377 research outputs found

    Long-term multi-wavelength variability and correlation study of Markarian 421 from 2007 to 2009

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    We study the multi-band variability and correlations of the TeV blazar Mrk 421 on year time scales, which can bring additional insight on the processes responsible for its broadband emission. We observed Mrk 421 in the very high energy (VHE) gamma-ray range with the Cherenkov telescope MAGIC-I from March 2007 to June 2009 for a total of 96 hours of effective time after quality cuts. The VHE flux variability is quantified with several methods, including the Bayesian Block algorithm, which is applied to data from Cherenkov telescopes for the first time. The 2.3 year long MAGIC light curve is complemented with data from the Swift/BAT and RXTE/ASM satellites and the KVA, GASP-WEBT, OVRO, and Mets\"ahovi telescopes from February 2007 to July 2009, allowing for an excellent characterisation of the multi-band variability and correlations over year time scales. Mrk 421 was found in different gamma-ray emission states during the 2.3 year long observation period. Flares and different levels of variability in the gamma-ray light curve could be identified with the Bayesian Block algorithm. The same behaviour of a quiet and active emission was found in the X-ray light curves measured by Swift/BAT and the RXTE/ASM, with a direct correlation in time. The behaviour of the optical light curve of GASP-WEBT and the radio light curves by OVRO and Mets\"ahovi are different as they show no coincident features with the higher energetic light curves and a less variable emission. The fractional variability is overall increasing with energy. The comparable variability in the X-ray and VHE bands and their direct correlation during both high- and low-activity periods spanning many months show that the electron populations radiating the X-ray and gamma-ray photons are either the same, as expected in the Synchrotron-Self-Compton mechanism, or at least strongly correlated, as expected in electromagnetic cascades.Comment: Corresponding authors: Ann-Kristin Overkemping ([email protected]), Marina Manganaro ([email protected]), Diego Tescaro ([email protected]), To be published in Astronomy&Astrophysics (A&A), 12 pages, 9 figure

    A search for spectral hysteresis and energy-dependent time lags from X-ray and TeV gamma-ray observations of Mrk 421

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    Blazars are variable emitters across all wavelengths over a wide range of timescales, from months down to minutes. It is therefore essential to observe blazars simultaneously at different wavelengths, especially in the X-ray and gamma-ray bands, where the broadband spectral energy distributions usually peak. In this work, we report on three "target-of-opportunity" (ToO) observations of Mrk 421, one of the brightest TeV blazars, triggered by a strong flaring event at TeV energies in 2014. These observations feature long, continuous, and simultaneous exposures with XMM-Newton (covering X-ray and optical/ultraviolet bands) and VERITAS (covering TeV gamma-ray band), along with contemporaneous observations from other gamma-ray facilities (MAGIC and Fermi-LAT) and a number of radio and optical facilities. Although neither rapid flares nor significant X-ray/TeV correlation are detected, these observations reveal subtle changes in the X-ray spectrum of the source over the course of a few days. We search the simultaneous X-ray and TeV data for spectral hysteresis patterns and time delays, which could provide insight into the emission mechanisms and the source properties (e.g. the radius of the emitting region, the strength of the magnetic field, and related timescales). The observed broadband spectra are consistent with a one-zone synchrotron self-Compton model. We find that the power spectral density distribution at ≳4×10−4\gtrsim 4\times 10^{-4} Hz from the X-ray data can be described by a power-law model with an index value between 1.2 and 1.8, and do not find evidence for a steepening of the power spectral index (often associated with a characteristic length scale) compared to the previously reported values at lower frequencies.Comment: 45 pages, 15 figure

