High Energy Astrophysical Phenomena (astro-ph.HE)
Fri, 30 Jun 2023
1.Modelling repetition in zDM: a single population of repeating fast radio bursts can explain CHIME data
Authors:C. W. James
Abstract: Regardless of whether or not all fast radio bursts (FRBs) repeat, those that do form a population with a distribution of rates. This work considers a power-law model of this population, with rate distribution $\Phi_r \sim R^{\gamma_r}$ between $R_{\rm min}$ and $R_{\rm max}$. The zDM code is used to model the probability of detecting this population as either apparently once-off or repeat events as a function of redshift, $z$, and dispersion measure, DM. I demonstrate that in the nearby Universe, repeating sources can contribute significantly to the total burst rate. This causes an apparent deficit in the total number of observed sources (once-off and repeaters) relative to the distant Universe that will cause a bias in FRB population models. Thus instruments with long exposure times should explicitly take repetition into account when fitting the FRB population. I then fit data from The Canadian Hydrogen Intensity Mapping Experiment (CHIME). The relative number of repeat and apparently once-off FRBs, and their DM, declination, and burst rate distributions, can be well-explained by 50--100\% of CHIME single FRBs being due to repeaters, with $R_{\rm max} > 0.75$ day$^{-1}$ above $10^{39}$ erg, and ${\gamma_r} = -2.2_{-0.8}^{+0.6}$. This result is surprisingly consistent with follow-up studies of FRBs detected by the Australian Square Kilometre Array Pathfinder (ASKAP). Thus the evidence suggests that CHIME and ASKAP view the same repeating FRB population, which is responsible not just for repeating FRBs, but the majority of apparently once-off bursts. For greater quantitative accuracy, non-Poissonian arrival times, second-order effects in the CHIME response, and a simultaneous fit to the total FRB population parameters, should be treated in more detail in future studies.
2.General Physical Properties of Fermi blazars
Authors:Yongyun Chen, Qiusheng Gu, Junhui Fan, Xiaoling Yu, Xiaogu Zhong, Hongyu Liu, Nan Ding, Dingrong Xiong, Xiaotong Guo
Abstract: We study the general physical properties of Fermi blazars using the Fermi fourth source catalog data (4FGL-DR2). The quasi-simultaneous multiwavelength data of Fermi blazar are fitted by using the one-zone leptonic model to obtain some physical parameters, such as jet power, magnetic field and Doppler factor. We study the distributions of the derived physical parameter as a function of black hole mass and accretion disk luminosity. The main results are as follows. (1) For a standard thin accretion disk, the jet kinetic power of most FSRQs can be explained by the BP mechanism. However, the jet kinetic power of most BL Lacs can not be explained by both the BZ mechanism or the BP mechanism. The BL Lacs may have ADAFs surrounding their massive black holes. (2) After excluding the redshift, there is a moderately strong correlation between the jet kinetic power and jet radiation power and the accretion disk luminosity for Fermi blazars. These results confirm a close connection between jet and accretion. The jet kinetic power is slightly larger than the accretion disk luminosity for Fermi blazars. (3) There is a significant correlation between jet kinetic power and gamma-ray luminosity and radio luminosity for Fermi blazars, which suggests that gamma-ray luminosity and radio luminosity can be used to indicate the jet kinetic power.
3.Constraints on thermalizing surfaces from infrared observations of supermassive black holes
Authors:Raúl Carballo-Rubio, Francesco Di Filippo, Stefano Liberati, Matt Visser
Abstract: Infrared observations of Sgr A$^*$ and M87$^*$ are incompatible with the assumption that these sources have physical surfaces in thermal equilibrium with their accreting environments. In this paper we discuss a general parametrization of the energy balance in a horizonless object, which permits to quantify how close a horizonless object is in its behavior to a black hole, and analyze the timescale in which its surface can thermalize. We show that the thermalization timescale is unbounded, growing large for objects that mimic closely the behavior of a black hole (and being infinite for the latter). In particular, the thermalization timescale is proportional to the time that energy spends inside the horizonless object due to propagation and interactions with the bulk. Hence, these observations can be used to quantitatively restrict the dynamical behavior of horizonless objects, without being able to discard the existence of a physical surface.
