M. Bryan
University of Amsterdam
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Featured researches published by M. Bryan.
Science | 2015
A. Abramowski; A. Balzer; D. Berge; M. Bryan; D. Salek; J. Vink
A light on the origin of cosmic rays Theres a new lab for studying the origins of cosmic rays: our neighbor galaxy, the Large Magellanic Cloud. Astronomers are now making progress on this topic by examining the gamma rays that are produced when cosmic rays interact with gas or lower-energy photons. The H.E.S.S. Collaboration has detected three sources of gamma rays in a variety of forms in the galactic satellite to the Milky Way. The sources include the pulsar wind nebula of N 157B, the supernova remnant N 132D, and the superbubble 30 Dor C. Oddly, supernova 1987A was not detected. Science, this issue p. 406 Three types of sources were detected at energies above 100 billion electron volts: a pulsar wind nebula, a supernova remnant, and a superbubble. The Large Magellanic Cloud, a satellite galaxy of the Milky Way, has been observed with the High Energy Stereoscopic System (H.E.S.S.) above an energy of 100 billion electron volts for a deep exposure of 210 hours. Three sources of different types were detected: the pulsar wind nebula of the most energetic pulsar known, N 157B; the radio-loud supernova remnant N 132D; and the largest nonthermal x-ray shell, the superbubble 30 Dor C. The unique object SN 1987A is, unexpectedly, not detected, which constrains the theoretical framework of particle acceleration in very young supernova remnants. These detections reveal the most energetic tip of a γ-ray source population in an external galaxy and provide via 30 Dor C the unambiguous detection of γ-ray emission from a superbubble.
The Astrophysical Journal | 2015
A. Abramowski; A. Balzer; D. Berge; M. Bryan; D. Salek; J. Vink
Very high energy (VHE, E > 100 GeV)gamma-ray flaring activity of the high-frequency peaked BL Lac object PG 1553 + 113 has been detected by the H.E.S.S. telescopes. The flux of the source increased by a factor of 3 during the nights of 2012 April 26 and 27 with respect to the archival measurements with a hint of intra-night variability. No counterpart of this event has been detected in the Fermi-Large Area Telescope data. This pattern is consistent with VHE gamma(-)ray flaring being caused by the injection of ultrarelativistic particles, emitting.-rays at the highest energies. The dataset offers a unique opportunity to constrain the redshift of this source at z = 0.49 +/- 0.04 using a novel method based on Bayesian statistics. The indication of intra-night variability is used to introduce a novel method to probe for a possible Lorentz invariance violation (LIV), and to set limits on the energy scale at which Quantum Gravity (QG) effects causing LIV may arise. For the subluminal case, the derived limits are E-QG,E- 1 > 4.10 x 10(17) GeV and E-QG,E- 2 > 2.10 x 10(10) GeV for linear and quadratic LIV effects, respectively.
The Astrophysical Journal | 2014
A. Abramowski; A. Balzer; D. Berge; M. Bryan; D. Salek; J. Vink
This Letter reports the discovery of a remarkably hard spectrum source, HESS J1641-463, by the High Energy Stereoscopic System (H.E.S.S.) in the very high energy (VHE) domain. HESS J1641-463 remained unnoticed by the usual analysis techniques due to confusion with the bright nearby source HESS J1640-465. It emerged at a significance level of 8.5 standard deviations after restricting the analysis to events with energies above 4 TeV. It shows a moderate flux level of phi(E > 1TeV) = (3.64 +/- 0.44(stat)+/- 0.73(sys)) x 10(-13) cm(-2) s(-1), corresponding to 1.8% of the Crab Nebula flux above the same energy, and a hard spectrum with a photon index of Gamma = 2.07 +/- 0.11(stat)+/- 0.20(sys). It is a point-like source, although an extension up to a Gaussian width of sigma = 3 arcmin cannot be discounted due to uncertainties in the H.E.S.S. point-spread function. The VHE gamma-ray flux of HESS J1641-463 is found to be constant over the observed period when checking time binnings from the year-by-year to the 28 minute exposure timescales. HESS J1641-463 is positionally coincident with the radio supernova remnant SNR G338.5+0.1. No X-ray candidate stands out as a clear association; however, Chandra and XMM-Newton data reveal some potential weak counterparts. Various VHE gamma-ray production scenarios are discussed. If the emission from HESS J1641-463 is produced by cosmic ray protons colliding with the ambient gas, then their spectrum must extend close to 1 PeV. This object may represent a source population contributing significantly to the galactic cosmic ray flux around the knee.
arXiv: Instrumentation and Methods for Astrophysics | 2017
J.J. Watson; A. De Franco; A. Abchiche; D. Allan; J. P. Amans; T. Armstrong; A. Balzer; D. Berge; C. Boisson; J. J. Bousquet; A. M. Brown; M. Bryan; Gilles Buchholtz; P. M. Chadwick; H. Costantini; Garret Cotter; M. K. Daniel; F. De Frondat; Jean-Laurent Dournaux; D. J. P. Dumas; J.-P. Ernenwein; G. Fasola; S. Funk; J. Gironnet; J. A. Graham; T. Greenshaw; O. Hervet; N. Hidaka; J. A. Hinton; Jean-Michel Huet
The Gamma-ray Cherenkov Telescope (GCT) is a candidate for the Small Size Telescopes (SSTs) of the Cherenkov Telescope Array (CTA). Its purpose is to extend the sensitivity of CTA to gamma-ray energies reaching 300 TeV. Its dual-mirror optical design and curved focal plane enables the use of a compact camera of 0.4 m diameter, while achieving a field of view of above 8 degrees. Through the use of the digitising TARGET ASICs, the Cherenkov flash is sampled once per nanosecond contin-uously and then digitised when triggering conditions are met within the analogue outputs of the photosensors. Entire waveforms (typically covering 96 ns) for all 2048 pixels are then stored for analysis, allowing for a broad spectrum of investigations to be performed on the data. Two prototypes of the GCT camera are under development, with differing photosensors: Multi-Anode Photomultipliers (MAPMs) and Silicon Photomultipliers (SiPMs). During November 2015, the GCT MAPM (GCT-M) prototype camera was integrated onto the GCT stru...
