M100 Band3 SingleDish 4.3: Difference between revisions
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[[Category:ALMA]][[Category:Calibration]][[Category:Spectral Line]] | [[Category:ALMA]][[Category:Calibration]][[Category:Spectral Line]] | ||
*'''This guide requires CASA 4.3 and assumes that you have downloaded | *'''This guide requires CASA 4.3 and assumes that you have downloaded M100_Band3_TP_UncalibratedData.tgz as described in [[M100_Band3#Obtaining_the_Data]]''' | ||
*'''Details of the ALMA observations are | *'''Details of the ALMA observations are described at [[M100_Band3]] | ||
*'''This portion of the guide covers calibration | *'''This portion of the guide covers calibration and imaging starting from the raw visibility data.''' | ||
= Overview = | = Overview = | ||
This portion of CASA Guide will cover the data reduction of the Total Power (TP) array observations of M100. | This portion of CASA Guide will cover the data reduction of the Total Power (TP) array observations of M100. | ||
The data consist of | The data consist of "amplitude calibrator" datasets (containing observational data of the quasar 3C279) and "science" datasets containing data for the science target M100. | ||
The data are reduced in the following steps: | The data are reduced in the following steps: | ||
* Both the amplitude calibrator and science datasets are calibrated into units of Kelvins. | * Both the amplitude calibrator and science datasets are calibrated into units of Kelvins. | ||
* The amplitude calibrator data are used | * The radio continuum emission from 3C279 in the amplitude calibrator data are used to derive the Jansky/Kelvin (Jy/K) factors for individual days and frequencies (spectral windows). | ||
* Using the derived Jy/K values, the science data are calibrated into Jy/beam units. | * Using the derived Jy/K values, the science data are calibrated into Jy/beam units. | ||
* The calibrated science data are imaged into a data cube. | * The calibrated science data are imaged into a data cube. | ||
The combination of the resultant image with the interferometric (12-m array and 7-m array) data is explained in a separate page | The combination of the resultant image with the interferometric (12-m array and 7-m array) data is explained in a separate page [[M100_Band3_Combine_4.3]]. | ||
This guide is designed for CASA 4.3.0. | This guide is designed for CASA 4.3.0. | ||
==Confirm | ==Confirm Your Version of CASA== | ||
This guide has been written for CASA release 4.3.0. Please confirm your version before proceeding. | This guide has been written for CASA release 4.3.0. Please confirm your version before proceeding. | ||
| Line 47: | Line 31: | ||
else: | else: | ||
print "Your version of CASA is appropriate for this guide." | print "Your version of CASA is appropriate for this guide." | ||
</source> | |||
== Import "Analysis Utilities" == | |||
The [[Analysis_Utilities]] package will be used for the following processes. | |||
Import the package and instantiate the stuffForScienceDataReduction class therein. | |||
<source lang="python"> | |||
# In CASA | |||
import analysisUtils as aU | |||
es = aU.stuffForScienceDataReduction() | |||
</source> | </source> | ||
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The observations were made on the 1st, 5th, 7th, and 17th July 2014, using two or three 12-m antennas and the ACA correlator. | The observations were made on the 1st, 5th, 7th, and 17th July 2014, using two or three 12-m antennas and the ACA correlator. | ||
The table below indicates the ID's of the Execution Blocks, their start and end times, and the antennas in the array. | The table below indicates the ID's of the Execution Blocks, their start and end times, and the antennas in the array. | ||
There are | There are nine science datasets (i.e., two or three per day). | ||
<pre style="background-color: #E0FFFF;"> | <pre style="background-color: #E0FFFF;"> | ||
#Science | #Science | ||
uid___A002_X85c183_X36f Observed from 2014-07-01T21:51:26.2 to 2014-07-01T22:40:28.4 (UTC) DA61, PM03, PM04 | uid___A002_X85c183_X36f Observed from 2014-07-01T21:51:26.2 to 2014-07-01T22:40:28.4 (UTC) DA61, PM03, PM04 | ||
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</pre> | </pre> | ||
Here we define the list of the Execution Block ID's of the science datasets, to facilitate data reduction using for-loops. | |||
Here we define the | |||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
basename_science = ['uid___A002_X85c183_X36f', 'uid___A002_X85c183_X60b', | basename_science = ['uid___A002_X85c183_X36f', 'uid___A002_X85c183_X60b', | ||