    ДИНАМИКА АКбИВНОСбИ ĐĐ•ĐšĐžĐąĐžĐ Đ«Đ„ КОМПОНЕНбОВ КОМПЛЕМЕНбА ПРИ ЛЕЧЕНИИ АбОПИЧЕСКОГО ДЕРМАбИбА ĐŁ ДЕбЕЙ

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    The article describes immunoassay methods of determining the functional activity of the components C3 and C9 and C1 inhibitor for diagnostic and prognostic purposes in the treatment of patients. The activity of these components, as well as the activity and the amount of C1 inhibitor in the blood serum of children aged 6 months to 18 years suffering from atopic dermatitis have been analyzed before and after treatment to determine the involvement of the complement system in the pathogenesis of this disease. The developed methods of enzyme immunoassay for determination of the functional components of the complement system have shown high sensitivity and reliability. The activity of C9 component involved in the membrane attack of the complement was significantly below normal in children with atopic dermatitis. That indicates the involvement of membrane attack complex components in the skin necrotic processes. Component C3 activity is also reduced. C3 is the key component of the activation cascade involved in the inflammatory processes. Specific activity of C1 inhibitor increased before and during the treatment, indicating an increased biosynthesis of this acute phase protein. Positive tendency towards the normalization of the status of complement after treatment has been observed. Data obtained in this study indicate the involvement of complement system in the pathological process of atopic dermatitis in children.Đ Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚Đ°ĐœŃ‹ ĐžĐŒĐŒŃƒĐœĐŸŃ„Đ”Ń€ĐŒĐ”ĐœŃ‚ĐœŃ‹Đ” ĐŒĐ”Ń‚ĐŸĐŽŃ‹ ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐžŃ Ń„ŃƒĐœĐșŃ†ĐžĐŸĐœĐ°Đ»ŃŒĐœĐŸĐč Đ°ĐșтоĐČĐœĐŸŃŃ‚Đž ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚ĐŸĐČ ĐĄ3, ĐĄ9 Đž ĐĄ1 ĐžĐœĐłĐžĐ±ĐžŃ‚ĐŸŃ€Đ° ŃĐžŃŃ‚Đ”ĐŒŃ‹ ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° ĐŽĐ»Ń Ń€Đ”ŃˆĐ”ĐœĐžŃ ĐŽĐžĐ°ĐłĐœĐŸŃŃ‚ĐžŃ‡Đ”ŃĐșох Đž ĐżŃ€ĐŸĐłĐœĐŸŃŃ‚ĐžŃ‡Đ”ŃĐșох заЎач про Đ»Đ”Ń‡Đ”ĐœĐžĐž Đ±ĐŸĐ»ŃŒĐœŃ‹Ń…. Đ˜ŃŃĐ»Đ”ĐŽĐŸĐČĐ°ĐœŃ‹ Đ°ĐșтоĐČĐœĐŸŃŃ‚Đž этох ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚ĐŸĐČ, Đ° таĐșжД Đ°ĐșтоĐČĐœĐŸŃŃ‚Đž Đž