45 results on '"C. Done"'
Search Results
2. X-ray/UV/optical variability of NGC 4593 with Swift: reprocessing of X-rays by an extended reprocessor
- Author
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I M McHardy, S D Connolly, K Horne, E M Cackett, J Gelbord, B M Peterson, M Pahari, N Gehrels, M Goad, P Lira, P Arevalo, R D Baldi, N Brandt, E Breedt, H Chand, G Dewangan, C Done, M Elvis, D Emmanoulopoulos, M M Fausnaugh, S Kaspi, C S Kochanek, K Korista, I E Papadakis, A R Rao, P Uttley, M Vestergaard, and M J Ward
- Published
- 2018
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3. Origins of the UV/X-ray relation in Arakelian 120
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R D Mahmoud, C Done, D Porquet, A Lobban, Laboratoire d'Astrophysique de Marseille (LAM), and Aix Marseille Université (AMU)-Institut national des sciences de l'Univers (INSU - CNRS)-Centre National d'Études Spatiales [Toulouse] (CNES)-Centre National de la Recherche Scientifique (CNRS)
- Subjects
High Energy Astrophysical Phenomena (astro-ph.HE) ,Space and Planetary Science ,black hole physics ,galaxies: active ,galaxies: individual: Ark 120 ,FOS: Physical sciences ,accretion, accretion discs ,Astronomy and Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena ,[PHYS.ASTR]Physics [physics]/Astrophysics [astro-ph] - Abstract
We explore the accretion geometry in Arakelian 120 using intensive UV and X-ray monitoring from \textit{Swift}. The hard X-rays ($1-10$ keV) show large amplitude, fast (few-day) variability, so we expect reverberation from the disc to produce UV variability from the varying hard X-ray illumination. We model the spectral energy distribution including an outer standard disc (optical), an intermediate warm Comptonisation region (UV and soft X-ray) and a hot corona (hard X-rays). Unlike the lower Eddington fraction AGN (NGC 4151 and NGC 5548 at $L/L_{Edd}\sim 0.02$ and $0.03$ respectively), the SED of Akn 120 ($L\sim 0.05L_{Edd}$) is dominated by the UV, restricting the impact of reverberating hard X-rays by energetics alone. Illumination from a hard X-ray corona with height $\sim10 R_g$ produces minimal UV variability. Increasing the coronal scale height to $\sim 100 R_g$ improves the match to the observed amplitude of UV variability as the disc subtends a larger solid angle, but results in too much fast variability to match the UV data. The soft X-rays (connected to the UV in the warm Comptonisation model) are more variable than the hard, but again contain too much fast variability to match the observed smoother variability seen in the UV. Results on lower Eddington fraction AGN have emphasised the contribution from reverberation from larger scales (the broad line region), but reverberation induces lags on similar timescales to the smoothing, producing a larger delay than is compatible with the data. We conclude that the majority of the UV variability is therefore intrinsic, connected to mass accretion rate fluctuations in the warm Comptonisation region., Accepted in MNRAS
- Published
- 2022
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4. A multi-wavelength view of distinct accretion regimes in the pulsating ultraluminous X-ray source NGC 1313 X-2
- Author
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R Sathyaprakash, T P Roberts, F Grisé, P Kaaret, E Ambrosi, C Done, J C Gladstone, J J E Kajava, R Soria, L Zampieri, Agenzia Spaziale Italiana, Istituto Nazionale di Astrofisica, and National Aeronautics and Space Administration (US)
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High Energy Astrophysical Phenomena (astro-ph.HE) ,Astrophysics::High Energy Astrophysical Phenomena ,FOS: Physical sciences ,neutron [Stars] ,Astronomy and Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Stars: neutron ,X-rays: binaries ,Space and Planetary Science ,Astrophysics::Solar and Stellar Astrophysics ,binaries [X-rays] ,Astrophysics::Earth and Planetary Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena ,Accretion discs ,Astrophysics::Galaxy Astrophysics - Abstract
NGC 1313 X-2 is one of the few known pulsating ultraluminous X-ray sources (PULXs), and so is thought to contain a neutron star that accretes at highly super-Eddington rates. However, the physics of this accretion remains to be determined. Here, we report the results of two simultaneous XMM-Newton and HST observations of this PULX taken to observe two distinct X-ray behaviours as defined from its Swift light curve. We find that the X-ray spectrum of the PULX is best described by the hard ultraluminous regime during the observation taken in the lower flux, lower variability amplitude behaviour; its spectrum changes to a broadened disc during the higher flux, higher variability amplitude epoch. However, we see no accompanying changes in the optical/UV fluxes, with the only difference being a reduction in flux in the near-infrared (NIR) as the X-ray flux increased. We attempt to fit irradiation models to explain the UV/optical/IR fluxes but they fail to provide meaningful constraints. Instead, a physical model for the system leads us to conclude that the optical light is dominated by a companion O/B star, albeit with an IR excess that may be indicative of a jet. We discuss how these results may be consistent with the precession of the inner regions of the accretion disc leading to changes in the observed X-ray properties, but not the optical, and whether we should expect to observe reprocessed emission from ULXs., RS gratefully acknowledges the receipt of a studentship grant from the STFC ST/N50404X/1. TPR was funded as part of the STFC consolidated grant ST/K000861/1. RS is extremely grateful for the guidance provided by Andrew Dolphin on HST data analysis. [...] EA acknowledges funding from the Italian Space Agency, contract ASI/INAF n. I/004/11/4. LZ acknowledges financial support from the Italian Space Agency (ASI) and National Institute for Astrophysics (INAF) under agreements ASI-INAF I/037/12/0 and ASI-INAF n.2017-14-H.0 and from INAF ’Sostegno alla ricerca scientifica main streams dell’INAF’ Presidential Decree 43/2018. RS acknowledges grant number 12073029 from the National Science Foundation of China.
- Published
- 2022
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5. The First Swift Intensive AGN Accretion Disk Reverberation Mapping Survey
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R. Edelson, J. Gelbord, E. Cackett, B. M. Peterson, Keith Horne, A. J. Barth, D. A. Starkey, M. Bentz, W. N. Brandt, M. Goad, M. Joner, K. Korista, H. Netzer, K. Page, P. Uttley, S. Vaughan, A. Breeveld, S. B. Cenko, C. Done, P. Evans, M. Fausnaugh, G. Ferland, D. Gonzalez-Buitrago, J. Gropp, D. Grupe, J. Kaastra, J. Kennea, G. Kriss, S. Mathur, M. Mehdipour, D. Mudd, J. Nousek, T. Schmidt, M. Vestergaard, and C. Villforth
- Subjects
Astrophysics - Abstract
Swift intensive accretion disk reverberation mapping of four AGN yielded light curves sampled ∼200–350 times in 0.3–10 keV X-ray and six UV/optical bands. Uniform reduction and cross-correlation analysis of these data sets yields three main results: (1) The X-ray/UV correlations are much weaker than those within the UV/optical, posing severe problems for the lamp-post reprocessing model in which variations in a central X-ray corona drive and power those in the surrounding accretion disk. (2) The UV/optical interband lags are generally consistent with t μ l4 3 as predicted by the centrally illuminated thin accretion disk model. While the average interband lags are somewhat larger than predicted, these results alone are not inconsistent with the thin disk model given the large systematic uncertainties involved. (3) The one exception is the U band lags, which are on average a factor of ∼2.2 larger than predicted from the surrounding band data and fits. This excess appears to be due to diffuse continuum emission from the broad-line region (BLR). The precise mixing of disk and BLR components cannot be determined from these data alone. The lags in different AGN appear to scale with mass or luminosity. We also find that there are systematic differences between the uncertainties derived by JAVELIN versus more standard lag measurement techniques, with JAVELIN reporting smaller uncertainties by a factor of 2.5 on average. In order to be conservative only standard techniques were used in the analyses reported herein.