4.Mass and tidal parameter extraction from gravitational waves of binary neutron stars mergers using deep learning
Authors:Shriya Soma, Horst Stöcker, Kai Zhou
Abstract: Gravitational Waves (GWs) from coalescing binaries carry crucial information about their component sources, like mass, spin and tidal effects. This implies that the analysis of GW signals from binary neutron star mergers can offer unique opportunities to extract information about the tidal properties of NSs, thereby adding constraints to the NS equation of state. In this work, we use Deep Learning (DL) techniques to overcome the computational challenges confronted in conventional methods of matched-filtering and Bayesian analyses for signal-detection and parameter-estimation. We devise a DL approach to classify GW signals from binary black hole and binary neutron star mergers. We further employ DL to analyze simulated GWs from binary neutron star merger events for parameter estimation, in particular, the regression of mass and tidal deformability of the component objects. The results presented in this work demonstrate the promising potential of DL techniques in GW analysis, paving the way for further advancement in this rapidly evolving field. The proposed approach is an efficient alternative to explore the wealth of information contained within GW signals of binary neutron star mergers, which can further help constrain the NS EoS.
5.Influence of Dark Matter on the Magnetized Neutron Star
Authors:Vishal Parmar, H. C. Das, M. K. Sharma, S. K. Patra
Abstract: Over the past two decades, significant strides have been made in the study of Dark Matter (DM) admixed neutron stars and their associated properties. However, an intriguing facet regarding the effect of DM on magnetized neutron stars still remains unexplored. This study is carried out to analyse the properties of DM admixed magnetized neutron stars. The equation of state for the DM admixed neutron star is calculated using the relativistic mean-field model with the inclusion of a density-dependent magnetic field. Several macroscopic properties such as mass, radius, particle fractions, tidal deformability, and the $f$-mode frequency are calculated with different magnetic field strengths and DM configurations. The equation of state is softer with the presence of DM as well as for the parallel components of the magnetic field, and vice-versa for the perpendicular one. Other macroscopic properties, such as mass, radius, tidal deformability, etc., are also affected by both DM and the magnetic fields. The change in the magnitude of different neutron star observables is proportional to the amount of DM percentage and the strength of the magnetic field. We observe that the change is seen mainly in the core part of the star without affecting the crustal properties.
6.A new redback pulsar candidate 4FGL J2054.2+6904
Authors:A. V. Karpova, D. A. Zyuzin, Yu. A. Shibanov, M. R. Gilfanov
Abstract: The Fermi catalogue contains about 2000 unassociated $\gamma$-ray sources. Some of them were recently identified as pulsars, including so called redbacks and black widows, which are millisecond pulsars in tight binary systems with non- and partially-degenerate low-mass stellar companions irradiated by the pulsar wind. We study a likely optical and X-ray counterpart of the Fermi source 4FGL J2054.2+6904 proposed earlier as a pulsar candidate. We use archival optical data as well as Swift/XRT and SRG/eROSITA X-ray data to clarify its nature. Using Zwicky Transient Facility data in $g$ and $r$ bands spanning over 4.7 years, we find a period of $\approx$7.5 h. The folded light curve has a smooth sinusoidal shape with the peak-to-peak amplitude of $\approx$0.4 mag. The spectral fit to the optical spectral energy distribution of the counterpart candidate gives the star radius of 0.5$\pm$0.1$R_\odot$ and temperature of 5500$\pm$300 K implying a G2--G9-type star. Its X-ray spectrum is well fitted by an absorbed power law with the photon index of 1.0$\pm$0.3 and unabsorbed flux of $\approx 2\times10^{-13}$ erg s$^{-1}$ cm$^{-2}$. All the properties of 4FGL J2054.2$+$6904 and its presumed counterpart suggest that it is a member of the redback family.
7.Self-consistent 3D radiative transfer for kilonovae: directional spectra from merger simulations
Authors:Luke J. Shingles, Christine E. Collins, Vimal Vijayan, Andreas Flörs, Oliver Just, Gerrit Leck, Zewei Xiong, Andreas Bauswein, Gabriel Martínez-Pinedo, Stuart A. Sim
Abstract: We present three-dimensional radiative transfer calculations for the ejecta from a neutron star merger that include line-by-line opacities for tens of millions of bound-bound transitions, composition from an r-process nuclear network, and time-dependent thermalization of decay products from individual $\alpha$ and $\beta^-$ decay reactions. In contrast to expansion opacities and other wavelength-binned treatments, a line-by-line treatment enables us include fluorescence effects and associate spectral features with the emitting and absorbing lines of individual elements. We find variations in the synthetic observables with both the polar and azimuthal viewing angles. The spectra exhibit blended features with strong interactions by Ce III, Sr II, Y II, and Zr II that vary with time and viewing direction. We demonstrate the importance of wavelength-calibration of atomic data using a model with calibrated Sr, Y, and Zr data, and find major differences in the resulting spectra, including a better agreement with AT2017gfo. The synthetic spectra for near-polar inclination show a feature at around 8000 A, similar to AT2017gfo. However, they evolve on a more rapid timescale, likely due to the low ejecta mass (0.005 M$_\odot$) as we take into account only the early ejecta. The comparatively featureless spectra for equatorial observers gives a tentative prediction that future observations of edge-on kilonovae will appear substantially different from AT2017gfo. We also show that 1D models obtained by spherically averaging the 3D ejecta lead to dramatically different direction-integrated luminosities and spectra compared to full 3D calculations.
