J. Brunaud
University of Paris
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Solar Physics | 1995
J.-P. Delaboudiniere; G. E. Artzner; J. Brunaud; A. H. Gabriel; Jean-François Hochedez; F. Millier; Xueyan Song; B. Au; K. P. Dere; Russell A. Howard; R. W. Kreplin; D. J. Michels; John Daniel Moses; Jean-Marc Defise; Claude Jamar; Pierre Rochus; J. P. Chauvineau; J. P. Marioge; R. C. Catura; James R. Lemen; L. Shing; R. A. Stern; Joseph B. Gurman; W. M. Neupert; Andre J. Maucherat; F. Clette; P. Cugnon; E. L. Van Dessel
The Extreme-ultraviolet Imaging Telescope (EIT) will provide wide-field images of the corona and transition region on the solar disc and up to 1.5 R⊙ above the solar limb. Its normal incidence multilayer-coated optics will select spectral emission lines from Fe IX (171 Å), Fe XII (195 Å), Fe XV (284 Å), and He II (304 Å) to provide sensitive temperature diagnostics in the range from 6 × 104 K to 3 × 106 K. The telescope has a 45 x 45 arcmin field of view and 2.6 arcsec pixels which will provide approximately 5-arcsec spatial resolution. The EIT will probe the coronal plasma on a global scale, as well as the underlying cooler and turbulent atmosphere, providing the basis for comparative analyses with observations from both the ground and other SOHO instruments. This paper presents details of the EIT instrumentation, its performance and operating modes.
Solar Physics | 1997
D. Moses; Frederic Clette; J.-P. Delaboudiniere; G. E. Artzner; M. Bougnet; J. Brunaud; Charles Carabetian; A. H. Gabriel; Jean-François Hochedez; F. Millier; X. Y. Song; B. Au; K. P. Dere; Russell A. Howard; R. Kreplin; D. J. Michels; Jean-Marc Defise; J. P. Chauvineau; J. P. Marioge; R. C. Catura; J. R. Lemen; L. Shing; R. A. Stern; J. B. Gurman; W. M. Neupert; J. Newmark; B. J. Thompson; Andre J. Maucherat; Fabrice Portier-Fozzani; David Berghmans
The Extreme Ultraviolet Imaging Telescope (EIT) on board the SOHO spacecraft has been operational since 2 January 1996. EIT observes the Sun over a 45 x 45 arc min field of view in four emission line groups: Feix, x, Fexii, Fexv, and Heii. A post-launch determination of the instrument flatfield, the instrument scattering function, and the instrument aging were necessary for the reduction and analysis of the data. The observed structures and their evolution in each of the four EUV bandpasses are characteristic of the peak emission temperature of the line(s) chosen for that bandpass. Reports on the initial results of a variety of analysis projects demonstrate the range of investigations now underway: EIT provides new observations of the corona in the temperature range of 1 to 2 MK. Temperature studies of the large-scale coronal features extend previous coronagraph work with low-noise temperature maps. Temperatures of radial, extended, plume-like structures in both the polar coronal hole and in a low latitude decaying active region were found to be cooler than the surrounding material. Active region loops were investigated in detail and found to be isothermal for the low loops but hottest at the loop tops for the large loops.Variability of solar EUV structures, as observed in the EIT time sequences, is pervasive and leads to a re-evaluation of the meaning of the term ‘quiet Sun’. Intensity fluctuations in a high cadence sequence of coronal and chromospheric images correspond to a Kolmogorov turbulence spectrum. This can be interpreted in terms of a mixed stochastic or periodic driving of the transition region and the base of the corona. No signature of the photospheric and chromospheric waves is found in spatially averaged power spectra, indicating that these waves do not propagate to the upper atmosphere or are channeled through narrow local magnetic structures covering a small fraction of the solar surface. Polar coronal hole observing campaigns have identified an outflow process with the discovery of transient Fexii jets. Coronal mass ejection observing campaigns have identified the beginning of a CME in an Fexii sequence with a near simultaneous filament eruption (seen in absorption), formation of a coronal void and the initiation of a bright outward-moving shell as well as the coronal manifestation of a ‘Moreton wave’.
Advances in Space Research | 1997
J.-P. Delaboudiniere; R. A. Stern; Andre J. Maucherat; Fabrice Portier-Fozzani; W. M. Neupert; J. B. Gurman; R. C. Catura; James R. Lemen; L. Shing; G. E. Artzner; J. Brunaud; A. H. Gabriel; D. J. Michels; John Daniel Moses; B. Au; K. P. Dere; Russell A. Howard; R. W. Kreplin; Jean-Marc Defise; Claude Jamar; Pierre Rochus; J. P. Chauvineau; J. P. Marioge; F. Clette; P. Cugnon; E. L. Van Dessel
Abstract The SOHO (SOlar and Heliospheric Observatory) satellite was launched on December 2nd 1995. After arriving at the Earth-Sun (L1) Lagrangian point on February 14th 1996, it began to continuously observe the Sun. As one of the instruments onboard SOHO, the EIT (Extreme ultraviolet Imaging Telescope) images the Suns corona in 4 EUV wavelengths. The He II filter at 304 A images the chromosphere and the base of the transition region at a temperature of 5 − 8 × 104 K; the Fe IX–X filter at 171 A images the corona at a temperature of ∼ 1.3 × 106 K; the Fe XII filter at 195 A images the quiet corona outside coronal holes at a temperature of ∼ 1.6 × 106 K; and the Fe XV filter at 284 A images active regions with a temperature of ∼ 2.0 × 106 K. About 5000 images have been obtained up to the present. In this paper, we describe also some aspects of the telescope and the detector performance for application in the observations. Images and movies of all the wavelengths allow a look at different phenomena present in the Suns corona, and in particular, magnetic field reconnection.