- Published
- 2019
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6. Localized thermonuclear bursts from accreting magnetic white dwarfs
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S. Scaringi, P. J. Groot, C. Knigge, A. J. Bird, E. Breedt, D. A. H. Buckley, Y. Cavecchi, N. D. Degenaar, D. de Martino, C. Done, M. Fratta, K. Iłkiewicz, E. Koerding, J.-P. Lasota, C. Littlefield, C. F. Manara, M. O’Brien, P. Szkody, F. X. Timmes, High Energy Astrophys. & Astropart. Phys (API, FNWI), and GBR
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High Energy Astrophysical Phenomena (astro-ph.HE) ,Multidisciplinary ,Astrophysics - Solar and Stellar Astrophysics ,Astrophysics::High Energy Astrophysical Phenomena ,Astronomy ,FOS: Physical sciences ,Astrophysics::Solar and Stellar Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics::Earth and Planetary Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena ,Solar and Stellar Astrophysics (astro-ph.SR) ,Astrophysics::Galaxy Astrophysics - Abstract
Nova explosions are caused by global thermonuclear runaways triggered in the surface layers of accreting white dwarfs. It has been predicted that localised thermonuclear bursts on white dwarfs can also take place, similar to Type I X-ray bursts observed in accreting neutron stars. Unexplained rapid bursts from the binary system TV Columbae, in which mass is accreted onto a moderately-strong magnetised white dwarf from a low-mass companion, have been observed on several occasions in the past $\approx40$ years. During these bursts the optical/UV luminosity increases by a factor of $>3$ in less than an hour and fades over $\approx10$ hours. Fast outflows have been observed in UV spectral lines, with velocities $>3500$ km s$^{-1}$, comparable to the escape velocity from the white dwarf surface. Here we report on optical bursts observed in TV Columbae as well as in two additional accreting systems, EI Ursae Majoris and ASASSN-19bh. The bursts have a total energy $\approx~10^{-6}$ those of classical nova explosions ("micronovae"), and bear a strong resemblance to Type I X-ray bursts. We exclude accretion or stellar magnetic reconnection events as their origin and suggest thermonuclear runaway events in magnetically-confined accretion columns as a viable explanation., 11 pages, 7 figures. Submitted on 4 October 2021. Accepted for publication in Nature on 1 February 2022
- Published
- 2022
7. EXISTENCE AND UNIQUENESS OF SOLUTION OF FIRST ORDER DIFFERENCE EQUATION OF FINITE DELAY IN CONE METRIC SPACE
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P. U. Chopade, G. C. Done, and K. L. Bondar
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Metric space ,Cone (topology) ,Differential equation ,General Mathematics ,Mathematical analysis ,Uniqueness ,First order ,Mathematics - Published
- 2020
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8. Frontiers in accretion physics at high X-ray spectral resolution
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P. Gandhi, T. Kawamuro, M. Díaz Trigo, J. A. Paice, P. G. Boorman, M. Cappi, C. Done, A. C. Fabian, K. Fukumura, J. A. García, C. L. Greenwell, M. Guainazzi, K. Makishima, M. S. Tashiro, R. Tomaru, F. Tombesi, and Y. Ueda
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Settore FIS/05 ,Astronomy and Astrophysics - Published
- 2022
9. Localized thermonuclear bursts from accreting magnetic white dwarfs
- Author
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S, Scaringi, P J, Groot, C, Knigge, A J, Bird, E, Breedt, D A H, Buckley, Y, Cavecchi, N D, Degenaar, D, de Martino, C, Done, M, Fratta, K, Iłkiewicz, E, Koerding, J-P, Lasota, C, Littlefield, C F, Manara, M, O'Brien, P, Szkody, and F X, Timmes
- Abstract
Nova explosions are caused by global thermonuclear runaways triggered in the surface layers of accreting white dwarfs
- Published
- 2021
10. Existence and Uniqueness Results of Second Order Summation–Difference Equations in Cone Metric Space
- Author
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K. L. Bondar, G. C. Done, and P. U. Chopade
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Metric space ,Cone (topology) ,Mathematical analysis ,Order (group theory) ,Uniqueness ,Type (model theory) ,Contraction principle ,Mathematics - Abstract
In this paper, we investigate the existence and uniqueness results for summation–difference type equations in cone metric spaces. The results are obtained by using some extensions of Banach’s contraction principle in a complete cone metric space.
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- 2021
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11. High performance recycled CFRP composites based on reused carbon fabrics through sustainable mild solvolysis route
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W. Ballout, N. Sallem-Idrissi, M. Sclavons, C. Doneux, C. Bailly, T. Pardoen, and P. Van Velthem
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Medicine ,Science - Abstract
Abstract A novel environmentally friendly recycling method is developed for large carbon-fibers reinforced-polymers composite panels whose efficiency is demonstrated through a proof-of-concept fabrication of a new composite part based on recycled fibers. The recycling process relies on formic acid as separation reagent at room temperature and atmospheric pressure with efficient recycling potential of the separating agent. Electron microscopy and thermal analysis indicate that the recycled fibers are covered by a thin layer of about 10wt.% of residual resin, alternating with few small particles, as compared to the smooth virgin fibers. The recycled composites show promising shear strength and compression after impact strength, with up to 93% retention of performance depending on the property as compared to the reference. The recycled carbon fibers can thus be reused for structural applications requiring moderate to high performances. The loss of properties is attributed to a lower adhesion between fresh epoxy resin and recycled carbon fibers due to the absence of sizing, partly compensated by a good interface between fresh and residual cured epoxy thanks to mechanical anchoring as well as chemical reactions. The room temperature and atmospheric pressure operating conditions combined to the recyclability of the forming acid contribute to the sustainability of the entire approach.
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- 2022
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12. Novel Methylpalladium(II) Complexes Bearing Tridentate Imidazole-Based Chelate Ligands: Synthesis, Structural Characterization, and Reactivity
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Allan H. White, Kingsley J. Cavell, Brian W. Skelton, Evan J. Peacock, Thomas Rüther, and Melanie C. Done
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chemistry.chemical_classification ,Chemistry ,Stereochemistry ,Ligand ,Dimer ,Organic Chemistry ,Crystal structure ,Coordination complex ,Inorganic Chemistry ,chemistry.chemical_compound ,Crystallography ,Imidazole ,Moiety ,Reactivity (chemistry) ,Physical and Theoretical Chemistry ,Organometallic chemistry - Abstract
Novel methylpalladium(II) complexes of the general composition [PdCl(CH3){N∧D∧N}] ({N∧D∧N} = (mim)3COCH3 (1a), (mim)2CHCH2C(O)Bu-t (3a)) were synthesized from [PdCl(CH3)(COD)] and the respective N-methylimidazole (mim) ligands. The cationic derivatives [Pd2(CH3)2{N∧D∧N}2](BF4)2 (1b; {N∧D∧N} = (mim)3COCH3) and [Pd(CH3){N∧D∧N)(CH3CN)](BF4) (3b; {N∧D∧N} = (mim)2CHCH2C(O)Bu-t) were obtained by halide abstraction with AgBF4. The effect of varying the third donor moiety (D = “O”, “N”, “P”) in the structurally very similar ligands on the coordination chemistry and reactivity of 1 and 3 and the previously reported [PdCl(CH3){N∧D∧N}] (2a; {N∧D∧N} = (mim)2CHCH2PPh2) was investigated in detail. Thus, a neutral monomeric and an ionic dimeric isomer were identified for 1a, with the ligand adopting a σ2-N∧N coordination mode in the former and a σ3-N∧N∧N coordination mode in the latter. Exclusive formation of the ionic dimer occurs in methanol. Crystal structures are recorded for 1b and [Pd2Cl(CH3){N∧N∧N}2]Cl2 (1c). Eac...
- Published
- 2001
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13. Novel cationic and neutral Pd(II) complexes bearing imidazole based chelate ligands: synthesis, structural characterisation and catalytic behaviour
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Melvyn Kilner, Thomas Rüther, Allan H. White, Kingsley J. Cavell, Melanie C. Done, Evan J. Peacock, Nathalie Braussaud, and Brian W. Skelton
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Stereochemistry ,Organic Chemistry ,Cyclohexane conformation ,Cationic polymerization ,chemistry.chemical_element ,Bite angle ,Biochemistry ,Medicinal chemistry ,Inorganic Chemistry ,NMR spectra database ,chemistry.chemical_compound ,chemistry ,Heck reaction ,Materials Chemistry ,Imidazole ,Physical and Theoretical Chemistry ,Organometallic chemistry ,Palladium - Abstract
A variety of neutral and cationic methyl palladium(II) complexes [Pd(CH 3 )(Cl)(L–L)] ( 3 ) and [Pd(CH 3 )(CH 3 CN)(L–L)]BF 4 ( 4 ), containing known and new N -methylimidazole-2-yl (mim) and N -methylbenzimidazole-2-yl (bmim) based chelate ligands (L–L) have been synthesised. The dichloro complexes [Pd(Cl) 2 {(mim) 2 CO}] ( 2b ) and [Pd(Cl) 2 (mim)PPh 2 ] ( 2e ) have also been synthesised. The crystal structures of [Pd(Cl) 2 {(mim) 2 CNPh}] ( 2d ) and [Pd(CH 3 )(Cl){(bmim) 2 CO}] ( 3c ) have been determined and show a square planar geometry at palladium(II) with an appreciable diminished bite angle (85.6°) in 3c compared to 2d (88.5°). The molecular structure of 2d and 3c show both bisimidazole ligands coordinated via the ring nitrogen donors and inclination of the chelate ring bridge to the coordination plane (boat conformation). Low temperature NMR spectra indicate boat-to-boat inversion of the chelate ring in [Pd(CH 3 )(CH 3 CN){(mim) 2 CO}] + ( 4b ). Examples of the neutral and cationic complexes were tested in the Heck reaction and CO/ethylene copolimerisation respectively. The CO bridged bisimidazole complex ( 3b ) exhibited high activity (TON of 100 000) in the Heck reaction whereas the closely related benzimidazole complex 3c was about half as active (TON of 53 000). Low activities were found for the cationic complex 4b in the CO/ethylene copolymerisation (TON 449).
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- 2000
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14. The Hard X-Ray Spectra of EF Eri and Other CVs
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C. Done, J. P. Osborne, and A. P. Beardmore
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Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics::Solar and Stellar Astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
Reflection of the X-ray emission from the surface of the white dwarf should be present in all hard X-ray emitting CV systems. It is clearly identified in the Ginga 2… 20 keV spectra of the polars AM Her and EF Eri, and also in the quiescent spectra of the dwarf novae SS Cyg. The inclusion of the hard reflection spectrum lowers the derived continuum temperature, so resolving a long standing problem of the mismatch of the iron line and continuum properties, and, with more realistic multi-temperature continuua, the derived shock temperatures are close to those expected from theoretical models of a strong shock.