8.AGN STORM 2. IV. Swift X-ray and ultraviolet/optical monitoring of Mrk 817
Authors:Edward M. Cackett, Jonathan Gelbord, Aaron J. Barth, Gisella De Rosa, Rick Edelson, Michael R. Goad, Yasaman Homayouni, Keith Horne, Erin A. Kara, Gerard A. Kriss, Kirk T. Korista, Hermine Landt, Rachel Plesha, Nahum Arav, Misty C. Bentz, Benjamin D. Boizelle, Elena Dalla Bonta, Maryam Dehghanian, Fergus Donnan, Pu Du, Gary J. Ferland, Carina Fian, Alexei V. Filippenko, Diego H. Gonzalez Buitrago, Catherine J. Grier, Patrick B. Hall, Chen Hu, Dragana Ilic, Jelle Kaastra, Shai Kaspi, Christopher S. Kochanek, Andjelka B. Kovacevic, Daniel Kynoch, Yan-Rong Li, Jacob N. McLane, Missagh Mehdipour, Jake A. Miller, John Montano, Hagai Netzer, Christos Panagiotou, Ethan Partington, Luka C. Popovic, Daniel Proga, Daniele Rogantini, David Sanmartim, Matthew R. Siebert, Thaisa Storchi-Bergmann, Marianne Vestergaard, Jian-Min Wang, Tim Waters, Fatima Zaidouni
Abstract: The AGN STORM 2 campaign is a large, multiwavelength reverberation mapping project designed to trace out the structure of Mrk 817 from the inner accretion disk to the broad emission line region and out to the dusty torus. As part of this campaign, Swift performed daily monitoring of Mrk 817 for approximately 15 months, obtaining observations in X-rays and six UV/optical filters. The X-ray monitoring shows that Mrk 817 was in a significantly fainter state than in previous observations, with only a brief flare where it reached prior flux levels. The X-ray spectrum is heavily obscured. The UV/optical light curves show significant variability throughout the campaign and are well correlated with one another, but uncorrelated with the X-rays. Combining the Swift UV/optical light curves with Hubble UV continuum light curves, we measure interband continuum lags, $\tau(\lambda)$, that increase with increasing wavelength roughly following $\tau(\lambda) \propto \lambda^{4/3}$, the dependence expected for a geometrically thin, optically thick, centrally illuminated disk. Modeling of the light curves reveals a period at the beginning of the campaign where the response of the continuum is suppressed compared to later in the light curve - the light curves are not simple shifted and scaled versions of each other. The interval of suppressed response corresponds to a period of high UV line and X-ray absorption, and reduced emission line variability amplitudes. We suggest that this indicates a significant contribution to the continuum from the broad line region gas that sees an absorbed ionizing continuum.
9.Fuzzy Dark Matter in Relativistic Stars
Authors:Zeinab Rezaei
Abstract: Fuzzy dark matter (FDM), a practical alternative to cold dark matter, can exist in compact stars. Here, applying the FDM equation of state (EoS) constrained by CMB and large-scale structure data, we calculate the structure of relativistic stars in the presence of FDM. For this aim, the EoS for the visible matter in neutron stars, quark stars, and hybrid stars from the observational data are employed. A piecewise polytropic EoS constrained by the observational data of GW170817 and the data of six low-mass X-ray binaries with thermonuclear burst or the symmetry energy of the nuclear interaction describes the neutron star matter. For quark star matter, we apply the EoSs within the Bayesian statistical approach using the mass and radius measurements of PSR J0030+0451 from NICER. Employing the two-fluid formalism, we study the structure of FDM admixed relativistic stars.