ĐșĐŸĐ»ĐžŃ‡Đ”ŃŃ‚ĐČĐ° ĐĄ1 ĐžĐœĐłĐžĐ±ĐžŃ‚ĐŸŃ€Đ° ĐČ ŃŃ‹ĐČĐŸŃ€ĐŸŃ‚Đșах ĐșŃ€ĐŸĐČĐž ЎДтДĐč ĐČ ĐČĐŸĐ·Ń€Đ°ŃŃ‚Đ” ĐŸŃ‚ 6 ĐŒĐ”ŃŃŃ†Đ”ĐČ ĐŽĐŸ 18 лДт, Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… Đ°Ń‚ĐŸĐżĐžŃ‡Đ”ŃĐșĐžĐŒ ĐŽĐ”Ń€ĐŒĐ°Ń‚ĐžŃ‚ĐŸĐŒ, ĐŽĐŸ Đž ĐżĐŸŃĐ»Đ” Đ»Đ”Ń‡Đ”ĐœĐžŃ ĐŽĐ»Ń ĐČŃ‹ŃŃĐœĐ”ĐœĐžŃ участоя ŃĐžŃŃ‚Đ”ĐŒŃ‹ ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° ĐČ ĐżĐ°Ń‚ĐŸĐłĐ”ĐœĐ”Đ·Đ” ŃŃ‚ĐŸĐłĐŸ Đ·Đ°Đ±ĐŸĐ»Đ”ĐČĐ°ĐœĐžŃ. Đ Đ°Đ·Ń€Đ°Đ±ĐŸŃ‚Đ°ĐœĐœŃ‹Đ” ĐŒĐ”Ń‚ĐŸĐŽŃ‹ ĐžĐŒĐŒŃƒĐœĐŸŃ„Đ”Ń€ĐŒĐ”ĐœŃ‚ĐœĐŸĐłĐŸ Đ°ĐœĐ°Đ»ĐžĐ·Đ° ĐŽĐ»Ń ĐŸĐżŃ€Đ”ĐŽĐ”Đ»Đ”ĐœĐžŃ Ń„ŃƒĐœĐșŃ†ĐžĐŸĐœĐ°Đ»ŃŒĐœĐŸĐč ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚ĐŸĐČ ŃĐžŃŃ‚Đ”ĐŒŃ‹ ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° ĐżĐŸĐșазалО ĐČŃ‹ŃĐŸĐșую чуĐČстĐČĐžŃ‚Đ”Đ»ŃŒĐœĐŸŃŃ‚ŃŒ Đž ĐœĐ°ĐŽĐ”Đ¶ĐœĐŸŃŃ‚ŃŒ. ĐŁ ЎДтДĐč с Đ°Ń‚ĐŸĐżĐžŃ‡Đ”ŃĐșĐžĐŒ ĐŽĐ”Ń€ĐŒĐ°Ń‚ĐžŃ‚ĐŸĐŒ Đ°ĐșтоĐČĐœĐŸŃŃ‚ŃŒ ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚Đ° ĐĄ9, участĐČŃƒŃŽŃ‰Đ”ĐłĐŸ ĐČ ĐŒĐ”ĐŒĐ±Ń€Đ°ĐœĐœĐŸĐč атаĐșĐ” ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° была ŃŃƒŃ‰Đ”ŃŃ‚ĐČĐ”ĐœĐœĐŸ ĐœĐžĐ¶Đ” ĐœĐŸŃ€ĐŒŃ‹, Ń‡Ń‚ĐŸ уĐșĐ°Đ·Ń‹ĐČаДт ĐœĐ° ŃƒŃ‡Đ°ŃŃ‚ĐžĐ” ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚ĐŸĐČ ĐŒĐ”ĐŒĐ±Ń€Đ°ĐœĐŸĐ°Ń‚Đ°ĐșŃƒŃŽŃ‰Đ”ĐłĐŸ ĐșĐŸĐŒĐżĐ»Đ”Đșса ĐČ ĐŸŃŃƒŃ‰Đ”ŃŃ‚ĐČĐ»Đ”ĐœĐžĐž ĐœĐ”ĐșŃ€ĐŸŃ‚ĐžŃ‡Đ”ŃĐșох ĐżŃ€ĐŸŃ†Đ”ŃŃĐŸĐČ ĐČ ĐŸĐ±Đ»Đ°ŃŃ‚Đž ĐșĐŸĐ¶ĐœŃ‹Ń… ĐżĐŸŃ€Đ°Đ¶Đ”ĐœĐžĐč. ĐĄĐœĐžĐ¶Đ”ĐœĐ° была таĐșжД Đ°ĐșтоĐČĐœĐŸŃŃ‚ŃŒ ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚Đ° ĐĄ3 ĐșлючДĐČĐŸĐłĐŸ ĐșĐŸĐŒĐżĐŸĐœĐ”ĐœŃ‚Đ° ĐșасĐșĐ°ĐŽĐ° Đ°ĐșтоĐČацоо, участĐČŃƒŃŽŃ‰Đ”ĐłĐŸ ĐČ ĐżŃ€ĐŸŃ†Đ”ŃŃĐ°Ń… ĐČĐŸŃĐżĐ°Đ»Đ”ĐœĐžŃ. Đ”ĐŸ Đž ĐČ Ń…ĐŸĐŽĐ” Đ»Đ”Ń‡Đ”ĐœĐžŃ Đ±ĐŸĐ»ŃŒĐœŃ‹Ń… ŃƒĐŽĐ”Đ»ŃŒĐœĐ°Ń Đ°ĐșтоĐČĐœĐŸŃŃ‚ŃŒ ĐĄ1 ĐžĐœĐłĐžĐ±ĐžŃ‚ĐŸŃ€Đ° была ĐżĐŸĐČŃ‹ŃˆĐ”ĐœĐ°, Ń‡Ń‚ĐŸ сĐČĐžĐŽĐ”Ń‚Đ”Đ»ŃŒŃŃ‚ĐČĐŸĐČĐ°Đ»ĐŸ ĐŸ ĐżĐŸĐČŃ‹ŃˆĐ”ĐœĐœĐŸĐŒ Đ±ĐžĐŸŃĐžĐœŃ‚Đ”Đ·Đ” ŃŃ‚ĐŸĐłĐŸ бДлĐșĐ°, яĐČĐ»ŃŃŽŃ‰Đ”ĐłĐŸŃŃ бДлĐșĐŸĐŒ ĐŸŃŃ‚Ń€ĐŸĐč Ń„Đ°Đ·Ń‹. ĐŸŃ€ĐŸŃĐ»Đ”Đ¶ĐžĐČаются ĐżĐŸĐ·ĐžŃ‚ĐžĐČĐœŃ‹Đ” сЎĐČОгО ĐČ ŃŃ‚ĐŸŃ€ĐŸĐœŃƒ ĐœĐŸŃ€ĐŒĐ°Đ»ĐžĐ·Đ°Ń†ĐžĐž статуса ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° ĐżĐŸŃĐ»Đ” Đ»Đ”Ń‡Đ”ĐœĐžŃ. ĐŸĐŸĐ»ŃƒŃ‡Đ”ĐœĐœŃ‹Đ” ĐČ Ń€Đ°Đ±ĐŸŃ‚Đ” ĐŽĐ°ĐœĐœŃ‹Đ” уĐșĐ°Đ·Ń‹ĐČают ĐœĐ° ŃƒŃ‡Đ°ŃŃ‚ĐžĐ” ŃĐžŃŃ‚Đ”ĐŒŃ‹ ĐșĐŸĐŒĐżĐ»Đ”ĐŒĐ”ĐœŃ‚Đ° ĐČ ĐżĐ°Ń‚ĐŸĐ»ĐŸĐłĐžŃ‡Đ”ŃĐșĐŸĐŒ ĐżŃ€ĐŸŃ†Đ”ŃŃĐ” про Đ°Ń‚ĐŸĐżĐžŃ‡Đ”ŃĐșĐŸĐŒ ĐŽĐ”Ń€ĐŒĐ°Ń‚ĐžŃ‚Đ” у ЎДтДĐč.

