Heliophysics Events Knowledgebase Coverage Registry (HCR)
Observation Details
Overview Where Groups: Mode, FOV, # spectra in map Data Links
2012-03-20 11:01:05-11:56:23
HOP 207 Support
Study of the Rela7onship between a CME and a Coronal (EIT) Wave
x,y:783",44"
Max FOV:277"x162"
Target:Quiet Sun
Nearby Events
6302A Continuum Intensity277"x162"873 spectra
6302A Longitudinal Flux Density277"x162"873 spectra
6302A Transverse Flux Density277"x162"873 spectra
6302A Velocity 6301.5A277"x162"873 spectra

Level 1 Summary
Level 2 Summary
Level 1 Monthly
Level 2 Monthly
SP Cubes 14 MB
SOTSP: HOP 207 Support
2012-03-20T11:01:05 to 2012-03-20T11:56:23
Science Goal: Study of the Rela7onship between a CME and a Coronal (EIT) Wave
Program: Fast map, 280"x164", Q65, 1-side CCD
Target: Quiet Sun
xcen=783 ycen=44
Instrument: SOTSP
HOP/JOP: 207
Description: Although observation of "EIT" waves, so called following their discovery with SOHO/EIT by Thompson et aI., 1998, has been continuing for more than a decade, many issues still remain to be clarified - see Gallagher and Long, 2011 for a recent comprehensive review. The power of high resolution EUV spectroscopic observation with EIS for studies of wave phenomena has recently been demonstrated by the first detection of a coronal Moreton wave associated with an EIT wave (Harra et aI., 2011). The observation to be undertaken in the present study would seek to determine the density change (if any) produced by the passage of an EIT wave following a CME. Although these waves have been observed in multiple passbands using imagers, any intensity increase could be produced by density or temperature increases or a combination of both. Using several different density diagnostics from EIS across a range of temperatures should allow this issue to be resolved. In addition by examining SWAP and AlA data, it will be possible to determine if the EIT wave forms the flank ofthe CME or is a separate feature. Harra, L. K. et aI., 2011, Ap.J.L., 773:L4, 1. Gallagher, P.T., Long, D.M., 2011, Space Sci. Rev., 158, 365. Thompson, B. J. et aI., 1998, Geophys. Res. Lett., 25, 2465. Target and Observation Plan The observation would be on a ToO basis with the selection of a suitable flare-productive AR located on disk, but close to either limb. Operation as outlined below would take place over a 12-24 hour period in conjunction with Proba-2/SWAP. Since the wave observation would begin in response to the XRT flare trigger, the XRT would have the AR in its field-of-view. EIS would engage in a synoptic sit-and-stare study of the quiet Sun in a pre-selected position in the direction of disc centre - positioning to be determined by the proposers. This will allow a comparison of the density change arising from the passage of the EIT wave pulse. However following receipt of the XRT flare trigger signal, EIS would enter continuous sit-and-stare mode with 45s exposures for ~1 - 2hr. XRT would also begin taking higher cadence images for the same time period with the thin filters if possible, although this would be optional.

Annotations:
Hits: 74
Chief Observer
Cruz (RCO)
Related Links
Cites: HOP 207 Support     
Timeline: gif use
See also
Datasets
Get All Data
saaIntervals hiIntervals

wavelength: 6302A Continuum Intensity cadence: 0 min fov: 277,162 images: 873 JavaScript Landing Page
wavelength: 6302A Velocity 6301.5A cadence: 0 min fov: 277,162 images: 873 JavaScript Landing Page
wavelength: 6302A Transverse Flux Density cadence: 0 min fov: 277,162 images: 873 JavaScript Landing Page
wavelength: 6302A Longitudinal Flux Density cadence: 0 min fov: 277,162 images: 873 JavaScript Landing Page
Time Series (SP Datacubes)