10.Observations of Magnetospheric Solar Wind Charge Exchange
Authors:R. Ringuette, K. D. Kuntz, D. Koutroumpa, P. Kaaret, D. LaRocca, J. Richardson
Abstract: The study of solar wind charge exchange (SWCX) emission is vital to both the X-ray astrophysics and heliophysics communities. SWCX emission contaminates all astrophysical observations in X-rays regardless of the direction. Ignoring this contribution to X-ray spectra can lead to erroneous conclusions regarding the astrophysical plasmas along the line of sight due to the similar spectral distributions of SWCX and several common types of more distant astrophysical plasmas. Since its discovery, literature has distinguished between diffuse SWCX emission resulting from solar wind neutral interactions within the terrestrial magnetosphere, called magnetospheric SWCX, and similar interactions occurring more generally throughout the heliosphere, called heliospheric SWCX. Here, we build upon previous work validating a modeling method for the heliospheric SWCX contribution in X-ray spectra obtained with a medium resolution CubeSat instrument named HaloSat at low ecliptic latitudes. We now apply this model to a specially designed set of extended observations with the same instrument and successfully separate the spectral contributions of the astrophysical background and the heliospheric SWCX from the remaining contributions. Specifically, we find significant excess emission for four observations in the O VII emission line not explained by other sources, possibly indicative of magnetospheric SWCX. We discuss these results in comparison with simulation results publicly available through the Community Coordinated Modeling Center. We also report an absorbed high-temperature component in two of the twelve fields of view analyzed.
11.Gravitational wave sources for Pulsar Timing Arrays
Authors:Ligong Bian, Shuailiang Ge, Jing Shu, Bo Wang, Xing-Yu Yang, Junchao Zong
Abstract: Very recently, several pulsar timing array collaborations, including CPTA, EPTA, and NANOGrav, reported their results from searches for an isotropic stochastic gravitational wave background (SGWB), with each finding positive evidence for SGWB. In this work, we assessed the credibility of interpreting the Hellings-Downs correlated free-spectrum process of EPTA, PPTA, and NANOGrav as either the result of supermassive black hole binary mergers or various stochastic SGWB sources that originated in the early Universe, including first-order phase transitions, cosmic strings, domain walls, and large-amplitude curvature perturbations. Our observations show that the current new datasets do not display a strong preference for any specific SGWB source based on Bayesian analysis.
12.Multiwavelength Observations of the Blazar PKS 0735+178 in Spatial and Temporal Coincidence with an Astrophysical Neutrino Candidate IceCube-211208A
Authors:A. Acharyya The VERITAS Collaboration, C. B. Adams The VERITAS Collaboration, A. Archer The VERITAS Collaboration, P. Bangale The VERITAS Collaboration, J. T. Bartkoske The VERITAS Collaboration, P. Batista The VERITAS Collaboration, W. Benbow The VERITAS Collaboration, A. Brill The VERITAS Collaboration, J. H. Buckley The VERITAS Collaboration, J. L. Christiansen The VERITAS Collaboration, A. J. Chromey The VERITAS Collaboration, M. Errando The VERITAS Collaboration, A. Falcone The VERITAS Collaboration, Q. Feng The VERITAS Collaboration, G. M. Foote The VERITAS Collaboration, L. Fortson The VERITAS Collaboration, A. Furniss The VERITAS Collaboration, G. Gallagher The VERITAS Collaboration, W. Hanlon The VERITAS Collaboration, D. Hanna The VERITAS Collaboration, O. Hervet The VERITAS Collaboration, C. E. Hinrichs The VERITAS Collaboration, J. Hoang The VERITAS Collaboration, J. Holder The VERITAS Collaboration, T. B. Humensky The VERITAS Collaboration, W. Jin The VERITAS Collaboration, P. Kaaret