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- 1996
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15. Carbon–oxygen bond formation at organopalladium centres
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Allan H. White, Brian W. Skelton, Allan J. Canty, and Melanie C. Done
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Inorganic chemistry ,chemistry.chemical_element ,Crystal structure ,Medicinal chemistry ,2,2'-Bipyridine ,Catalysis ,Inorganic Chemistry ,chemistry.chemical_compound ,chemistry ,Organopalladium ,Materials Chemistry ,Physical and Theoretical Chemistry ,Organometallic chemistry ,Carbon–oxygen bond ,Methyl group ,Palladium - Abstract
The reaction of PdMe2(bpy) (bpy = 2,2-bipyridine) with diaroyl peroxides is a complex process in which initial oxidation of Pd(II) is followed by methyl group exchange between an undetected Pd(IV) intermediate and PdMe2(bpy) to give PdMe(O2CAr)(bpy) and PdMe3(O2CAr)(bpy); the latter Pd(IV) complex decomposes by elimination of Me–Me to give additional PdMe(O2CAr)(bpy) which reacts with (ArCO2)2 to give Me–O2CAr and Pd(O2CAr)2(bpy). The complexes Pd(O2CPh)2(L2) (L2=bpy, N,N,N′,N′-tetramethylethylyenediamine) have been characterised by X-ray diffraction.
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- 2001
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16. The Ultraluminous State
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T. P. Roberts, J. C. Gladstone, L. M. Hetf, C. Done, S. A. Vaughan, A. Comastri, L. Angelini, and M. Cappi
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Physics ,Photosphere ,Brightness ,Stellar mass ,Astrophysics::High Energy Astrophysical Phenomena ,X-ray binary ,Astronomy ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics ,Corona ,Spectral line ,Accretion (astrophysics) ,Black hole ,Astrophysics::Solar and Stellar Astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
Although a great deal of progress has been made towards understanding the nature of ultraluminous X‐ray sources (ULXs) over the past decade, many basic issues remain to be settled. Chief amongst these is the mass of the accretor in these systems: what proportion of ULXs are powered by accretion onto an intermediate‐mass black hole (IMBH), and how big are these objects? Or can we explain their extraordinary X‐ray luminosities by exotic, extreme accretion rate processes onto more prosaic stellar‐mass black holes? Here we report the results of two new studies using the best available XMM‐Newton observations to probe the astrophysics of ULXs. A systematic study of ULX power spectra shows a significant proportion of luminous objects with unusually suppressed variability compared to standard black hole binaries and AGN. Furthermore, detailed spectral studies confirm that ULX spectra appear unlike any standard accretion state in the XMM‐Newton band pass. Hence we infer that many ULXs contain small black holes operating in a new, super‐Eddington “ultraluminous” accretion state. We show that ULX spectra appear to vary with accretion rate, being closest to standard states at around Eddington, with an optically thick corona becoming the characteristic feature as we reach super‐Eddington rates. At the highest rates we see evidence for the emergence of a cool photosphere, likely related to a massive outflowing wind.
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- 2010
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17. Suzaku wide-band observations of black-hole binaries and AGNs: continuum and Fe-K lines
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Shin’ya Yamada, K. Makishima, K. Nakazawa, H. Noda, H. Takahashi, T. Dotani, A. Kubota, K. Ebisawa, Y. Ueda, C. Done, A. Comastri, L. Angelini, and M. Cappi
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Black hole ,Physics ,Thermal ,Continuum (design consultancy) ,Astronomy ,Astrophysics ,Wide band ,Spectral component ,Galactic nuclei ,Spectral line ,Line (formation) - Abstract
Suzaku has enabled us to study wide‐band spectral and timing properties of black‐hole binaries and AGNs more accurately than ever, and revealed how the continuum definition can affect Fe‐Kline profiles. We have reproduced 0.5–300 keV spectra of Cyg X‐1 and GRO J1655‐40 in terms of thermal Comptonization in highly inhomogeneous coronae. In both objects, Rin was constrained by the Fe‐K line profile and soft excess as ∼10 Rg, as opposed to the relativistic Fe‐K line reported in the literature. We also re‐analyzed the 0.7–300 keV Suzaku spectra of GX 339‐4, and found that a careful modeling of the continuum leads to Rin>Rg(Yamada et al. 2009), again in disagreement with Miller et al. (2008). Furthermore, through a systematic analysis of AGNs, we discovered a hard spectral component in the HXD‐PIN band, which varies independently of the powerlaw. Taking this into account, the time‐averaged spectra of MCG‐6‐30‐15 have been explained by invoking neither a large refection fraction, nor an extreme broad Fe‐K line....
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- 2010
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18. The X-ray Binary Analogy to the First AGN QPO
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M. Middleton, C. Done, M. Gierliński, A. Comastri, L. Angelini, and M. Cappi
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Physics ,High Energy Astrophysical Phenomena (astro-ph.HE) ,Brightness ,Astrophysics::High Energy Astrophysical Phenomena ,X-ray binary ,Spectral density ,FOS: Physical sciences ,Astrophysics ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Galactic nuclei ,Mass scaling ,Astrophysics - High Energy Astrophysical Phenomena ,X ray spectra ,Astrophysics::Galaxy Astrophysics - Abstract
The Narrow Line Seyfert 1 galaxy REJ1034+396 is so far unique amongst AGN in showing a Quasi-periodic oscillation (QPO) in its variability power spectrum. There are multiple types of QPO seen in black hole binary (BHB) systems, so we need to identify which BHB QPO corresponds to the one seen in the AGN. A key hint is the `hot disc dominated' energy spectrum of REJ1034+396 which is sufficiently unusual that it suggests a mildly super-Eddington flow, also favoured by the most recent mass estimates for the AGN. This suggests the 67Hz QPO seen occasionally in the mildly super-Eddington BHB GRS 1915+105 as the most likely counterpart, assuming mass scaling of the QPO frequency. This is supported by the fact that these data from GRS 1915+105 have an energy spectrum which is also dominated by a `hot disc' component. Here we show that the underlying broad band power spectral shape and normalisation are also similar, providing further consistency checks for this identification. Thus the AGN QPO adds to the growing evidence for a simple mass scaling of the accretion flow properties between stellar and supermassive black holes., 9 pages, 12 figures, to be published in MNRAS
- Published
- 2009
19. Nephrin is involved in podocyte maturation but not survival during glomerular development
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Karl Tryggvason, S. C. Done, Ying Sun, Minoru Takemoto, Kjell Hultenby, Liqun He, and Christer Betsholtz
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medicine.medical_specialty ,Organogenesis ,congenital nephrotic syndrome ,Kidney Glomerulus ,glomerulus ,Biology ,urologic and male genital diseases ,Podocyte ,Nephrin ,Mice ,Internal medicine ,medicine ,Animals ,Claudin-3 ,Claudin ,Regulation of gene expression ,Mice, Knockout ,urogenital system ,Podocytes ,Glomerular basement membrane ,Gene Expression Regulation, Developmental ,Membrane Proteins ,nephrin ,female genital diseases and pregnancy complications ,Cell biology ,Up-Regulation ,Endocrinology ,medicine.anatomical_structure ,Membrane protein ,Nephrology ,Knockout mouse ,biology.protein ,Slit diaphragm - Abstract
Nephrin, a major component of the glomerular slit diaphragm (SD), is both a structural protein as well as a signaling molecule influencing foot process (FP) formation and maintenance of podocyte integrity. Analyses of near-term embryonic kidneys showed normal cellular viability and no apoptosis in glomeruli from nephrin knockout mice. Moreover, expression and location of other SD or glomerular basement membrane components were similar in wild-type and mutant mice as was the location and levels of most podocyte-specific proteins. Transcriptional profiling showed that the lack of nephrin had minor impact on the expression of genes for FPs and SD proteins. Claudin 3, a tight-junction protein normally absent in glomeruli, was upregulated threefold in the knockout mice, suggesting a role of nephrin in claudin 3 gene expression within the glomeruli. Our results suggest that nephrin is expressed late in the process of podocyte differentiation and is a locus for the formation of SD and FP maintenance and physical integrity in vivo. Nephrin does not seem to have a primary role in cell survival but has a small impact on gene regulation during glomerular development.
