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|| [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline.mpg Vector Hedgehog] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_west.mpg WEST] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_east.mpg EAST] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_large.mpg Vector Hedgehog (large)] ||
|| [ftp:pail.stanford.edu/pub/HMIvector/movie/Ic_Bl.mov Intensity + Blos] || [ftp:pail.stanford.edu/pub/HMIvector/movie/track-movie.2011-feb-NEW_1.mp4 Full Disk Regions 1-16 Feb (HARP 0883)] || [ftp:pail.stanford.edu/pub/HMIvector/movie/track-movie.2011-feb-NEW_2.mp4 Full Disk Regions 16-28 Feb] ||
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 || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline.mpg Vector Hedgehog] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_west.mpg WEST] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_east.mpg EAST] || [ftp:pail.stanford.edu/pub/HMIvector/movie/surface_vectorline_large.mpg Vector Hedgehog (large)] ||

 || [ftp:pail.stanford.edu/pub/HMIvector/movie/Ic_Bl.mov Intensity + Blos] || [ftp:pail.stanford.edu/pub/HMIvector/movie/track-movie.2011-feb-NEW_1.mp4 Full Disk Regions 1-16 Feb (HARP 0883)] || [ftp:pail.stanford.edu/pub/HMIvector/movie/track-movie.2011-feb-NEW_2.mp4 Full Disk Regions 16-28 Feb] ||

Measuring the Vector Magnetic Field of AR 11158 with HMI

The first disambiguated vector field data released by the HMI project for science analysis is a 5-day interval of 12-minute active region patches encompassing AR 11158. The region developed rapidly from February 12-16, 2011 and produced the first X-class flare of Solar Cycle 24 at ~01:56 UT on February 15.

The vector magnetic field is derived from the standard HMI 720-second Stokes-parameter data series, hmi.S_720s. Patches on the Sun that include AR 11158 were identified using the HMI Active Region Patch (HARP) code and then enlarged to provide a surrounding buffer of weak field. The VFISV inversion code was run with very strict convergence criteria to determine the optimal values; this required additional computing resources compared to the expected standard pipeline processing. The disambiguation was computed with spherical geometry in a limited region with fairly generous thresholds on field strength and very gradual annealing; this also required significant additional computing resources.

The HMI team is working to document the reduction pipeline and the uncertainties in the data a processing. We are reasonably confident in the results for this time series and are releasing this first HMI data series for test purposes now. Rather than wait longer, the HMI vector team asks that you treat these preliminary data with care and not publish results until the documentation is complete. The data series may change and the descriptions provided below will definitely improve as we move toward publication in early December, 2011. We welcome your feedback on the data and documentation.

For this specific release, data have been exported into two special formats - direct cut outs and remapped images. Details and helpful information are provided at ReleaseNotes. You are strongly encouraged to read them.

  • For each time in the "cut out" series there are 10 FITS files giving the three vector magnetic field quantities, computed error estimates for each quantity, the three pair-wise correlations between the field quantities (the square root of the covariances), and a quality map, [http://hmi.stanford.edu/doc/magnetic/qual_map.pdf qual_map], with information about the quality of the processing at each pixel. Maps of additional quantities and covariances can be provided on request.

  • Cut outs of the original CCD data are provided in a tracked 650 * 600 CCD-pixel window. The field components are the total flux, the inclination of the field relative to the local line of sight, and the azimuth measured counter-clockwise from 'up' on the CCD. Keywords in each FITS file provide information, including the solar geometry. Note that solar north is down in the cut-outs.

  • The format perhaps more useful for modeling gives remapped images computed with a Lambert cylindrical equal area projection centered on the tracked region. The vector field components are heliographic Br, Btheta, and Bphi on a 600 * 600 longitude - latitude grid. Errors for each component and a quality estimate for the processing, both at the nearest original pixel, are provided, for a total of 7 files per time step.

Vector field data must be used with care. There are several issues with vector magnetic field data that make inversions fail in some pixels and make definitive disambiguation problematic. Additionally, various systematic errors must be considered when using the data. These include daily, 12-hour, and other long-period variations associated with SDO's orbital velocity that cause large-scale spatial and temporal variations in sensitivity and in cross-talk in the Q and U components of the Stokes vector; these arise in part due to limitations in the knowledge of instrument characteristics. Various confidence and error estimates are provided, but they do not always indicate which pixels are suspect. These are describe in the paper outlined below, particularly section 8.

AR 11158 emerged quickly in a complex way, with three major centers of flux emergence. During the build-up to the flare, mixed-polarity regions intensified and strong horizontal flows were apparent. At the time of the flare significant long-lasting changes in the horizontal magnetic field occurred.