The VERITAS Collaboration, M. Kertzman The VERITAS Collaboration, M. Kherlakian The VERITAS Collaboration, D. Kieda The VERITAS Collaboration, T. K. Kleiner The VERITAS Collaboration, N. Korzoun The VERITAS Collaboration, S. Kumar The VERITAS Collaboration, M. J. Lang The VERITAS Collaboration, M. Lundy The VERITAS Collaboration, G. Maier The VERITAS Collaboration, C. E McGrath The VERITAS Collaboration, M. J. Millard The VERITAS Collaboration, J. Millis The VERITAS Collaboration, C. L. Mooney The VERITAS Collaboration, P. Moriarty The VERITAS Collaboration, R. Mukherjee The VERITAS Collaboration, S. O'Brien The VERITAS Collaboration, R. A. Ong The VERITAS Collaboration, M. Pohl The VERITAS Collaboration, E. Pueschel The VERITAS Collaboration, J. Quinn The VERITAS Collaboration, K. Ragan The VERITAS Collaboration, P. T. Reynolds The VERITAS Collaboration, D. Ribeiro The VERITAS Collaboration, E. Roache The VERITAS Collaboration, I. Sadeh The VERITAS Collaboration, A. C. Sadun The VERITAS Collaboration, L. Saha The VERITAS Collaboration, M. Santander The VERITAS Collaboration, G. H. Sembroski The VERITAS Collaboration, R. Shang The VERITAS Collaboration, M. Splettstoesser The VERITAS Collaboration, A. Kaushik Talluri The VERITAS Collaboration, J. V. Tucci The VERITAS Collaboration, V. V. Vassiliev The VERITAS Collaboration, A. Weinstein The VERITAS Collaboration, D. A. Williams The VERITAS Collaboration, S. L. Wong The VERITAS Collaboration, J. Woo The VERITAS Collaboration, F. Aharonian The H.E.S.S. Collaboration, J. Aschersleben The H.E.S.S. Collaboration, M. Backes The H.E.S.S. Collaboration, V. Barbosa Martins The H.E.S.S. Collaboration, R. Batzofin The H.E.S.S. Collaboration, Y. Becherini The H.E.S.S. Collaboration, D. Berge The H.E.S.S. Collaboration, K. Bernlohr The H.E.S.S. Collaboration, B. Bi The H.E.S.S. Collaboration, M. Bottcher The H.E.S.S. Collaboration, C. Boisson The H.E.S.S. Collaboration, J. Bolmont The H.E.S.S. Collaboration, M. de Bony de Lavergne The H.E.S.S. Collaboration, J. Borowska The H.E.S.S. Collaboration, M. Bouyahiaoui The H.E.S.S. Collaboration, F. Bradascio The H.E.S.S. Collaboration, M. Breuhaus The H.E.S.S. Collaboration, R. Brose The H.E.S.S. Collaboration, F. Brun The H.E.S.S. Collaboration, B. Bruno The H.E.S.S. Collaboration, T. Bulik The H.E.S.S. Collaboration, C. Burger-Scheidlin The H.E.S.S. Collaboration, S. Caroff The H.E.S.S. Collaboration, S. Casanova The H.E.S.S. Collaboration, R. Cecil The H.E.S.S. Collaboration, J. Celic The H.E.S.S. Collaboration, M. Cerruti The H.E.S.S. Collaboration, T. Chand The H.E.S.S. Collaboration, S. Chandra The H.E.S.S. Collaboration, A. Chen The H.E.S.S. Collaboration, J. Chibueze The H.E.S.S. Collaboration, O. Chibueze The H.E.S.S. Collaboration, G. Cotter The H.E.S.S. Collaboration, S. Dai The H.E.S.S. Collaboration, J. Damascene Mbarubucyeye The H.E.S.S. Collaboration, A. Djannati-Atai The H.E.S.S. Collaboration, A. Dmytriiev The H.E.S.S. Collaboration, V. Doroshenko The H.E.S.S. Collaboration, S. Einecke The H.E.S.S. Collaboration, J. -P. Ernenwein The H.E.S.S. Collaboration, G. Fichet de Clairfontaine The H.E.S.S. Collaboration, M. Filipovic The H.E.S.S. Collaboration, G. Fontaine The H.E.S.S. Collaboration, M. Fussling The H.E.S.S. Collaboration, S. Funk The H.E.S.S. Collaboration, S. Gabici The H.E.S.S. Collaboration, S. Ghafourizadeh The H.E.S.S. Collaboration, G. Giavitto The H.E.S.S. Collaboration, D. Glawion The H.E.S.S. Collaboration, J. F. Glicenstein The H.E.S.S. Collaboration, P. Goswami The H.E.S.S. Collaboration, G. Grolleron The H.E.S.S. Collaboration, L. Haerer The H.E.S.S. Collaboration, J. A. Hinton The H.E.S.S. Collaboration, T. L. Holch The H.E.S.S. Collaboration, M. Holler The H.E.S.S. Collaboration, D. Horns The H.E.S.S. Collaboration, M. Jamrozy The H.E.S.S. Collaboration, F. Jankowsky The H.E.S.S. Collaboration, V. Joshi