'uid___A002_X8602fa_X2ab', 'uid___A002_X8602fa_X577', | 'uid___A002_X8602fa_X2ab', 'uid___A002_X8602fa_X577', | ||
| Line 90: | Line 74: | ||
</source> | </source> | ||
= | = Calibration into Brightness Temperature in Kelvins = | ||
In this section, the data are calibrated into brightness temperature in units of K. | |||
''This is done in the steps that are described below, using uid___A002_X85c183_X36f as an example.'' | |||
The | If you wish to simply calibrate the data without working through the steps, you can instead execute the script | ||
[[media:A002_X85c183_X36f.ms.scriptForSDCalibration.py|A002_X85c183_X36f.ms.scriptForSDCalibration.py]] using the execfile command. | |||
<pre style="background-color: #E0FFFF;"> | |||
# In CASA | |||
execfile('A002_X85c183_X36f.ms.scriptForSDCalibration.py') | |||
</pre> | |||
The other datasets also need to be calibrated using the following scripts; | |||
[[media:A002_X85c183_X60b.ms.scriptForSDCalibration.py|A002_X85c183_X60b.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X8602fa_X2ab.ms.scriptForSDCalibration.py|A002_X8602fa_X2ab.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X8602fa_X577.ms.scriptForSDCalibration.py|A002_X8602fa_X577.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X864236_X2d4.ms.scriptForSDCalibration.py|A002_X8602fa_X2d4.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X864236_X693.ms.scriptForSDCalibration.py|A002_X864236_X693.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X86fcfa_Xd9.ms.scriptForSDCalibration.py|A002_X86fcfa_Xd9.ms.scriptForSDCalibration.py]], | |||
[[media:A002_X86fcfa_X664.ms.scriptForSDCalibration.py|A002_X86fcfa_X664.ms.scriptForSDCalibration.py]], and | |||
[[media:A002_X86fcfa_X96c.ms.scriptForSDCalibration.py|A002_X86fcfa_X96c.ms.scriptForSDCalibration.py]]. | |||
The following piece of code executes these scripts. | |||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
for | for basename in basename_science: | ||
scriptname = basename[6:]+'.ms.scriptForSDCalibration.py' | |||
if basename == 'uid___A002_X85c183_X36f': | |||
print 'Calibration procedure for %s is described in the Guide.' % basename | |||
print 'Please go through the Guide, ' | |||
print 'or run execfile("%s") instead.' % scriptname | |||
else: | |||
print 'Calibrating %s ...' % basename | |||
execfile(scriptname) | |||
</source> | </source> | ||
== Import the Data == | |||
The | The first thing to do is to convert the dataset into the CASA Measurement Set (MS) format. | ||
The raw data have been provided to you in the ASDM (ALMA Science Data Model). | |||
It is the native format of the data produced by the observatory but cannot be processed by CASA. | |||
The conversion from ASDM to MS is done with the task {{importasdm}}. | |||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
importasdm('uid___A002_X85c183_X36f', | |||
asis='Antenna Station Receiver Source CalAtmosphere CalWVR', | |||
bdfflags=False) | |||
</source> | </source> | ||
The converted dataset (with a suffix ".ms") is created. | |||
Then some sort of flags embedded in the binary files in the ASDM dataset (so-called "BDF flags") are transferred to MS using the command bdflags2MS. | |||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
os.system(os.environ['CASAPATH'].split()[0] + \ | |||
'/bin/bdflags2MS -f "COR DELA INT MIS SIG SYN TFB WVR ZER" ' + \ | |||
'uid___A002_X85c183_X36f uid___A002_X85c183_X36f.ms') | |||
</source> | </source> | ||
== Initial Inspection == | == Initial Inspection == | ||
| Line 146: | Line 154: | ||
</source> | </source> | ||
Alternatively you can use your favorite pager | Alternatively you can use your favorite pager or editor, instead of "cat" command. | ||
Here is an example | Here is an abridged example extracted from the output from listobs for uid___A002_X85c183_X36f: | ||
<pre style="background-color: #fffacd;"> | <pre style="background-color: #fffacd;"> | ||
Fields: 2 | Fields: 2 | ||
ID Code Name RA Decl Epoch SrcId nRows | ID Code Name RA Decl Epoch SrcId nRows | ||
| Line 266: | Line 250: | ||
From this output you can for example see the followings. | From this output you can for example see the followings. | ||
* From "Data records" section: The execution consists of 15 scans with various scan intents. | * From "Data records" section (not shown here): The execution consists of 15 scans with various scan intents. | ||
* From "Spectral Windows" section: | ** Scans 1 and 2 are pointing and sideband gain ratio calibrations (done interferometrically), which need to be done prior to observing the target, on the quasar J1215+1654. | ||