- Published
- 2007
20. Testing models of X-ray reflection from irradiated disks
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C. Done and S. Nayakshin
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Physics ,Active galactic nucleus ,Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics (astro-ph) ,FOS: Physical sciences ,Astronomy and Astrophysics ,Astrophysics ,Nova (laser) ,Spectral line ,Black hole ,Orbit ,Space and Planetary Science ,Ionization ,Reflection (physics) ,Astrophysics::Solar and Stellar Astrophysics ,Irradiation ,Astrophysics::Earth and Planetary Astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
We model the reflected spectrum expected from localized magnetic flares above an ionised accretion disk. We concentrate on the case of very luminous magnetic flares above a standard accretion disk extending down to the last stable orbit, and use a simple parameterisation to allow for an X-ray driven wind. Full disk spectra including relativistic smearing are calculated. When fit with the constant density reflection models, these spectra give both a low reflected fraction and a small line width as seen in the hard spectra from Galactic Black Hole Binaries and Active Galactic Nuclei. We fit our calculated spectra to real data from the low/hard state of Nova Muscae and Cyg X-1 and show that these models give comparable $\chi^2$ to those obtained from the constant density reflection models which implied a truncated disk. This explicitally demonstrates that the data are consistent with either magnetic flares above an ionized disk extending down to the last stable orbit around a black hole, or with non-ionized, truncated disks., Comment: 8 pages, accepted for publication in MNRAS
- Published
- 2001
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21. Transfer of the Illusion of Control Between two Gambling Tasks
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Kenny R. Coventry and C Done
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Illusion of control ,Experimental and Cognitive Psychology ,Psychology ,Cognitive psychology - Published
- 2000
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22. Complex Absorption and Reflection of a Multi-temperature Cyclotron-Bremsstrahlung X-ray Cooling Shock in BY Cam
- Author
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P. Magdziarz and C. Done
- Subjects
Physics ,Solar mass ,Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics (astro-ph) ,Cyclotron ,Bremsstrahlung ,Electron shell ,FOS: Physical sciences ,White dwarf ,Astronomy and Astrophysics ,Astrophysics ,Plasma ,Power law ,Spectral line ,law.invention ,Space and Planetary Science ,law ,Astrophysics::Solar and Stellar Astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
We re-analyse the ASCA and GINGA X-ray data from BY Cam, a slightly asynchronous magnetic accreting white dwarf. The spectra are strongly affected by complex absorption, which we model as a continuous (power law) distribution of covering fraction and column of neutral material. This absorption causes a smooth hardening of the spectrum below 3 keV, and is probably produced by material in the preshock column which overlies the X-ray emission region. The ASCA data show that the intrinsic emission from the shock is not consistent with a single temperature plasma. Significant iron L emission co-existing with iron K shell lines from H and He-like iron clearly shows that there is a wide range of temperatures present, as expected from a cooling shock structure. The GINGA data give the best constraints on the maximum temperature emission in the shocked plasma, with kT(max)=21(+18,-4) keV. Cyclotron cooling should also be important, which supresses the highest temperature bremsstrahlung components, so the X-ray data only give a lower limit on the mass of the white dwarf of M> 0.5 solar masses. Reflection of the multi-temperature bremsstrahlung emission from the white dwarf surface is also significantly detected. We stress the importance of modelling ALL these effects in order to gain a physically self-consistent picture of the X-ray spectra from polars in general and BY Cam in particular., 9 pages, 4 figures, MNRAS, accepted
- Published
- 1997
23. The Ginga Hard X-Ray Spectrum of AM Herculis
- Author
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A. P. Beardmore, C. Done, J. P. Osborne, and M. Ishida
- Published
- 1995
- Full Text
- View/download PDF
24. Pair loading in compact sources
- Author
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C Done, G Ghisellini, and A C Fabian
- Subjects
Space and Planetary Science ,Astrophysics::High Energy Astrophysical Phenomena ,Astronomy and Astrophysics - Abstract
Summary We investigate the effects of a re-acceleration mechanism in compact sources where electron-positron pair production is important. The pairs increase the number of particles to be accelerated and decrease the mean particle energy if the source luminosity remains constant. The acceleration mechanism is loaded. Models in which this effect is included reproduce the γ-ray break seen in active galactic nuclei. It is mainly due to the reduced particle energy and not to photon-photon absorption. The X-ray spectra are generally flatter than those observed if the electrons are accelerated to a single energy. Pair reradiation no longer steepens the spectrum, since loading enhances the importance of the primary emission spectrum. Spectra in agreement with observations can be obtained if the electrons are re-accelerated with a power-law energy distribution. Our investigation highlights the accumulation of cooled particles within the source. It is a severe constraint on continuous injection models. The lack of any obvious spectral break attributable to Compton downscattering in the high-energy spectra of active galactic nuclei conflicts with the predictions of most models. Highly compact sources produce large amounts of pairs and so have a high optical depth of cooled electrons. We consider this ‘dead electron’ problem for a wide range of models. Reacceleration of the electrons, which is often invoked as a means of overcoming the problem, is not an adequate solution in most cases.
- Published
- 1990
- Full Text
- View/download PDF
25. Assessment of barley varieties as potential pollen-parents for F1 — hybrid varieties
- Author
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A. C. Done and R. C. F. Macer
- Subjects
business.industry ,food and beverages ,General Medicine ,Biology ,Plant disease resistance ,Marked effect ,medicine.disease_cause ,Hybrid seed ,Agronomy ,Agriculture ,Pollinator ,Pollen ,Genetics ,medicine ,Cultivar ,Experimental methods ,business ,Agronomy and Crop Science ,Biotechnology - Abstract
The choice of male parents for an F1-hybrid barley variety depends upon a number of characteristics, among which will be the combining ability for yield, the transference of disease resistance and the ability to release large quantities of viable pollen to ensure a high set of F1 -hybrid seed on the male-sterile Une. A number of cultivars were assessed as potential pollen parents using a common male-sterile variety. Various experimental methods to assess the potential of male parents were used at locations in the United Kingdom and elsewhere in Western Europe over a period of three years. Significant differences were demonstrated between the cross-pollinating ability of varieties; ‘good’ pollinators gave consistent results. A marked effect of crossing-block size was found and there was also some evidence of environmental interactions.
- Published
- 1978
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- View/download PDF
26. Eucalyptus ceracea, E. rupestris and E. chlorophylla (Myrtaceae), three new species in the Kimberley Division of Western Australia
- Author
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Chris C Done and Murray Ian Hill Brooker
- Subjects
Plant Science - Published
- 1986
- Full Text
- View/download PDF
27. Some expression of heterosis in F1-hybrid barley
- Author
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R. C. F. Macer and Angela C. Done
- Subjects
Agronomy ,Heterosis ,Biology ,Agronomy and Crop Science ,Hybrid - Abstract
SUMMARY Small and large scale trials of F1 barley hybrids were done in a glasshouse in the United Kingdom and in the field in the United Kingdom and Europe in 1970, 1971 and 1972. The results showed that there were few instances of significant positive heterosis in yield with either the small or field scale experiments. The hybrids studied were all derived from American varieties as male-sterile parents and therefore the hybrids were not adapted to European countries, thus the case for or against F1-hybrids cannot be assessed solely on this material.
- Published
- 1979
- Full Text
- View/download PDF
28. Implications of the introduction of hybrid cereals on disease patterns
- Author
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Angela C. Done
- Subjects
Agronomy ,Evolutionary biology ,Disease patterns ,Biology ,Agronomy and Crop Science - Published
- 1973
- Full Text
- View/download PDF
29. Implementation of an Undergraduate Medical Education Course in Global Health Based on the Consortium of Universities for Global Health Core Competencies: A Pilot Program
- Author
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C. Donelan, M. Wagar, C. Howard, S. Benson, and C. Dahl
- Subjects
Infectious and parasitic diseases ,RC109-216 ,Public aspects of medicine ,RA1-1270 - Published
- 2017
- Full Text
- View/download PDF
30. Pair Production in AGN
- Author
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C. Done and A. C. Fabian
- Subjects
Astrophysics::High Energy Astrophysical Phenomena ,Astrophysics::Cosmology and Extragalactic Astrophysics ,Astrophysics::Galaxy Astrophysics - Abstract
The X-ray luminosity and variability of many AGN are sufficiently extreme that any hard γ-rays produced in the source will collide with the X-rays and create electron-positron pairs, rather than escape. A small region where vast amounts of energy are produced, such as an AGN, is an ideal place to accelerate particles to relativistic energies and so produce γ-rays by Compton scattering. The observed X-ray spectra of AGN are hard and indicate that most of the luminosity is at the highest energies so that absorption of the γ-rays represents a large fraction of the energy flux, which can then be re-radiated at lower energies. Pairs can thus effectively reprocess much of the radiant power in an AGN.
- Published
- 1989
- Full Text
- View/download PDF
31. Space Telescope and Optical Reverberation Mapping Project. VIII. Time Variability of Emission and Absorption in NGC 5548 Based on Modeling the Ultraviolet Spectrum.