The H.E.S.S. Collaboration, I. Jung-Richardt The H.E.S.S. Collaboration, E. Kasai The H.E.S.S. Collaboration, K. Katarzynski The H.E.S.S. Collaboration, R. Khatoon The H.E.S.S. Collaboration, B. Khelifi The H.E.S.S. Collaboration, S. Klepser The H.E.S.S. Collaboration, W. Kluzniak The H.E.S.S. Collaboration, K. Kosack The H.E.S.S. Collaboration, D. Kostunin The H.E.S.S. Collaboration, R. G. Lang The H.E.S.S. Collaboration, S. Le Stum The H.E.S.S. Collaboration, A. Lemiere The H.E.S.S. Collaboration, J. P. Lenain The H.E.S.S. Collaboration, F. Leuschner The H.E.S.S. Collaboration, T. Lohse The H.E.S.S. Collaboration, A. Luashvili The H.E.S.S. Collaboration, I. Lypova The H.E.S.S. Collaboration, J. Mackey The H.E.S.S. Collaboration, D. Malyshev The H.E.S.S. Collaboration, V. Marandon The H.E.S.S. Collaboration, P. Marchegiani The H.E.S.S. Collaboration, A. Marcowith The H.E.S.S. Collaboration, G. Marti-Devesa The H.E.S.S. Collaboration, R. Marx The H.E.S.S. Collaboration, A. Mitchell The H.E.S.S. Collaboration, R. Moderski The H.E.S.S. Collaboration, L. Mohrmann The H.E.S.S. Collaboration, A. Montanari The H.E.S.S. Collaboration, E. Moulin The H.E.S.S. Collaboration, T. Murach The H.E.S.S. Collaboration, K. Nakashima The H.E.S.S. Collaboration, J. Niemiec The H.E.S.S. Collaboration, A. Priyana Noel The H.E.S.S. Collaboration, P. O'Brien The H.E.S.S. Collaboration, L. Olivera-Nieto The H.E.S.S. Collaboration, E. de Ona Wilhelmi The H.E.S.S. Collaboration, M. Ostrowski The H.E.S.S. Collaboration, S. Panny The H.E.S.S. Collaboration, M. Panter The H.E.S.S. Collaboration, G. Peron The H.E.S.S. Collaboration, D. A. Prokhorov The H.E.S.S. Collaboration, G. Puhlhofer The H.E.S.S. Collaboration, M. Punch The H.E.S.S. Collaboration, A. Quirrenbach The H.E.S.S. Collaboration, P. Reichherzer The H.E.S.S. Collaboration, A. Reimer The H.E.S.S. Collaboration, O. Reimer The H.E.S.S. Collaboration, H. Ren The H.E.S.S. Collaboration, M. Renaud The H.E.S.S. Collaboration, F. Rieger The H.E.S.S. Collaboration, B. Rudak The H.E.S.S. Collaboration, E. Ruiz-Velasco The H.E.S.S. Collaboration, V. Sahakian The H.E.S.S. Collaboration, A. Santangelo The H.E.S.S. Collaboration, M. Sasaki The H.E.S.S. Collaboration, J. Schafer The H.E.S.S. Collaboration, F. Schussler The H.E.S.S. Collaboration, H. M. Schutte The H.E.S.S. Collaboration, U. Schwanke The H.E.S.S. Collaboration, J. N. S. Shapopi The H.E.S.S. Collaboration, A. Specovius The H.E.S.S. Collaboration, S. Spencer The H.E.S.S. Collaboration, L. Stawarz The H.E.S.S. Collaboration, R. Steenkamp The H.E.S.S. Collaboration, S. Steinmassl The H.E.S.S. Collaboration, I. Sushch The H.E.S.S. Collaboration, H. Suzuki The H.E.S.S. Collaboration, T. Takahashi The H.E.S.S. Collaboration, T. Tanaka The H.E.S.S. Collaboration, R. Terrier The H.E.S.S. Collaboration, C. van Eldik The H.E.S.S. Collaboration, M. Vecchi The H.E.S.S. Collaboration, J. Veh The H.E.S.S. Collaboration, C. Venter The H.E.S.S. Collaboration, J. Vink The H.E.S.S. Collaboration, R. White The H.E.S.S. Collaboration, A. Wierzcholska The H.E.S.S. Collaboration, Yu Wun Wong The H.E.S.S. Collaboration, M. Zacharias The H.E.S.S. Collaboration, D. Zargaryan The H.E.S.S. Collaboration, A. A. Zdziarski The H.E.S.S. Collaboration, A. Zech The H.E.S.S. Collaboration, S. Zouari The H.E.S.S. Collaboration, N. Zywucka The H.E.S.S. Collaboration, K. Mori