SPIE's 1995 International Symposium on Optical Science, Engineering, and Instrumentation | 1995
Jean-Marc Defise; Xueyan Song; J.-P. Delaboudiniere; G. E. Artzner; Charles Carabetian; Jean-François Hochedez; J. Brunaud; J. Daniel Moses; R. C. Catura; F. Clette; Andre J. Maucherat
Optical characteristics in the wavelength range 15 - 75 nm of the EUV imaging telescope to be launched soon on the SOHO mission are discussed. Bandpasses and photometric sensitivity of the multilayered optics telescope have been measured by a dedicated synchrotron light source at Orsay, France.
Proceedings of SPIE, the International Society for Optical Engineering | 2000
J. Newmark; J. Daniel Moses; J. W. Cook; Jean-Pierre Delaboudiniere; Xueyan Song; Charles Carabetian; Marie Bougnet; J. Brunaud; Jean-Marc Defise; Frederic Clette; Jean-François Hochedez
The ability to derive physical parameters of the Sun from observations by the Solar and Heliospheric Observatory (SOHO) Extreme Ultraviolet Imaging Telescope (EIT) greatly increases the scientific return of the mission. The absolute and time variable calibration of EIT therefore is of extreme interest. The NRL EIT Calibration Sounding Rocket (CalRoc) program was initiated to provide well calibrated, contemporaneous observations in support of SOHO EIT. These observations provide three benefits to the SOHO EIT data, absolute calibration points, temporal and spatial information of the EIT EUV response variability in flight via flat field information and clues to the physics of the degradation. Details of the bandpasses of the multilayered optics and the total telescope photometry are presented. Comparisons are shown with the contemporaneous images from SOHO EIT. Plans for the second CalRoc flight are discussed. Loss of reflectivity in the multilayer mirrors has been identified as a new component to the SOHO EIT and CalRoc degradation.
Astronomical Telescopes and Instrumentation | 2000
M. Ollivier; J.-M. Mariotti; Predrag Sekulic; Guy Michel; A. Léger; Patrick Bouchareine; J. Brunaud; Vincent Coude du Foresto; Bertrand Mennesson; P. Bordé; Anne Amy-Klein; A. Vanlerberghe; Pierre-Olivier Lagage; G. E. Artzner; Fabien Malbet
Present projects of space interferometers dedicated to the detection and analysis of extrasolar planets (DARWIN in Europe, TPF in the United States) are based on the nulling interferometry concept. This concept has been proposed by Bracewell in 1978 but has never been demonstrated with high values of rejection, in the thermal infrared range, where the planet detection should be performed (6 - 18 micrometers ). We have thus built a two-beam laboratory interferometer to validate this concept in a monochromatic case (at 10 micrometers ). The keypoint of our interferometer is the use of optical filtering by pinhole and optical fibers to clean the interfering beams. We present in this paper the principle of the experimental setup, its realization, and the first measurements of rejection it allowed. We also present the future developments of this interferometer.
Solar Physics | 1997
K. P. Dere; Guenter E. Brueckner; Russell A. Howard; M. J. Koomen; C. M. Korendyke; R. W. Kreplin; D. J. Michels; John Daniel Moses; Norman Edward Moulton; Dennis G. Socker; O. C. St. Cyr; J.-P. Delaboudiniere; G. E. Artzner; J. Brunaud; A. H. Gabriel; J.-F. Hochedez; F. Millier; Xueyan Song; J. P. Chauvineau; J. P. Marioge; Jean-Marc Defise; Claude Jamar; Pierre Rochus; R. C. Catura; J. R. Lemen; J. B. Gurman; W. M. Neupert; F. Clette; P. Cugnon; E. L. Van Dessel
Solar Physics | 2000
K. P. Dere; John Daniel Moses; J.-P. Delaboudiniere; J. Brunaud; Charles Carabetian; Jean-François Hochedez; Xueyan Song; R. C. Catura; F. Clette; Jean-Marc Defise
Comptes Rendus De L Academie Des Sciences Serie Iv Physique Astrophysique | 2001
M. Ollivier; J.-M. Mariotti; A. Léger; Predrag Sekulic; J. Brunaud; Guy Michel
International Conference on Space Optics — ICSO 1997 | 2018
M. Ollivier; J.-M. Mariotti; J. Brunaud; Guy Michel; Patrick Bouchareine; A. Léger; G. E. Artzner; Fabien Malbet; P. Puget; Vincent Coude du Foresto; Bertrand Mennesson