This page (revision-27) was last changed on 26-Oct-2022 21:57 by Peter Young

This page was created on 07-Jun-2010 19:35 by PeterYoung

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25 05-Apr-2011 18:14 6 KB PeterYoung to previous | to last
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EISmethods
EISmethods

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At line 1 removed 2 lines
[{ALLOW edit EISMainUsers}]
[{ALLOW view Anonymous}]
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To get the 1D wavelength array for the window, do:
!!Pointing coordinates (getxpos, getxcen, etc.)
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{{{IDL> wvl=data->getlam(iwin)
}}}
The heliocentric coordinates for the data are given by
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although bear in mind that the spectra shift in the detector-X direction during an orbit, and in the Y-direction due to the tilt of the EIS slit relative to the detector. These issues are discussed in [EIS Software Note 5|http://solarb.mssl.ucl.ac.uk/SolarB/eis_docs/eis_notes/05_WAVELENGTH_CORRECTION/eis_swnote_05.pdf] and [EIS Software Note 4|http://solarb.mssl.ucl.ac.uk/SolarB/eis_docs/eis_notes/04_SLIT_TILT/eis_swnote_04.pdf], respectively.
{{{IDL> xpos=data->getxpos()
IDL> ypos=data->getypos()}}}
At line 39 changed one line
!!Pointing coordinates (getxpos, getxcen, etc.)
XPOS gives the X-coordinate for each slit position and YPOS gives the position for each pixel in the Y direction. The X-coordinate given includes the jitter (in X) that was recorded by the AOCS system as well as the telscope tracking, the pixel position (Y-coordinate) given does not, but is rather based on the ycen at exposure '0'. In case the latter is desired for exposure 'n' then the (ycen(n)-ycen(0)) should be added to ypos(n) (see below).
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The heliocentric coordinates for the center of a raster at a given wavelength, WVL, are obtained with:
In addition, the coordinates of the reference point used in the data object are given by
At line 43 changed 4 lines
{{{
IDL> xcen=data->getxcen(/raster)
IDL> ycen=data->getycen(wvl,/raster)
}}}
{{{IDL> xcen=data->getxcen()
IDL> ycen=data->getycen()}}}
At line 48 changed one line
More details about EIS pointing information are given on the wiki page [Obtaining pointing information from EIS data|EISPointing].
These points are defined to be the home position of the fine mirror in X including telescope tracking and jitter, and the middle of the physical slit i Y including jitter. Note that this definition differs from that given in the FITS file header where XCEN and YCEN refer to the center of the raster (at the beginning of the observation). Thus, the center of the raster can be accessed by
At line 46 added 2 lines
{{{IDL> xcen=data->getinfo('XCEN')
IDL> ycen=data->getinfo('YCEN')}}}
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!!Time routines
or, perhaps more reliably (especially as concerns older data), by taking the average of the extreme values given by the xpos and ypos methods.
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!Exposure time
Note that each of these is an array of same size as the number of exposures. This is because the center of the raster moves with time due to the spacecraft jitter.
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The exposure time (in seconds) for each exposure of the raster is given by
!!Exposure times and time routines
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The exposure time for each exposure of the raster is given by
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Note that the exposure times generally vary between exposures, and will not be exactly equal to the requested exposure time.
There are a number of other potentially useful methods to time related phenomena:
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!The start and end times of an exposure
The start and end times of an exposure can be obtained through the shutter open and close times (ti1 and ti2):
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The units are given in TI format, which is the Hinode spacecraft time. The TI format can be converted to standard time formats using:
to find the shutter open (and close) times in 'TI' format.
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The last method gives the time in second since the start of the first exposure in the sequence.
NOTE: the difference between the shutter open and close times, and the exposure time returned by the getexp() method generally do not agree. The former being larger by a fraction of a second. There are various technical reasons for this including a latency between the Instrument Control Unit (ICU) communicating with the Mechanism & Heater Controller (MHC), and a delayed response time of the MHC. __Users are recommended to always use the exposure time returned by getexp().__
!Other time routines
The date of an observation can be obtained with various methods:
Convert 'TI' format time to atomic time units ('TAI') or UTC, if no 'ti' parameter is given, the shutter open (ti_1) times for the data object are converted. The final method 'SEC_FROM_OBS_START' computes the number of seconds from the start of observations given by the input array assumed to be in 'TI' format.
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getdate_obs() gives the date in 'yyyy-mm-ddThh:mm:ss.sss' format, and getdate() in 'yyyymmdd' format. The date_obs2date converts the former to the latter format, if no date_obs is given the data object's date_obs is converted. days_since_launch() gives the number of days since launch, if no date is given then the data object's date is used.
Gives the date of obsvation in 'yyyy-mm-ddThh:mm:ss.sss' format ('GETDATE_OBS') or in 'yyyymmdd' format ('GETDATE'). The 'DATE_OBS2DATE' converts the former to the latter format, if no date_obs is given the data objects date_obs is converted. 'DAYS_SINCE_LAUNCH' gives the number of days since launch, if no date is given, the data objects date is used.
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!!Intensity units
To find the units for the intensity arrays in the data object, do
{{{IDL> units=data->getunit()}}}
which returns a 3-element string array, with the first element containing the intensity units. (The other elements are empty.)
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IDL> wp=cal->warm_pixels(data,iwin[0])}}}
IDL> wp=cal->warm_pixels(data,iwin)}}}
This page (revision-27) was last changed on 26-Oct-2022 21:57 by Peter YoungTop