- Author
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G. A. Kriss, G. De Rosa, J. Ely, B. M. Peterson, J. Kaastra, M. Mehdipour, G. J. Ferland, M. Dehghanian, S. Mathur, R. Edelson, K. T. Korista, N. Arav, A. J. Barth, M. C. Bentz, W. N. Brandt, D. M. Crenshaw, E. Dalla Bontà, K. D. Denney, C. Done, and M. Eracleous
- Subjects
ULTRAVIOLET spectra ,OPTICAL telescopes ,SPACE telescopes ,ABSORPTION ,SEYFERT galaxies ,SOUND reverberation - Abstract
We model the ultraviolet spectra of the Seyfert 1 galaxy NGC 5548 obtained with the Hubble Space Telescope during the 6 month reverberation mapping campaign in 2014. Our model of the emission from NGC 5548 corrects for overlying absorption and deblends the individual emission lines. Using the modeled spectra, we measure the response to continuum variations for the deblended and absorption-corrected individual broad emission lines, the velocity-dependent profiles of Lyα and C iv, and the narrow and broad intrinsic absorption features. We find that the time lags for the corrected emission lines are comparable to those for the original data. The velocity-binned lag profiles of Lyα and C iv have a double-peaked structure indicative of a truncated Keplerian disk. The narrow absorption lines show a delayed response to continuum variations corresponding to recombination in gas with a density of ∼10
5 cm−3 . The high-ionization narrow absorption lines decorrelate from continuum variations during the same period as the broad emission lines. Analyzing the response of these absorption lines during this period shows that the ionizing flux is diminished in strength relative to the far-ultraviolet continuum. The broad absorption lines associated with the X-ray obscurer decrease in strength during this same time interval. The appearance of X-ray obscuration in ∼2012 corresponds with an increase in the luminosity of NGC 5548 following an extended low state. We suggest that the obscurer is a disk wind triggered by the brightening of NGC 5548 following the decrease in size of the broad-line region during the preceding low-luminosity state. [ABSTRACT FROM AUTHOR]- Published
- 2019
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- View/download PDF
32. Geological Jargonese
- Author
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J. P. C. DONE
- Subjects
Multidisciplinary - Published
- 1928
- Full Text
- View/download PDF
33. Swift Monitoring of NGC 4151: Evidence for a Second X-Ray/UV Reprocessing.
- Author
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R. Edelson, J. Gelbord, E. Cackett, S. Connolly, C. Done, M. Fausnaugh, E. Gardner, N. Gehrels, M. Goad, K. Horne, I. McHardy, B. M. Peterson, S. Vaughan, M. Vestergaard, A. Breeveld, A. J. Barth, M. Bentz, M. Bottorff, W. N. Brandt, and S. M. Crawford
- Subjects
STELLAR corona ,SPIRAL galaxies ,X-rays ,LIGHT curves ,ULTRAVIOLET radiation ,ACCRETION disks - Abstract
Swift monitoring of NGC 4151 with an ∼6 hr sampling over a total of 69 days in early 2016 is used to construct light curves covering five bands in the X-rays (0.3–50 keV) and six in the ultraviolet (UV)/optical (1900–5500 Å). The three hardest X-ray bands (>2.5 keV) are all strongly correlated with no measurable interband lag, while the two softer bands show lower variability and weaker correlations. The UV/optical bands are significantly correlated with the X-rays, lagging ∼3–4 days behind the hard X-rays. The variability within the UV/optical bands is also strongly correlated, with the UV appearing to lead the optical by ∼0.5–1 days. This combination of ≳3 day lags between the X-rays and UV and ≲1 day lags within the UV/optical appears to rule out the “lamp-post” reprocessing model in which a hot, X-ray emitting corona directly illuminates the accretion disk, which then reprocesses the energy in the UV/optical. Instead, these results appear consistent with the Gardner & Done picture in which two separate reprocessings occur: first, emission from the corona illuminates an extreme-UV-emitting toroidal component that shields the disk from the corona; this then heats the extreme-UV component, which illuminates the disk and drives its variability. [ABSTRACT FROM AUTHOR]
- Published
- 2017
- Full Text
- View/download PDF
34. AN OPTICALLY THICK DISK WIND IN GRO J1655–40?
- Author
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M. Shidatsu, C. Done, and Y. Ueda
- Subjects
- *
DATA analysis , *RADIATION pressure , *ELECTROMAGNETIC waves , *VACUUM tubes , *FLUOROSCOPY - Abstract
We revisited the unusual wind in GRO J1655−40, detected with Chandra in 2005 April, using long-term Rossi X-ray Timing Explorer X-ray data and simultaneous optical/near-infrared photometric data. This wind is the most convincing case for magnetic driving in black hole binaries, as it has an inferred launch radius that is a factor of 10 smaller than the thermal wind prediction. However, the optical and near-infrared (OIR) fluxes monotonically increase around the Chandra observation, whereas the X-ray flux monotonically decreases from 10 days beforehand. Yet the optical and near-infrared fluxes are from the outer, irradiated disk, so for them to increase implies that the X-rays likewise increased. We applied a new irradiated disk model to the multi-wavelength spectral energy distributions. Fitting the OIR fluxes, we estimated the intrinsic luminosity at the Chandra epoch was , which is more than one order of magnitude larger than the observed X-ray luminosity. These results could be explained if a Compton-thick, almost completely ionized gas was present in the wind and strong scattering reduced the apparent X-ray luminosity. The effects of scattering in the wind should then be taken into account for discussion of the wind-driving mechanism. Radiation pressure and Compton heating may also contribute to powering the wind at this high luminosity. [ABSTRACT FROM AUTHOR]
- Published
- 2016
- Full Text
- View/download PDF
35. The Large Observatory for X-ray Timing (LOFT)
- Author
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Feroci, M., Stella, L., Klis, M., Courvoisier, T. J. -L, Hernanz, M., Hudec, R., Santangelo, A., Walton, D., Zdziarski, A., Barret, D., Belloni, T., Braga, José, Brandt, S., Budtz-Jørgensen, C., Campana, S., Den Herder, J. -W, Huovelin, J., Israel, G. L., Pohl, M., Ray, P., Vacchi, A., Zane, S., Argan, A., Primo Attinà, Bertuccio, G., Bozzo, E., Campana, R., Chakrabarty, D., Costa, E., Rosa, A., Del Monte, E., Di Cosimo, S., Donnarumma, I., Evangelista, Y., Haas, D., Jonker, P., Korpela, S., Labanti, C., Malcovati, P., Mignani, R., Muleri, F., Rapisarda, M., Rashevsky, A., Rea, N., Rubini, A., Tenzer, C., Wilson-Hodge, C., Winter, B., Wood, K., Zampa, G., Zampa, N., Abramowicz, M. A., Alpar, M. A., Altamirano, D., Alvarez, J. M., Amati, L., Amoros, C., Antonelli, L. A., Artigue, R., Azzarello, P., Bachetti, M., Baldazzi, G., Barbera, M., Barbieri, C., Basa, S., Baykal, A., Belmont, R., Boirin, L., Bonvicini, V., Burderi, L., Bursa, M., Cabanac, C., Cackett, E., Caliandro, G. A., Casella, P., Chaty, S., Chenevez, J., Coe, M. J., Collura, A., Corongiu, A., Covino, S., Cusumano, G., D Amico, Frank, Dall Osso, S., Martino, D., Paris, G., Di Persio, G., Di Salvo, T., Done, C., Dovčiak, M., Drago, A., Ertan, U., Fabiani, S., Falanga, M., Fender, R., Ferrando, P., Della Monica Ferreira, D., Fraser, G., Frontera, F., Fuschino, F., Galvez, J. L., Gandhi, P., Giommi, P., Godet, O., Göǧüş, E., Goldwurm, A., Götz, D., Grassi, M., Guttridge, P., Hakala, P., Henri, G., Hermsen, W., Horak, J., Hornstrup, A., In T Zand, J. J. M., Isern, J., Kalemci, E., Kanbach, G., Karas, V., Kataria, D., Kennedy, T., Klochkov, D., Kluźniak, W., Kokkotas, K., Kreykenbohm, I., Krolik, J., Kuiper, L., Kuvvetli, I., Kylafis, N., Lattimer, J. M., Lazzarotto, F., Leahy, D., Lebrun, F., Lin, D., Lund, N., Maccarone, T., Malzac, J., Marisaldi, M., Martindale, A., Mastropietro, M., Mcclintock, J., Mchardy, I., Mendez, M., Mereghetti, S., Miller, M. C., Mineo, T., Morelli, E., Morsink, S., Motch, C., Motta, S., Muñoz-Darias, T., Naletto, G., Neustroev, V., Nevalainen, J., Olive, J. F., Orio, M., Orlandini, M., Orleanski, P., Ozel, F., Pacciani, L., Paltani, S., Papadakis, I., Papitto, A., Patruno, A., Pellizzoni, A., Petráček, V., Petri, J., Petrucci, P. O., Phlips, B., Picolli, L., Possenti, A., Psaltis, D., Rambaud, D., Reig, P., Remillard, R., Rodriguez, J., Romano, P., Romanova, M., Schanz, T., Schmid, C., Segreto, A., Shearer, A., Smith, A., Smith, P. J., Soffitta, P., Stergioulas, N., Stolarski, M., Stuchlik, Z., Tiengo, A., Torres, D., Török, G., Turolla, R., Uttley, P., Vaughan, S., Vercellone, S., Waters, R., Watts, A., Wawrzaszek, R., Webb, N., Wilms, J., Zampieri, L., Zezas, A., Ziolkowski, J., Institut de Recherches sur les lois Fondamentales de l'Univers (IRFU), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris-Saclay, AstroParticule et Cosmologie (APC (UMR_7164)), Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3), APC - Astrophysique des Hautes Energies (APC - AHE), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Dipartimento di Astronomia, Universita degli Studi di Bologna, Alma Mater Studiorum Università di Bologna [Bologna] (UNIBO)-Alma Mater Studiorum Università di Bologna [Bologna] (UNIBO), Astrophysique Interprétation Modélisation (AIM (UMR_7158 / UMR_E_9005 / UM_112)), Centre National de la Recherche Scientifique (CNRS)-Institut national des sciences de