Sixteen years of X-ray monitoring of Sagittarius A*: Evidence for a decay of the faint flaring rate from 2013 August, 13 months before a rise in the bright flaring rate

Recently, in a study the X-ray flaring activity of Sgr A* with Chandra and XMM-Newton public observations from 1999 to 2014 and 2014 Swift data, it has been argued that the "bright and very bright" flaring rate raised from 2014 Aug. 31. Thanks to 482ks of observations performed in 2015 with Chandra, XMM-Newton and Swift, we test the significance of this rise of flaring rate and determine the threshold of unabsorbed flare flux or fluence leading to any flaring-rate change. The mean unabsorbed fluxes of the 107 flares detected in the 1999-2015 observations are consistently computed from the extracted spectra and calibration files, assuming the same spectral parameters. We construct the observed flare fluxes and durations distribution for the XMM-Newton and Chandra flares and correct it from the detection biases to estimate the intrinsic distribution from which we determine the average flare detection efficiency for each observation. We apply the BB algorithm on the flare arrival times corrected from the corresponding efficiency. We confirm a constant overall flaring rate in 1999-2015 and a rise in the flaring rate for the most luminous/energetic flares from 2014 Aug. 31 (4 months after the passage of the DSO/G2 close to Sgr A*). We also identify a decay of the flaring rate for the less luminous and less energetic flares from 2013 Aug. and Nov., respectively (10 and 7 months before the pericenter of the DSO/G2). The decay of the faint flaring rate is difficult to explain by the tidal disruption of the DSO/G2, whose stellar nature is now well established, since it occurred well before its pericenter. Moreover, a mass transfer from the DSO/G2 to Sgr A* is not required to produce the rise in the bright flaring rate since the energy saved by the decay of the number of faint flares during a long time period may be later released by several bright flares during a shorter time period. (abridged)Comment: Accepted in A&A in 2017 April 2

Fe xxv line profiles in colliding wind binaries

Strong wind-wind collisions in massive binaries generate a very hot plasma that frequently produces a moderately strong iron line. The morphology of this line depends upon the properties of the wind interaction zone and its orientation with respect to the line of sight. As the binary components revolve around their common centre of mass, the line profiles are thus expected to vary. With the advent of the next generation of X-ray observatories (Astro-H, Athena) that will offer high-resolution spectroscopy above 6 keV, it will become possible to exploit these changes as the most sensitive probe of the inner parts of the colliding wind interaction. Using a simple prescription of the wind-wind interaction in an early-type binary, we have generated synthetic line profiles for a number of configurations and orbital phases. These profiles can help constrain the properties of the stellar winds in such binary systems.Comment: Accepted for publication in New Astronom

L'application du principe du pollueur-payeur à la gestion du risque environnemental et à la mutualisation des coûts de la pollution

Le but de cette étude est de déterminer qui paie pour le risque de pollution et par conséquent de vérifier si le principe du pollueur-payeur est effectivement mis en œuvre dans le domaine de la gestion du risque environnemental. Il s’agit d’examiner le degré de mutualisation de la gestion du risque dans différentes législations particulière. Les payeurs peuvent a priori se classer dans quatre catégories : les personnes dont l’activité contribue au risque de pollution, les compagnies d’assurance qui acceptent d’assurer ces personnes, les organismes ou autorités publics et les tiers. Divers exemples issus de la législation belge ou européenne seront examinés afin de déterminer s’ils sont conformes à la lettre et/ou à l’esprit du principe pollueur-payeur. Il s’agit notamment de la responsabilité civile, de la responsabilité environnementale, de la gestion des déchets et du marché de quotas d’émissions de gaz à effet de serre. Les techniques de responsabilité qui interviennent après que le dommage ait lieu et requièrent la démonstration de l’existence d’un lien de causalité ne permettent pas toujours d’assurer pleinement la fonction préventive du principe du pollueur-payeur. Elles ne constituent pas des instruments adéquats de gestion de la pollution diffuse ou chronique. En conséquence, des techniques de mutualisation de la gestion du risque environnemental se sont développées. Le recours à ces techniques de mutualisation (par le recours à l’assurance, aux fonds publics financés par la fiscalité environnementale ou aux marchés de droit d’émissions) est-il conforme au principe pollueur-payeur et permet-il d’atteindre l’objectif d’un niveau élevé de protection de l’environnement ? L’effet dissuasif du principe pollueur-payeur n’est-il pas amoindri par la mutualisation ? L’article montre que la définition du principe pollueur-payeur par la Cour de Justice de l’Union européenne est centrée sur la contribution au risque de pollution ce qui permet de recourir aux techniques de mutualisation de la gestion du risque tout en respectant le Traité sur le fonctionnement de l’Union européenne. The aim of this paper is to identify who pays for the risk of pollution and to verify if the polluter-pays principle is effectively implemented in the field of environmental risk management. We will examine the degree of risk-sharing in various specific legislations. Payers can a priori be classified in four categories: those whose activity contributes to the risk of pollution, the insurance companies who agree to insure such persons, agencies or public authorities and third parties. Various examples from the Belgian or European legal system will be examined to determine if they comply with the letter and/or spirit of the polluter pays principle. These include civil liability, environmental liability, waste management and greenhouse gas emission allowance trading. The liability rules which act after the damage occurs and require the demonstration of the existence of a causal link do not always fulfill the preventive function of the polluter pays. They are not appropriate for the management of diffuse or chronic pollution. Consequently, risk-sharing rules were developed. The question arises whether the use of these risk-sharing instruments (insurances, public funds financed by environmental taxes or emission allowance trading schemes) is consistent with the polluter pays principle and helps to reach the objective of a high level of environmental protection. Is the deterrent effect of the polluter pays principle reduced by risk-sharing? The paper shows that the definition of the polluter pays principle by the European Court of Justice focuses on the contribution to the risk of pollution. As a consequence, the use of risk-sharing instruments to manage environmental risk is consistent with the Treaty on the functioning of the European Union and the case law