arXiv: Instrumentation and Methods for Astrophysics | 2017
L. Tibaldo; A. Abchiche; D. Allan; J. P. Amans; T. Armstrong; A. Balzer; D. Berge; C. Boisson; J. J. Bousquet; A. M. Brown; M. Bryan; Gilles Buchholtz; P. M. Chadwick; H. Costantini; Garret Cotter; M. K. Daniel; A. De Franco; F. De Frondat; Jean-Laurent Dournaux; D. J. P. Dumas; J.-P. Ernenwein; G. Fasola; S. Funk; J. Gironnet; J. A. Graham; T. Greenshaw; O. Hervet; N. Hidaka; J. A. Hinton; Jean-Michel Huet
The Cherenkov Telescope Array (CTA) is a forthcoming ground-based observatory for very-high-energy gamma rays. CTA will consist of two arrays of imaging atmospheric Cherenkov telescopes in the Northern and Southern hemispheres, and will combine telescopes of different types to achieve unprecedented performance and energy coverage. The Gamma-ray Cherenkov Telescope (GCT) is one of the small-sized telescopes proposed for CTA to explore the energy range from a few TeV to hundreds of TeV with a field of view ≳ 8° and angular resolution of a few arcminutes. The GCT design features dual-mirror Schwarzschild-Couder optics and a compact camera based on densely-pixelated photodetectors as well as custom electronics. In this contribution we provide an overview of the GCT project with focus on prototype development and testing that is currently ongoing. We present results obtained during the first on-telescope campaign in late 2015 at the Observatoire de Paris-Meudon, during which we recorded the first Cherenkov ima...
Astronomy and Astrophysics | 2015
A. Abramowski; A. Balzer; D. Berge; M. Bryan; D. Salek; J. Vink
Re-observations with the H.E.S.S. telescope array of the very-high-energy (VHE) source HESS J1018-589 A coincident with the Fermi-LAT
Proceedings of SPIE | 2016
J. L. Dournaux; A. Abchiche; D. Allan; J. P. Amans; T. Armstrong; A. Balzer; D. Berge; C. Boisson; J. J. Bousquet; A. M. Brown; M. Bryan; G. Buchholtz; P. M. Chadwick; H. Costantini; Garret Cotter; L. Dangeon; M. K. Daniel; A. De Franco; F. De Frondat; D. Dumas; J.-P. Ernenwein; G. Fasola; S. Funk; J. Gironnet; J. A. Graham; T. Greenshaw; B. Hameau; O. Hervet; N. Hidaka; J. A. Hinton
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Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2016
Anthony M. Brown; A. Abchiche; D. Allan; J. P. Amans; T. Armstrong; A. Balzer; D. Berge; C. Boisson; J. J. Bousquet; M. Bryan; G. Buchholtz; P. M. Chadwick; H. Costantini; Garret Cotter; M. K. Daniel; A. De Franco; F. De Frondat; J. L. Dournaux; D. Dumas; G. Fasola; S. Funk; J. Gironnet; J. A. Graham; T. Greenshaw; O. Hervet; N. Hidaka; J. A. Hinton; J. M. Huet; I. Jegouzo; T. Jogler
-ray binary 1FGL J1018.6-5856 have resulted in a source detection significance of more than 9
Nuclear Instruments & Methods in Physics Research Section A-accelerators Spectrometers Detectors and Associated Equipment | 2017
J.-L. Dournaux; A. De Franco; P. Laporte; Richard White; T. Greenshaw; H. Sol; A. Abchiche; D. Allan; J. P. Amans; T. Armstrong; A. Balzer; D. Berge; C. Boisson; J. J. Bousquet; A. M. Brown; M. Bryan; G. Buchholtz; P. M. Chadwick; H. Costantini; Garret Cotter; M. K. Daniel; F. De Frondat; D. Dumas; J.-P. Ernenwein; G. Fasola; S. Funk; J. Gaudemard; J. A. Graham; J. Gironnet; O. Hervet
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arXiv: High Energy Astrophysical Phenomena | 2017
H. Abdalla; A. Abramowski; F. Aharonian; F. Ait Benkhali; A. G. Akhperjaniany; T. Andersson; E. O. Angüner; M. Arakawa; M. Arrieta; P. Aubert; M. Backes; A. Balzer; M. Barnard; Y. Becherini; J. Becker Tjus; D. Berge; S. Bernhard; K. Bernlöhr; R. Blackwell; M. Böttcher; C. Boisson; J. Bolmont; S. Bonnefoy; P. Bordas; J. Bregeon; Francois Brun; P. Brun; M. Bryan; M. Büchele; T. Bulik
, and the detection of variability (