Therese Ann Kucera
Goddard Space Flight Center
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Featured researches published by Therese Ann Kucera.
Frontiers in Astronomy and Space Sciences | 2016
Sarah E. Gibson; Therese Ann Kucera; Stephen M. White; James B. Dove; Yuhong Fan; Blake Forland; Laurel A. Rachmeler; Cooper Downs; Katharine K. Reeves
Determining the 3D coronal magnetic field is a critical, but extremely difficult problem to solve. Since different types of multiwavelength coronal data probe different aspects of the coronal magnetic field, ideally these data should be used together to validate and constrain specifications of that field. Such a task requires the ability to create observable quantities at a range of wavelengths from a distribution of magnetic field and associated plasma -- i.e., to perform forward calculations. In this paper we describe the capabilities of the FORWARD SolarSoft IDL package, a uniquely comprehensive toolset for coronal magnetometry. FORWARD is a community resource that may be used both to synthesize a broad range of coronal observables, and to access and compare synthetic observables to existing data. It enables forward fitting of specific observations, and helps to build intuition into how the physical properties of coronal magnetic structures translate to observable properties. FORWARD can also be used to generate synthetic test beds from MHD simulations in order to facilitate the development of coronal magnetometric inversion methods, and to prepare for the analysis of future large solar telescope data.
Solar Physics | 1997
J. E. Wiik; B. Schmieder; Therese Ann Kucera; A. I. Poland; P. Brekke; G. M. Simnett
Observations of an eruptive prominence were obtained on 1 May 1996, with the SUMER and CDS instruments aboard SOHO during the preparatory phase of the Joint Observing Programme JOP12. A coronal mass ejection observed with LASCO is associated temporally and spatially with this prominence. The main objective of JOP12 is to study the dynamics of prominences and the prominence–corona interface. By analysing the spectra of Oiv and Siiv lines observed with SUMER and the spectra of 15 lines with CDS, Doppler shifts, temperatures and electron densities (ratio of Oiv 1401 to 1399Å) were derived in different structures of the prominence. The eruptive part of the prominence consists of a bubble (plasmoid) of material already at transition region temperatures with red shifts up to 100 km s-1 and an electron density of the order of 1010cm-3. The whole prominence was very active. It developed both a large helical loop and several smaller loops consisting of twisted threads or multiple ropes. These may be studied in the SUMER movie (movie 2). The profiles of the SUMER lines show a large dispersion of velocities (±50 km s-1) and the ratio of the Oiv lines indicates a large dispersion in electron density (3 x 109cm-3 to 3x 1011cm-3). The CME observed by LASCO left the corona some tens of minutes before the prominence erupted. This is evidence that the prominence eruptions are probably the result of the removal of the restraining coronal magnetic fields which are in part responsible for the original stability of the prominence.
The Astrophysical Journal | 2015
Leon Ofman; Kalman Knizhnik; Therese Ann Kucera; Brigitte Schmieder
We study nonlinear waves in a prominence foot using 2.5D MHD model motivated by recent high-resolution observations with Hinode/SOT in Ca~II emission of a prominence on October 10, 2012 showing highly dynamic small-scale motions in the prominence material. Observations of H
Advances in Space Research | 2000
G. Aulanier; B. Schmieder; L. van Driel-Gesztelyi; Therese Ann Kucera; P. Démoulin; C. Fang; N. Mein; J.-C. Vial; Pierre Mein; Yu-hua Tang; C DeForest
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Advances in Space Research | 1999
K. Wilhelm; P. Lemaire; I. E. Dammasch; J. Hollandt; U. Schühle; W. Curdt; Therese Ann Kucera; D. M. Hassler; Martin C. E. Huber
intensities and of Doppler shifts show similar propagating fluctuations. However the optically thick nature of the emission lines inhibits unique quantitative interpretation in terms of density. Nevertheless, we find evidence of nonlinear wave activity in the prominence foot by examining the relative magnitude of the fluctuation intensity (
In: Webb, D and Rust, D and Schmieder, B, (eds.) (Proceedings) IAU Colloquium 167 on New Perspectives on Solar Prominences. (pp. pp. 366-369). ASTRONOMICAL SOC PACIFIC (1998) | 1998
L van Driel-Gesztelyi; B. Schmieder; G. Aulanier; P. Démoulin; Pch Martens; D Zarro; C DeForest; B. J. Thompson; Cs Cyr; Therese Ann Kucera; Jt Burkepile; Or White; Y Hanaoka; Nariaki V. Nitta
\delta I/I\sim \delta n/n
Astrophysical Journal Supplement Series | 2018
M. Luna; Judith T. Karpen; J. L. Ballester; Karin Muglach; J. Terradas; Therese Ann Kucera; Holly Gilbert
). The waves are evident as significant density fluctuations that vary with height, and apparently travel upward from the chromosphere into the prominence material with quasi-periodic fluctuations with typical period in the range of 5-11 minutes, and wavelengths
arXiv: Solar and Stellar Astrophysics | 2013
Kalman Knizhnik; Manuel Luna; Karin Muglach; Holly Gilbert; Therese Ann Kucera; Judith T. Karpen
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Physics and Chemistry of The Earth Part C-solar-terrestial and Planetary Science | 2000
K. Wilhelm; P. Lemaire; I. E. Dammasch; J. Hollandt; U. Schühle; W. Curdt; Therese Ann Kucera; D. M. Hassler; M. C. E. Huber
2000 km. Recent Doppler shift observations show the transverse displacement of the propagating waves. The magnetic field was measured with THEMIS instrument and was found to be 5-14 G. For the typical prominence density the corresponding fast magnetosonic speed is
Space Science Reviews | 2008
M. L. Kaiser; Therese Ann Kucera; Joseph M. Davila; O. C. St. Cyr; Madhulika Guhathakurta; E. Christian
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