    Caenorhabditis elegans: a model to monitor bacterial air quality

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    <p>Abstract</p> <p>Background</p> <p>Low environmental air quality is a significant cause of mortality and morbidity and this question is now emerging as a main concern of governmental authorities. Airborne pollution results from the combination of chemicals, fine particles, and micro-organisms quantitatively or qualitatively dangerous for health or for the environment. Increasing regulations and limitations for outdoor air quality have been decreed in regards to chemicals and particles contrary to micro-organisms. Indeed, pertinent and reliable tests to evaluate this biohazard are scarce. In this work, our purpose was to evaluate the <it>Caenorhaditis elegans </it>killing test, a model considered as an equivalent to the mouse acute toxicity test in pharmaceutical industry, in order to monitor air bacterial quality.</p> <p>Findings</p> <p>The present study investigates the bacterial population in dust clouds generated during crop ship loading in harbor installations (Rouen harbor, Normandy, France). With a biocollector, airborne bacteria were impacted onto the surface of agar medium. After incubation, a replicate of the colonies on a fresh agar medium was done using a velvet. All the replicated colonies were pooled creating the "Total Air Sample". Meanwhile, all the colonies on the original plate were isolated. Among which, five representative bacterial strains were chosen. The virulence of these representatives was compared to that of the "Total Air Sample" using the <it>Caenorhaditis elegans </it>killing test. The survival kinetic of nematodes fed with the "Total Air Sample" is consistent with the kinetics obtained using the five different representatives strains.</p> <p>Conclusions</p> <p>Bacterial air quality can now be monitored in a one shot test using the <it>Caenorhaditis elegans </it>killing test.</p

    Detection of very high energy gamma-ray emission from the gravitationally-lensed blazar QSO B0218+357 with the MAGIC telescopes