l'Univers (INSU - CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Université Paris Diderot - Paris 7 (UPD7), Astronomy, Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Observatoire de Paris, Université Paris sciences et lettres (PSL)-Université Paris sciences et lettres (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS)-Alma Mater Studiorum Università di Bologna [Bologna] (UNIBO), Astrophysique Interprétation Modélisation (AIM (UMR7158 / UMR_E_9005 / UM_112)), Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Institut national des sciences de l'Univers (INSU - CNRS)-Université Paris Diderot - Paris 7 (UPD7)-Centre National de la Recherche Scientifique (CNRS), M. Feroci, L. Stella, M. v. der, T. Courvoisier, M. Hernanz, R. Hudec, A. Santangelo, D. Walton, A. Zdziarski, D. Barret, T. Belloni, J. Braga, S. Brandt, C. Budtz-Jorgensen, S. Campana, J. d. Herder, J. Huovelin, G. Israel, M. Pohl, P. Ray, A. Vacchi, S. Zane, A. Argan, P. Attina, G. Bertuccio, E. Bozzo, R. Campana, D. Chakrabarty, E. Costa, A. D. Rosa, E. D. Monte, S. D. Cosimo, I. Donnarumma, Y. Evangelista, D. Haa, P. Jonker, S. Korpela, C. Labanti, P. Malcovati, R. Mignani, F. Muleri, M. Rapisarda, A. Rashevsky, N. Rea, A. Rubini, C. Tenzer, C. Wilson-Hodge, B. Winter, K. Wood, G. Zampa, N. Zampa, M. Abramowicz, M. Alpar, D. Altamirano, J. Alvarez, L. Amati, C. Amoro, L. Antonelli, R. Artigue, P. Azzarello, M. Bachetti, G. Baldazzi, M. Barbera, C. Barbieri, S. Basa, A. Baykal, R. Belmont, L. Boirin, V. Bonvicini, L. Burderi, M. Bursa, C. Cabanac, E. Cackett, G. Caliandro, P. Casella, S. Chaty, J. Chenevez, M. Coe, A. Collura, A. Corongiu, S. Covino, G. Cusumano, F. D'Amico, S. Dall'Osso, D. D. Martino, G. D. Pari, G. D. Persio, T. D. Salvo, C. Done, M. Dovciak, A. Drago, U. Ertan, S. Fabiani, M. Falanga, R. Fender, P. Ferrando, D. Ferreira, G. Fraser, F. Frontera, F. Fuschino, J. Galvez, P. Gandhi, P. Giommi, O. Godet, E. Gogu, A. Goldwurm, D. Gotz, M. Grassi, P. Guttridge, P. Hakala, G. Henri, W. Hermsen, J. Horak, A. Hornstrup, J. i. Zand, J. Isern, E. Kalemci, G. Kanbach, V. Kara, D. Kataria, T. Kennedy, D. Klochkov, W. Kluzniak, K. Kokkota, I. Kreykenbohm, J. Krolik, L. Kuiper, I. Kuvvetli, N. Kylafi, J. Lattimer, F. Lazzarotto, D. Leahy, F. Lebrun, D. Lin, N. Lund, T. Maccarone, J. Malzac, M. Marisaldi, A. Martindale, M. Mastropietro, J. McClintock, I. McHardy, M. Mendez, S. Mereghetti, M. Miller, T. Mineo, E. Morelli, S. Morsink, C. Motch, S. Motta, T. Munoz-Daria, G. Naletto, V. Neustroev, J. Nevalainen, J. Olive, M. Orio, M. Orlandini, P. Orleanski, F. Ozel, L. Pacciani, S. Paltani, I. Papadaki, A. Papitto, A. Patruno, A. Pellizzoni, V. Petracek, J. Petri, P. Petrucci, B. Phlip, L. Picolli, A. Possenti, D. Psalti, D. Rambaud, P. Reig, R. Remillard, J. Rodriguez, P. Romano, M. Romanova, T. Schanz, C. Schmid, A. Segreto, A. Shearer, A. Smith, P. Smith, P. Soffitta, N. Stergioula, M. Stolarski, Z. Stuchlik, A. Tiengo, D. Torre, G. Torok, R. Turolla, P. Uttley, S. Vaughan, S. Vercellone, R. Water, A. Watt, R. Wawrzaszek, N. Webb, J. Wilm, L. Zampieri, A. Zeza, J. Ziolkowski, High Energy Astrophys. & Astropart. Phys (API, FNWI), Feroci, M., Stella, L., van der Klis, M., Courvoisier, T. J.-L., Hernanz, M., Hudec, R., Santangelo, A., Walton, D., Zdziarski, A., Barret, D., Belloni, T., Braga, J., Brandt, S., Budtz-Jørgensen, C., Campana, S., den Herder, J.-W., Huovelin, J., Israel, G. L., Pohl, M., Ray, P., Vacchi, A., Zane, S., Argan, A., Attinà, P., Bertuccio, G., Bozzo, E., Campana, R., Chakrabarty, D., Costa, E., De Rosa, A., Del Monte, E., Di Cosimo, S., Donnarumma, I., Evangelista, Y., Haas, D., Jonker, P., Korpela, S., Labanti, C., Malcovati, P., Mignani, R., Muleri, F., Rapisarda, M., Rashevsky, A., Rea, N., Rubini, A., Tenzer, C., Wilson-Hodge, C., Winter, B., Wood, K., Zampa, G., Zampa, N., Abramowicz, M. A., Alpar, M. A., Altamirano, D., Alvarez, J. M., Amati, L., Amoros, C., Antonelli, L. A., Artigue, R., Azzarello, P., Bachetti, M., Baldazzi, G., Barbera, M., Barbieri, C., Basa, S., Baykal, A., Belmont, R., Boirin, L., Bonvicini, V., Burderi, L., Bursa, M., Cabanac, C., Cackett, E., Caliandro, G. A., Casella, P., Chaty, S., Chenevez, J., Coe, M. J., Collura, A., Corongiu, A., Covino, S., Cusumano, G., D'Amico, F., Dall'Osso, S., De Martino, D., De Paris, G., Di Persio, G., Di Salvo, T., Done, C., Dovčiak, M., Drago, A., Ertan, U., Fabiani, S., Falanga, M., Fender, R., Ferrando, P., Della Monica Ferreira, D., Fraser, G., Frontera, F., Fuschino, F., Galvez, J. L., Gandhi, P., Giommi, P., Godet, O., Göǧüş, E., Goldwurm, A., Götz, D., Grassi, M., Guttridge, P., Hakala, P., Henri, G., Hermsen, W., Horak, J., Hornstrup, A., in't Zand, J. J. M., Isern, J., Kalemci, E., Kanbach, G., Karas, V., Kataria, D., Kennedy, T., Klochkov, D., Kluźniak, W., Kokkotas, K., Kreykenbohm, I., Krolik, J., Kuiper, L., Kuvvetli, I., Kylafis, N., Lattimer, J. M., Lazzarotto, F., Leahy, D., Lebrun, F., Lin, D., Lund, N., Maccarone, T., Malzac, J., Marisaldi, M., Martindale, A., Mastropietro, M., McClintock, J., McHardy, I., Mendez, M., Mereghetti, S., Miller, M. C., Mineo, T., Morelli, E., Morsink, S., Motch, C., Motta, S., Muñoz-Darias, T., Naletto, G., Neustroev, V., Nevalainen, J., Olive, J. F., Orio, M., Orlandini, M., Orleanski, P., Ozel, F., Pacciani, L., Paltani, S., Papadakis, I., Papitto, A., Patruno, A., Pellizzoni, A., Petráček, V., Petri, J., Petrucci, P. O., Phlips, B., Picolli, L., Possenti, A., Psaltis, D., Rambaud, D., Reig, P., Remillard, R., Rodriguez, J., Romano, P., Romanova, M., Schanz, T., Schmid, C., Segreto, A., Shearer, A., Smith, A., Smith, P. J., Soffitta, P., Stergioulas, N., Stolarski, M., Stuchlik, Z., Tiengo, A., Torres, D., Török, G., Turolla, R., Uttley, P., Vaughan, S., Vercellone, S., Waters, R., Watts, A., Wawrzaszek, R., Webb, N., Wilms, J., Zampieri, L., Zezas, A., Ziolkowski, J., Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Observatoire de Paris, PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7), PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Institut National de Physique Nucléaire et de Physique des Particules du CNRS (IN2P3)-Centre National de la Recherche Scientifique (CNRS)-Commissariat à l'énergie atomique et aux énergies alternatives (CEA)-Observatoire de Paris, PSL Research University (PSL)-PSL Research University (PSL)-Université Paris Diderot - Paris 7 (UPD7)-Dipartimento di Astronomia, Universita degli Studi di Bologna, and Università di Bologna [Bologna] (UNIBO)-Università di Bologna [Bologna] (UNIBO)
- Subjects
Event horizon ,X-ray timing ,Mission ,7. Clean energy ,01 natural sciences ,neutron stars ,T175 Industrial research. Research and development ,BINARIES ,Settore FIS/05 - Astronomia E Astrofisica ,ALICE ,SILICON DRIFT DETECTOR ,Observatory ,EQUATION ,neutron star ,010303 astronomy & astrophysics ,High Energy Astrophysical Phenomena (astro-ph.HE) ,Physics ,[SDU.ASTR.HE]Sciences of the Universe [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE] ,Astrophysics::Instrumentation and Methods for Astrophysics ,Missions, X-ray timing, compact objects, black holes, neutron stars ,compact objects ,Astrophysics - Instrumentation and Methods for Astrophysics ,Astrophysics - High Energy Astrophysical Phenomena ,PROPORTIONAL COUNTER ,[PHYS.ASTR.HE]Physics [physics]/Astrophysics [astro-ph]/High Energy Astrophysical Phenomena [astro-ph.HE] ,Active galactic nucleus ,Cosmic Vision ,X-ray astronomy ,high time variability ,Astrophysics::High Energy Astrophysical Phenomena ,black holes ,Missions ,FOS: Physical sciences ,0103 physical sciences ,OSCILLATIONS ,Instrumentation and Methods for Astrophysics (astro-ph.IM) ,Supermassive black hole ,010308 nuclear & particles physics ,Astronomy ,CONSTRAINTS ,Astronomy and Astrophysics ,Galaxy ,Black hole ,Neutron star ,Space and Planetary Science ,QB460-466 Astrophysics ,DISCOVERY ,BLACK-HOLE ,SUPERAGILE - Abstract
High-time-resolution X-ray observations of compact objects provide direct access to strong-field gravity, to the equation of state of ultra-dense matter and to black hole masses and spins. A 10 m^2-class instrument in combination with good spectral resolution is required to exploit the relevant diagnostics and answer two of the fundamental questions of the European Space Agency (ESA) Cosmic Vision Theme "Matter under extreme conditions", namely: does matter orbiting close to the event horizon follow the predictions of general relativity? What is the equation of state of matter in neutron stars? The Large Observatory For X-ray Timing (LOFT), selected by ESA as one of the four Cosmic Vision M3 candidate missions to undergo an assessment phase, will revolutionise the study of collapsed objects in our galaxy and of the brightest supermassive black holes in active galactic nuclei. Thanks to an innovative design and the development of large-area monolithic Silicon Drift Detectors, the Large Area Detector (LAD) on board LOFT will achieve an effective area of ~12 m^2 (more than an order of magnitude larger than any spaceborne predecessor) in the 2-30 keV range (up to 50 keV in expanded mode), yet still fits a conventional platform and small/medium-class launcher. With this large area and a spectral resolution of, 29 pages, 10 figures. Accepted for publication in Experimental Astronomy
- Published
- 2012
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36. Localized thermonuclear bursts from accreting magnetic white dwarfs.