The following outlines the analysis of the vector field for this region; the paper based on this outline will be submitted to Solar Physics shortly. Sections will be updated as they become available. Pointers to the data and more detailed treatments of some aspects of the processing follow. We strongly advise that you become familiar with the strengths and weaknesses of the data outlined below. Please contact a member of the VectorFieldTeam if you have questions about the data.

Measuring the Vector Magnetic Field of AR 11158 with HMI

  • 1 Intro – Vector magnetic fields
    • 1.1 HMI Vector Field Overview
    • 1.2 AR 11158 – X-class Flare
  • 2 Instrument and Data Processing
    • 2.1 HMI instrument
    • 2.2 Framelist for vector field
    • 2.3 Relevant calibration of HMI instrument
    • 2.4 Specifics of vector data camera, filtergrams
    • 2.5 Processing of filtergrams – dark, flat, cosmic rays, gap filling, distortion
    • 2.6 Pipeline and special HMI processing

  • 3 IQUV calculation [http://hmi.stanford.edu/doc/magnetic/observables_code.pdf Section 3]

    • 3.1 Computation of IQUV
    • 3.2 720 calculation – interpolation in time and space, averaging
    • 3.3 Other 720s quantities (very briefly)

  • 4 VFISV inversion [http://hmi.stanford.edu/doc/magnetic/section4.pdf Section 4 ]

    • 4.1 ME method and VFISV summary
    • 4.2 Specifics of implemented VFISV for this data series
      • 4.2.1 Weighting
      • 4.2.2 Filter Profile Approximation - Wavelength Hack
      • 4.2.3 Model Initialization
      • 4.2.4 Convergence Criteria, multiple minima
    • 4.3 Formal Error estimation

  • 5 Disambiguation [http://hmi.stanford.edu/doc/magnetic/disambig_longer.pdf Section 5]

    • 5.1 General method, issues, and uncertainties - planar and spherical
      • 5.1.1 Selection of Pixels to Anneal
      • 5.1.2 Potential Field Calculation
      • 5.1.3 Minimum Energy Methods
      • 5.1.4 Treatment of Weak Field Areas
    • 5.2 Computation Parameters

  • 6 HMI.B Data series and access VectorPaper6

    • 6.1 Organization of data series
    • 6.2 Details of HMI.B contents
    • 6.3 Description of HARPs
    • 6.4 Export – general

    • 6.5 HMI Vector Data Versions and Referencing Data in publications - VectorDataReference

  • 7 Projections - [http://hmi.stanford.edu/doc/magnetic/VectorTransformation.pdf Remapping and Vector Transformation]

  • 8 Known and unresolved issues with HMI data and processing [http://hmi.stanford.edu/doc/magnetic/hmivectorissues.pdf Section 8 Topics] {10.26.2011}

    • 8.1 Periodic Errors
    • 8.2 Large-scale Variations
    • 8.3 Bad Pixels
    • 8.4 Comparison of Vector and Line-of-Sight Magnetic Field
    • 8.X Inversion Dependence on Initial Guess
    • 8.X Residual Cross-talk
    • 8.X Disambiguation issues
    • 8.X Other systematic and instrumental issues that affect data
  • 9 Discussion of HMI measurements of AR 11158 - Validation
    • 9.1 General comments on determination of vector magnetic field
    • 9.2 Time Evolution of AR 11158 – features both real and otherwise
    • 9.3 Validation and limitations of HMI processing and data
    • 9.4 Qualitative comparison with B_LoS, Hinode, and other field measures
  • 10 Summary
    • 10.1 Remaining work for pipeline modules
    • 10.2 Uses of data – NLFFF, DAVE4VM, other

Access to AR 11158 Vector Field Data

ReleaseNotes for AR 11158 Vector Field Data

Movies of the Vector Field

Vector Field Data - One-Day Tar Files of 12-minute Cadence

One-Per-Day Sample Images and FITS Files

Other HMI data are available

A range of other HMI data pipeline products are available for this time period through the JSOC. These include the original Stokes parameters (the data series hmi.S_720s), the line-of-sight magnetic field (hmi.M), Doppler velocity (hmi.V), continuum intensity (hmi.Ic), line depth (hmi.Ld), and line width (hmi.Lw).

A collection of topical discussions of the processing

Details of some aspects of the processing and some older documentaiton can be found below. Watch for updates:

JsocWiki: VectorPaper (last edited 2013-05-01 04:35:25 by localhost)