's light cylinder via $β$-decay. This radio synchrotron emission has a total duration of hundreds of milliseconds and matches the observed spectrum while reducing the inferred dispersion measure by approximately 200 cm$^{-3}$ pc. The model allows indirect measurement of neutron star magnetic fields and periods in addition to providing astronomical measurements of $β$-decay chains of unstable neutron rich nuclei. Using this model, we can calculate expected FRB average energies ($\sim$ 10$^{41}$ ergs), spectra shapes and provide a theoretical framework for determining distances.

astro-ph.HE↗