The long-period massive binary HD~54662 revisited

HD54662 is an O-type binary star belonging to the CMa OB1 association. Due to its long-period orbit, this system is an interesting target to test the adiabatic wind shock model. The goal is to improve our knowledge of the orbital and stellar parameters of HD54662 and to analyze its X-ray emission to test the theoretical scaling of the X-ray emission with orbital separation for adiabatic wind shocks. We applied a spectral disentangling code to optical spectra to determine the radial velocities and the individual spectra of each star. The individual spectra were analyzed using the CMFGEN model atmosphere code. We fitted two X-ray spectra using a Markov Chain Monte Carlo algorithm and compared them to the emission expected from adiabatic shocks. We determine an orbital period of 2103.4days, a low orbital eccentricity of 0.11, and a mass ratio m2/m1=0.84. Combined with the orbital inclination inferred in a previous astrometric study, we obtain surprisingly low masses of 9.7 and 8.2Msun. From the individual spectra, we infer O6.5 spectral types for both stars and a brightness ratio of l1/l2~2. The softness of the X-ray spectra, the very small variation of spectral parameters, and the comparison of the X-ray-to-bolometric luminosity ratio with the canonical value for O-type stars allow us to conclude that X-ray emission from the wind interaction region is quite low. We cannot confirm the runaway status previously attributed to HD54662 and we find no X-ray emission associated with the bow shock detected in the infrared. The lack of hard X-ray emission from the wind-shock region suggests that the mass-loss rates are lower than expected and/or that the pre-shock wind velocities are much lower than the terminal wind velocities. The bow shock associated with HD54662 possibly corresponds to a wind-blown arc created by the interaction of the stellar winds with the ionized gas of CMa OB1. (abridged)Comment: Manuscript has been accepted. A&A, in pres

Study of the X-ray activity of Sgr A* during the 2011 XMM-Newton campaign

In Spring 2011 we observed Sgr A*, the supermassive black hole at the center of our Galaxy, with XMM-Newton with a total exposure of ~226 ks in coordination with the 1.3 mm VLBI. We have performed timing analysis of the X-ray emission from Sgr A* using Bayesian blocks algorithm to detect X-ray flares observed with XMM-Newton. Furthermore, we computed X-ray smoothed light curves observed in this campaign in order to have better accuracy on the position and the amplitude of the flares. We detected 2 X-ray flares on the 2011 March 30 and April 3 which have for comparison a peak detection level of 6.8 and 5.9 sigma in the XMM-Newton/EPIC light curve in the 2-10 keV energy range with a 300 s bin. The former is characterized by 2 sub-flares: the first one is very short (~458 s) with a peak luminosity of ~9.4E34 erg/s whereas the second one is longer (~1542 s) with a lower peak luminosity of ~6.8E34 erg/s. The comparison with the sample of X-ray flares detected during the 2012 Chandra XVP campaign favors the hypothesis that the 2011 March 30 flare is a single flare rather than 2 distinct sub-flares. We model the light curve of this flare with the gravitational lensing of a simple hotspot-like structure but we can not satisfactorily reproduce the large decay of the light curve between the 2 sub-flares with this model. From magnetic energy heating during the rise phase of the first sub-flare and assuming an X-ray photons production efficiency of 1 and a magnetic field of 100 G at 2 r_g, we derive an upper limit to the radial distance of the first sub-flare of 100 r_g. We estimate using the decay phase of the first sub-flare a lower limit to the radial distance of 4 r_g from synchrotron cooling in the infrared. The X-ray emitting region of the first sub-flare is located at a radial position of 4-100 and has a corresponding radius of 1.8-2.87 in r_g unit for a magnetic field of 100 G at 2 r_g.Comment: Version published in A&A + corrigendum published in A&