Abstract: We report on multiwavelength target-of-opportunity observations of the blazar PKS 0735+178, located 2.2$^\circ$ away from the best-fit position of the IceCube neutrino event IceCube-211208A detected on December 8, 2021. The source was in a high-flux state in the optical, ultraviolet, X-ray, and GeV gamma-ray bands around the time of the neutrino event, exhibiting daily variability in the soft X-ray flux. The X-ray data from Swift-XRT and NuSTAR characterize the transition between the low-energy and high-energy components of the broadband spectral energy distribution (SED), and the gamma-ray data from Fermi -LAT, VERITAS, and H.E.S.S. require a spectral cut-off near 100 GeV. Both X-ray and gamma-ray measurements provide strong constraints on the leptonic and hadronic models. We analytically explore a synchrotron self-Compton model, an external Compton model, and a lepto-hadronic model. Models that are entirely based on internal photon fields face serious difficulties in matching the observed SED. The existence of an external photon field in the source would instead explain the observed gamma-ray spectral cut-off in both leptonic and lepto-hadronic models and allow a proton jet power that marginally agrees with the Eddington limit in the lepto-hadronic model. We show a numerical lepto-hadronic model with external target photons that reproduces the observed SED and is reasonably consistent with the neutrino event despite requiring a high jet power.
13.Binary Supermassive Black Holes Orbiting Dark Matter Solitons: From the Dual AGN in UGC4211 to NanoHertz Gravitational Waves
Authors:Tom Broadhurst, Chao Chen, Tao Liu, Kai-Feng Zheng
Abstract: We explore the orbital implications of the Supermassive Black Hole (SMBH) binary in UGC4211, for the frequency spectrum of stochastic gravitational wave background (SGWB) being measured with pulsar timing arrays. The SMBH binary in UGC4211 has a projected separation of $\sim 230$ pc and relative velocity of $\sim 150$ km/s along the line of sight. It orbits a common disk of gas and stars, with a total dynamical mass of $\sim 10^9 M_\odot$ which is several times larger than the combined SMBHs plus the observed gas and stars. This can be explained by a massive soliton of wave dark matter present within the orbit of two SMBHs. Such a scenario is encouraging as during galaxy merger, the two precursor galactic solitons are expected to combine to generate a new soliton and hence the two initial SMBHs become efficiently bound. Generalizing this scenario to the cosmological population of SMBH binaries, we show that the SGWB spectrum produced by their late-stage inspiraling is modified preferentially at low frequency by the presence of the soliton. Finally we discuss future prospects for this proof-of-concept study, by fitting this scenario to the 15-year NANOGrav data.
14.Theory of spatially non-symmetric kinetic equilibria for collisionless plasmas
Authors:Claudio Cremaschini, Massimo Tessarotto
Abstract: The problem posed by the possible existence/non-existence of spatially non-symmetric kinetic equilibria has remained unsolved in plasma theory. For collisionless magnetized plasmas this involves the construction of stationary solutions of the Vlasov-Maxwell equations. In this paper the issue is addressed for non-relativistic plasmas both in astrophysical and laboratory contexts. The treatment is based on a Lagrangian variational description of single-particle dynamics. Starting point is a non-perturbative formulation of gyrokinetic theory, which allows one to construct "a posteriori" with prescribed order of accuracy an asymptotic representation for the magnetic moment. In terms of the relevant particle adiabatic invariants generalized bi-Maxwellian equilibria are proved to exist. These are shown to recover, under suitable assumptions, a Chapman-Enskog form which permits an analytical treatment of the corresponding fluid moments. In particular, the constrained posed by the Poisson and the Ampere equations are analyzed, both for quasi-neutral and non-neutral plasmas. The conditions of existence of the corresponding non-symmetric kinetic equilibria are investigated. As a notable feature, both astrophysical and laboratory plasmas are shown to exhibit, under suitable conditions, a kinetic dynamo, whereby the equilibrium magnetic field can be self-generated by the equilibrium plasma currents.