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Scaringi S, Groot PJ, Knigge C, Bird AJ, Breedt E, Buckley DAH, Cavecchi Y, Degenaar ND, de Martino D, Done C, Fratta M, Iłkiewicz K, Koerding E, Lasota JP, Littlefield C, Manara CF, O'Brien M, Szkody P, and Timmes FX
- Abstract
Nova explosions are caused by global thermonuclear runaways triggered in the surface layers of accreting white dwarfs
1-3 . It has been predicted4-6 that localized thermonuclear bursts on white dwarfs can also take place, similar to type-I X-ray bursts observed in accreting neutron stars. Unexplained rapid bursts from the binary system TV Columbae, in which mass is accreted onto a moderately strong magnetized white dwarf from a low-mass companion, have been observed on several occasions in the past 40 years7-11 . During these bursts, the optical/ultraviolet luminosity increases by a factor of more than three in less than an hour and fades in around ten hours. Fast outflows have been observed in ultraviolet spectral lines7 , with velocities of more than 3,500 kilometres per second, comparable to the escape velocity from the white dwarf surface. Here we report on optical bursts observed in TV Columbae and in two additional accreting systems, EI Ursae Majoris and ASASSN-19bh. The bursts have a total energy of approximately 10-6 times than those of classical nova explosions (micronovae) and bear a strong resemblance to type-I X-ray bursts12-14 . We exclude accretion or stellar magnetic reconnection events as their origin and suggest thermonuclear runaway events in magnetically confined accretion columns as a viable explanation., (© 2022. The Author(s), under exclusive licence to Springer Nature Limited.)- Published
- 2022
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37. Hitomi X-ray studies of Giant Radio Pulses from the Crab pulsar.
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Aharonian F, Akamatsu H, Akimoto F, Allen SW, Angelini L, Audard M, Awaki H, Axelsson M, Bamba A, Bautz MW, Blandford R, Brenneman LW, Brown GV, Bulbul E, Cackett EM, Chernyakova M, Chiao MP, Coppi PS, Costantini E, De Plaa J, De Vries CP, Den Herder JW, Done C, Dotani T, Ebisawa K, Eckart ME, Enoto T, Ezoe Y, Fabian AC, Ferrigno C, Foster AR, Fujimoto R, Fukazawa Y, Furuzawa A, Galeazzi M, Gallo LC, Gandhi P, Giustini M, Goldwurm A, Gu L, Guainazzi M, Haba Y, Hagino K, Hamaguchi K, Harrus IM, Hatsukade I, Hayashi K, Hayashi T, Hayashida K, Hiraga JS, Hornschemeier A, Hoshino A, Hughes JP, Ichinohe Y, Iizuka R, Inoue H, Inoue Y, Ishida M, Ishikawa K, Ishisaki Y, Iwai M, Kaastra J, Kallman T, Kamae T, Kataoka J, Katsuda S, Kawai N, Kelley RL, Kilbourne CA, Kitaguchi T, Kitamoto S, Kitayama T, Kohmura T, Kokubun M, Koyama K, Koyama S, Kretschmar P, Krimm HA, Kubota A, Kunieda H, Laurent P, Lee SH, Leutenegger MA, Limousin OO, Loewenstein M, Long KS, Lumb D, Madejski G, Maeda Y, Maier D, Makishima K, Markevitch M, Matsumoto H, Matsushita K, Mccammon D, Mcnamara BR, Mehdipour M, Miller ED, Miller JM, Mineshige S, Mitsuda K, Mitsuishi I, Miyazawa T, Mizuno T, Mori H, Mori K, Mukai K, Murakami H, Mushotzky RF, Nakagawa T, Nakajima H, Nakamori T, Nakashima S, Nakazawa K, Nobukawa KK, Nobukawa M, Noda H, Odaka H, Ohashi T, Ohno M, Okajima T, Oshimizu K, Ota N, Ozaki M, Paerels F, Paltani S, Petre R, Pinto C, Porter FS, Pottschmidt K, Reynolds CS, Safi-Harb S, Saito S, Sakai K, Sasaki T, Sato G, Sato K, Sato R, Sawada M, Schartel N, Serlemtsos PJ, Seta H, Shidatsu M, Simionescu A, Smith RK, Soong Y, Stawarz Ł, Sugawara Y, Sugita S, Szymkowiak A, Tajima H, Takahashi H, Takahashi T, Takeda S, Takei Y, Tamagawa T, Tamura T, Tanaka T, Tanaka Y, Tanaka YT, Tashiro MS, Tawara Y, Terada Y, Terashima Y, Tombesi F, Tomida H, Tsuboi Y, Tsujimoto M, Tsunemi H, Tsuru TG, Uchida H, Uchiyama H, Uchiyama Y, Ueda S, Ueda Y, Uno S, Urry CM, Ursino E, Watanabe S, Werner N, Wilkins DR, Williams BJ, Yamada S, Yamaguchi H, Yamaoka K, Yamasaki NY, Yamauchi M, Yamauchi S, Yaqoob T, Yatsu Y, Yonetoku D, Zhuravleva I, Zoghbi A, Terasawa T, Sekido M, Takefuji K, Kawai E, Misawa H, Tsuchiya F, Yamazaki R, Kobayashi E, Kisaka S, and Aoki T
- Abstract
To search for giant X-ray pulses correlated with the giant radio pulses (GRPs) from the Crab pulsar, we performed a simultaneous observation of the Crab pulsar with the X-ray satellite Hitomi in the 2 - 300 keV band and the Kashima NICT radio observatory in the 1.4 - 1.7 GHz band with a net exposure of about 2 ks on 25 March 2016, just before the loss of the Hitomi mission. The timing performance of the Hitomi instruments was confirmed to meet the timing requirement and about 1,000 and 100 GRPs were simultaneously observed at the main and inter-pulse phases, respectively, and we found no apparent correlation between the giant radio pulses and the X-ray emission in either the main or inter-pulse phases. All variations are within the 2 sigma fluctuations of the X-ray fluxes at the pulse peaks, and the 3 sigma upper limits of variations of main- or inter-pulse GRPs are 22% or 80% of the peak flux in a 0.20 phase width, respectively, in the 2 - 300 keV band. The values become 25% or 110% for main or inter-pulse GRPs, respectively, when the phase width is restricted into the 0.03 phase. Among the upper limits from the Hitomi satellite, those in the 4.5-10 keV and the 70-300 keV are obtained for the first time, and those in other bands are consistent with previous reports. Numerically, the upper limits of main- and inter-pulse GRPs in the 0.20 phase width are about (2.4 and 9.3) ×10
-11 erg cm-2 , respectively. No significant variability in pulse profiles implies that the GRPs originated from a local place within the magnetosphere and the number of photon-emitting particles temporally increases. However, the results do not statistically rule out variations correlated with the GRPs, because the possible X-ray enhancement may appear due to a > 0.02% brightening of the pulse-peak flux under such conditions.- Published
- 2018
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38. Bright radio emission from an ultraluminous stellar-mass microquasar in M 31.