Sixteen years of X-ray monitoring of Sagittarius A*: Evidence for a decay of the faint flaring rate from 2013 August, 13 months before a rise in the bright flaring rate

Recently, in a study the X-ray flaring activity of Sgr A* with Chandra and XMM-Newton public observations from 1999 to 2014 and 2014 Swift data, it has been argued that the "bright and very bright" flaring rate raised from 2014 Aug. 31. Thanks to 482ks of observations performed in 2015 with Chandra, XMM-Newton and Swift, we test the significance of this rise of flaring rate and determine the threshold of unabsorbed flare flux or fluence leading to any flaring-rate change. The mean unabsorbed fluxes of the 107 flares detected in the 1999-2015 observations are consistently computed from the extracted spectra and calibration files, assuming the same spectral parameters. We construct the observed flare fluxes and durations distribution for the XMM-Newton and Chandra flares and correct it from the detection biases to estimate the intrinsic distribution from which we determine the average flare detection efficiency for each observation. We apply the BB algorithm on the flare arrival times corrected from the corresponding efficiency. We confirm a constant overall flaring rate in 1999-2015 and a rise in the flaring rate for the most luminous/energetic flares from 2014 Aug. 31 (4 months after the passage of the DSO/G2 close to Sgr A*). We also identify a decay of the flaring rate for the less luminous and less energetic flares from 2013 Aug. and Nov., respectively (10 and 7 months before the pericenter of the DSO/G2). The decay of the faint flaring rate is difficult to explain by the tidal disruption of the DSO/G2, whose stellar nature is now well established, since it occurred well before its pericenter. Moreover, a mass transfer from the DSO/G2 to Sgr A* is not required to produce the rise in the bright flaring rate since the energy saved by the decay of the number of faint flares during a long time period may be later released by several bright flares during a shorter time period. (abridged)Comment: Accepted in A&A in 2017 April 2

Search for non-thermal X-ray emission in the colliding wind binary Cygnus OB2 #8A⋆

Aims. Cyg OB2 #8A is a massive O-type binary displaying strong non-thermal radio emission. Owing to the compactness of this binary, emission of non-thermal X-ray photons via inverse Compton scattering is expected. Methods. We first revised the orbital solution for Cyg OB2 #8A using new optical spectra. We then reduced and analysed X-ray spectra obtained with XMM-Newton, Swift, INTEGRAL, and NuSTAR. Results. The analysis of the XMM-Newton and Swift data allows us to better characterise the X-ray emission from the stellar winds and colliding winds region at energies below 10 keV. We confirm the variation of the broad-band light curve of Cyg OB2 #8A along the orbit with, for the first time, the observation of the maximum emission around phase 0.8. The minimum ratio of the X-ray to bolometric flux of Cyg OB2 #8A remains well above the level expected for single O-type stars, indicating that the colliding wind region is not disrupted during the periastron passage. The analysis of the full set of publicly available INTEGRAL observations allows us to refine the upper limit on the non-thermal X-ray flux of the Cyg OB2 region between 20 and 200 keV. Two NuSTAR observations (phases 0.028 and 0.085) allow us to study the Cyg OB2 #8A spectrum up to 30 keV. These data do not provide evidence of the presence of non-thermal X-rays, but bring more stringent constraints on the flux of a putative non-thermal component. Finally, we computed, thanks to a new dedicated model, the anisotropic inverse Compton emission generated in the wind shock region. The theoretical non-thermal emission appears to be compatible with observational limits and the kinetic luminosity computed from these models is in good agreement with the unabsorbed flux observed below 10 keV

Colliding winds in massive binary systems to be diagnosed with X-IFU

OB and Wolf-Rayet stars feature energetic stellar winds. In massive binary systems, the winds of both components collide. This leads to the formation of a hot X-ray emitting plasma. The properties of this plasma are best studied via Athena/X-IFU observations of the line profiles of the Fe xxv line complex at 6.7 keV. We have designed numerical tools to predict the morphology of those lines for a variety of configurations and to extract a maximum of information from the future observations.PRODEX HERMe