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    Context. QSO B0218+357 is a gravitationally lensed blazar located at a redshift of 0.944. The gravitational lensing splits the emitted radiation into two components, spatially indistinguishable by gamma-ray instruments, but separated by a 10-12 day delay. In July 2014, QSO B0218+357 experienced a violent flare observed by the Fermi-LAT and followed by the MAGIC telescopes. Aims. The spectral energy distribution of QSO B0218+357 can give information on the energetics of z ~ 1 very high energy gamma- ray sources. Moreover the gamma-ray emission can also be used as a probe of the extragalactic background light at z ~ 1. Methods. MAGIC performed observations of QSO B0218+357 during the expected arrival time of the delayed component of the emission. The MAGIC and Fermi-LAT observations were accompanied by quasi-simultaneous optical data from the KVA telescope and X-ray observations by Swift-XRT. We construct a multiwavelength spectral energy distribution of QSO B0218+357 and use it to model the source. The GeV and sub-TeV data, obtained by Fermi-LAT and MAGIC, are used to set constraints on the extragalactic background light. Results. Very high energy gamma-ray emission was detected from the direction of QSO B0218+357 by the MAGIC telescopes during the expected time of arrival of the trailing component of the flare, making it the farthest very high energy gamma-ray sources detected to date. The observed emission spans the energy range from 65 to 175 GeV. The combined MAGIC and Fermi-LAT spectral energy distribution of QSO B0218+357 is consistent with current extragalactic background light models. The broad band emission can be modeled in the framework of a two zone external Compton scenario, where the GeV emission comes from an emission region in the jet, located outside the broad line region.Comment: 11 pages, 6 figures, accepted for publication in A&

    Investigating the peculiar emission from the new VHE gamma-ray source H1722+119

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    The MAGIC (Major Atmospheric Gamma-ray Imaging Cherenkov) telescopes observed the BL Lac object H1722+119 (redshift unknown) for six consecutive nights between 2013 May 17 and 22, for a total of 12.5 h. The observations were triggered by high activity in the optical band measured by the KVA (Kungliga Vetenskapsakademien) telescope. The source was for the first time detected in the very high energy (VHE, E>100E > 100 GeV) Îł\gamma-ray band with a statistical significance of 5.9 σ\sigma. The integral flux above 150 GeV is estimated to be (2.0±0.5)(2.0\pm 0.5) per cent of the Crab Nebula flux. We used contemporaneous high energy (HE, 100 MeV <E<100 < E < 100 GeV) Îł\gamma-ray observations from Fermi-LAT (Large Area Telescope) to estimate the redshift of the source. Within the framework of the current extragalactic background light models, we estimate the redshift to be z=0.34±0.15z = 0.34 \pm 0.15. Additionally, we used contemporaneous X-ray to radio data collected by the instruments on board the Swift satellite, the KVA, and the OVRO (Owens Valley Radio Observatory) telescope to study multifrequency characteristics of the source. We found no significant temporal variability of the flux in the HE and VHE bands. The flux in the optical and radio wavebands, on the other hand, did vary with different patterns. The spectral energy distribution (SED) of H1722+119 shows surprising behaviour in the ∌3×1014−1018\sim 3\times10^{14} - 10^{18} Hz frequency range. It can be modelled using an inhomogeneous helical jet synchrotron self-Compton model.Comment: 12 pages, 5 figures, 2 table

    Anisotropy and chemical composition of ultra-high energy cosmic rays using arrival directions measured by the Pierre Auger Observatory

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    The Pierre Auger Collaboration has reported evidence for anisotropy in the distribution of arrival directions of the cosmic rays with energies E>Eth=5.5×1019E>E_{th}=5.5\times 10^{19} eV. These show a correlation with the distribution of nearby extragalactic objects, including an apparent excess around the direction of Centaurus A. If the particles responsible for these excesses at E>EthE>E_{th} are heavy nuclei with charge ZZ, the proton component of the sources should lead to excesses in the same regions at energies E/ZE/Z. We here report the lack of anisotropies in these directions at energies above Eth/ZE_{th}/Z (for illustrative values of Z=6, 13, 26Z=6,\ 13,\ 26). If the anisotropies above EthE_{th} are due to nuclei with charge ZZ, and under reasonable assumptions about the acceleration process, these observations imply stringent constraints on the allowed proton fraction at the lower energies
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