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Middleton MJ, Miller-Jones JC, Markoff S, Fender R, Henze M, Hurley-Walker N, Scaife AM, Roberts TP, Walton D, Carpenter J, Macquart JP, Bower GC, Gurwell M, Pietsch W, Haberl F, Harris J, Daniel M, Miah J, Done C, Morgan JS, Dickinson H, Charles P, Burwitz V, Della Valle M, Freyberg M, Greiner J, Hernanz M, Hartmann DH, Hatzidimitriou D, Riffeser A, Sala G, Seitz S, Reig P, Rau A, Orio M, Titterington D, and Grainge K
- Abstract
A subset of ultraluminous X-ray sources (those with luminosities of less than 10(40) erg s(-1); ref. 1) are thought to be powered by the accretion of gas onto black holes with masses of ∼5-20M cicled dot, probably by means of an accretion disk. The X-ray and radio emission are coupled in such Galactic sources; the radio emission originates in a relativistic jet thought to be launched from the innermost regions near the black hole, with the most powerful emission occurring when the rate of infalling matter approaches a theoretical maximum (the Eddington limit). Only four such maximal sources are known in the Milky Way, and the absorption of soft X-rays in the interstellar medium hinders the determination of the causal sequence of events that leads to the ejection of the jet. Here we report radio and X-ray observations of a bright new X-ray source in the nearby galaxy M 31, whose peak luminosity exceeded 10(39) erg s(-1). The radio luminosity is extremely high and shows variability on a timescale of tens of minutes, arguing that the source is highly compact and powered by accretion close to the Eddington limit onto a black hole of stellar mass. Continued radio and X-ray monitoring of such sources should reveal the causal relationship between the accretion flow and the powerful jet emission.
- Published
- 2013
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39. A periodicity of approximately 1 hour in X-ray emission from the active galaxy RE J1034+396.
- Author
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Gierliński M, Middleton M, Ward M, and Done C
- Abstract
Active galactic nuclei and quasars are thought to be scaled-up versions of Galactic black hole binaries, powered by accretion onto supermassive black holes with masses of 10(6)-10(9) M[symbol: see text], as opposed to the approximately 10 M [symbol: see text] in binaries (here M [symbol: see text] is the solar mass). One example of the similarities between these two types of systems is the characteristic rapid X-ray variability seen from the accretion flow. The power spectrum of this variability in black hole binaries consists of a broad noise with multiple quasi-periodic oscillations superimposed on it. Although the broad noise component has been observed in many active galactic nuclei, there have hitherto been no significant detections of quasi-periodic oscillations. Here we report the discovery of an approximately 1-hour X-ray periodicity in a bright active galaxy, RE J1034+396. The signal is highly statistically significant (at the 5.6 sigma level) and very coherent, with quality factor Q > 16. The X-ray modulation arises from the direct vicinity of the black hole.
- Published
- 2008
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40. Accretion flows in X-ray binaries.
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Done C
- Abstract
I review the X-ray observations of galactic accreting black holes and neutron stars and interpretations of these in terms of solutions of the accretion flow equations.
- Published
- 2002
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41. Structure of the Circumnuclear Region of Seyfert 2 Galaxies Revealed by Rossi X-Ray Timing Explorer Hard X-Ray Observations of NGC 4945.
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Madejski G, Zycki P, Done C, Valinia A, Blanco P, Rothschild R, and Turek B
- Abstract
NGC 4945 is one of the brightest Seyfert galaxies on the sky at 100 keV, but is completely absorbed below 10 keV; its absorption column is probably the largest that still allows a direct view of the nucleus at hard X-ray energies. Our observations of it with the Rossi X-Ray Timing Explorer (RXTE) satellite confirm the large absorption, which for a simple phenomenological fit using an absorber with solar abundances implies a column of 4.5+0.4-0.4x1024 cm(-2). Using a more realistic scenario (requiring Monte Carlo modeling of the scattering), we infer the optical depth to Thomson scattering of approximately 2.4. If such a scattering medium were to subtend a large solid angle from the nucleus, it should smear out any intrinsic hard X-ray variability on timescales shorter than the light-travel time through it. The rapid (with a timescale of approximately 1 day) hard X-ray variability of NGC 4945 discovered by us with RXTE implies that the bulk of the extreme absorption in this object does not originate in a parsec-size, geometrically thick molecular torus. Instead, the optically thick material on parsec scales must be rather geometrically thin, subtending a half-angle less than 10 degrees, and it is likely to be the same disk of material that is responsible for the water maser emission observed in NGC 4945. Local number counts of Seyfert 1 and Seyfert 2 galaxies show a large population of heavily obscured active galactic nuclei (AGNs) which are proposed to make up the cosmic X-ray background (CXRB). However, for this to be the case, the absorption geometry in the context of axially symmetric unification schemes must have the obscuring material subtending a large scale height-contrary to our inferences about NGC 4945-implying that NGC 4945 is not a prototype of obscured AGNs postulated to make up the CXRB. The small solid angle of the absorber, together with the black hole mass (of approximately 1.4x106 M( middle dot in circle)) from megamaser measurements, allows a robust determination of the nuclear luminosity, which in turn implies that the source radiates at approximately 10% of the Eddington limit.
- Published
- 2000
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42. In vivo monoamine release during naloxone-precipitated morphine withdrawal.
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Silverstone PH, Done C, and Sharp T
- Subjects
- Animals, Dialysis, Hippocampus metabolism, Male, Nucleus Accumbens metabolism, Rats, Rats, Sprague-Dawley, Dopamine metabolism, Morphine adverse effects, Naloxone pharmacology, Norepinephrine metabolism, Serotonin metabolism, Substance Withdrawal Syndrome metabolism
- Abstract
There is much evidence from animal work suggesting that the release of noradrenaline (NA) in the brain increases during naloxone-precipitated morphine withdrawal, but the evidence in favour of changes in release of 5-hydroxytryptamine (5-HT) and dopamine (DA) is contradictory. Here we demonstrate, using in vivo microdialysis, that whilst there is a considerable increase (300%) in release of NA in hippocampus precipitated by naloxone in morphine-dependent rats, there is no change in the release of either 5-HT (in hippocampus) or DA (in nucleus accumbens). These results are consistent with suggestions that the symptoms of morphine withdrawal in rats are due primarily to an increase in central NA release.
- Published
- 1993
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43. Effect of naloxone-precipitated morphine withdrawal on noradrenaline release in rat hippocampus in vivo.
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Done C, Silverstone P, and Sharp T
- Subjects
- Animals, Chromatography, High Pressure Liquid, Clonidine pharmacology, Dialysis, Electrochemistry, Hippocampus drug effects, Locus Coeruleus drug effects, Male, Rats, Rats, Sprague-Dawley, Substance-Related Disorders metabolism, Hippocampus metabolism, Morphine pharmacology, Naloxone pharmacology, Norepinephrine metabolism, Substance Withdrawal Syndrome metabolism
- Abstract
Here we investigated the effect of naloxone-precipitated morphine withdrawal on the release of noradrenaline in hippocampus of the anaesthetised rat. Naloxone (1 mg/kg i.p.) injected 3 and 24 h, but not 3 weeks, after eight daily injections of morphine, induced an immediate increase in hippocampal noradrenaline release. This striking effect of naloxone was markedly attenuated by pretreatment with clonidine (0.1 mg/kg s.c.). These findings provide direct evidence for a marked release of noradrenaline in hippocampus during opiate withdrawal in vivo.
- Published
- 1992
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44. Clonidine but not nifedipine prevents the release of noradrenaline during naloxone-precipitated opiate withdrawal: an in vivo microdialysis study in the rat.
- Author
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Silverstone PH, Done C, and Sharp T
- Subjects
- Animals, Behavior, Animal drug effects, Male, Microdialysis, Morphine Dependence psychology, Rats, Rats, Sprague-Dawley, Substance Withdrawal Syndrome metabolism, Substance Withdrawal Syndrome psychology, Weight Loss drug effects, Clonidine therapeutic use, Naloxone pharmacology, Nifedipine therapeutic use, Norepinephrine metabolism, Substance Withdrawal Syndrome drug therapy
- Abstract
In this study we have examined whether the alpha 2-adrenoceptor agonist clonidine and the calcium channel antagonist nifedipine firstly inhibit the naloxone-precipitated withdrawal syndrome in morphine-dependent rats and secondly reduce central noradrenaline release during withdrawal. We demonstrate that both clonidine (0.1 mg/kg) and nifedipine (10 mg/kg) attenuate the naloxone-precipitated withdrawal syndrome. Using in vivo microdialysis, we demonstrate that following naloxone the release of noradrenaline, as measured by perfusates from hippocampus, increases 300% in morphine-dependent rats. However, whilst pretreatment with clonidine inhibited this increased noradrenaline release, nifedipine did not. These findings suggest that whilst the action of clonidine in attenuating the morphine withdrawal syndrome may be mediated by decreasing central noradrenaline release, this is not the mechanism by which nifedipine acts.
- Published
- 1992
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45. High-energy neutrinos from active galactic nuclei.
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Stecker FW, Done C, Salamon MH, and Sommers P
- Published
- 1991
- Full Text
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