** Scans 3 and 4 are interferometric delay and system noise temperature (Tsys) measurements also on J1215+1654 (they are in principle unnecessary; just a hack to make things happen on the telescope control software). | |||
** Scans 6, 7, 9, 10, 12, 13, and 15, whose scan intents contain "OBSERVE_TARGET", are for raster mapping of the target M100. The associated spectral window (SPW) ID's are 0 and 17-24. | |||
** Scans 5, 8, 11, and 14 with scan intents "CALIBRATE_ATMOSPHERE" are Tsys measurements for M100. The SPW ID's for Tsys scans are 0 and 9-16. | |||
* From "Spectral Windows" section: | |||
** SPW 0 contains the Water Vapor Radiometer (WVR) data, which are taken for all scans, but which are not used here. | |||
** SPW's 1, 3, 5, and 7 are placed on standard continuum frequencies and are used for the pointing scan only. | |||
** SPW's 9, 11, 13, and 15 cover the same frequency range as the science SPW's (see the next bullet) and are used to measure the Tsys used for calibration. They have 128 spectral channels (15.6 MHz spacing) in 2000 MHz bandwidth. | |||
** SPW's 17, 19, 21, and 23 cover the frequency ranges used for the actual science observations. They have 4080 spectral channels (488 kHz spacing) in 1992 MHz bandwidth. Hereafter these SPW's are referred to as "science" SPW's. The target line, CO J=1-0, is placed in SPW 23, the corresponding Tsys is taken from SPW 15. | |||
** The remaining, even-number SPW's contain channel-averages of the actually used SPW's (e.g., SPW 24 corresponds to SPW 23 averaged into one channel). | |||
* From "Antennas" section: Three 12-m antennas (DA61, PM03, and PM04) were used for the observations. | * From "Antennas" section: Three 12-m antennas (DA61, PM03, and PM04) were used for the observations. | ||
| Line 286: | Line 279: | ||
== Convert MS into Single-Dish Data Format == | == Convert MS into Single-Dish Data Format == | ||
To calibrate the data, we need the data to be in the single-dish scantable (ASAP) format. | |||
Most of the tasks that we will use for calibration are inherited from the ASAP package, which has been incorporated into CASA. | Most of the tasks that we will use for calibration are inherited from the ASAP package, which has been incorporated into CASA. | ||
The ASAP package uses a different data format, so from a global point of view, what we are going to do is, first convert the MS to the ASAP format, then run the necessary calibration tasks, then convert the data back to the MS format. | The ASAP package uses a different data format, so from a global point of view, what we are going to do is, first convert the MS to the ASAP format, then run the necessary calibration tasks, then convert the data back to the MS format. | ||
An effort for transition from ASAP to MS is ongoing; in a future version of CASA this step will become unnecessary. | An effort for transition from ASAP to MS is ongoing; in a future version of CASA this step will become unnecessary. | ||
We use the task {{sdsave}} to do this | We use the task {{sdsave}} to do this. | ||
The option outform, which specifies the format of the output data, is left as the default value 'ASAP'. | |||
We will split the data by antennas by using the option splitant=True. | |||
<source lang="python"> | <source lang="python"> | ||
| Line 302: | Line 296: | ||
</source> | </source> | ||
As three antennas were used in the observation, three corresponding ASAP datasets (uid___A002_X85c183_X36f.ms.DA61.asap, uid___A002_X85c183_X36f.ms.PM03.asap, and uid___A002_X85c183_X36f.ms.PM04.asap) are generated. | |||
As usual, we will first obtain information about the content of the datasets, using the task {{sdlist}} (which plays the same role as {{listobs}}). | As usual, we will first obtain information about the content of the datasets, using the task {{sdlist}} (which plays the same role as {{listobs}}). | ||
| Line 312: | Line 306: | ||
</source> | </source> | ||
Here is an example of the output for uid___A002_X85c183_X36f.ms.DA61.asap. The displayed information is in principle the same as what you got from {{listobs}} (except for reduced number of antennas), although {{sdlist}} uses different expression (inherited from ASAP) from that of {{listobs}} (CASA native) -- e.g., "ScanIntent" in {{listobs}} is shown as "SrcType" in {{sdlist}} (CALIBRATE_something to CALON, ON_SOURCE to PSON, OFF_SOURCE to PSOFF, etc.). | Here is an example of the output for uid___A002_X85c183_X36f.ms.DA61.asap. The displayed information is in principle the same as what you got from {{listobs}} (except for reduced number of antennas), although {{sdlist}} uses different expression (inherited from ASAP) from that of {{listobs}} (CASA native) -- e.g., "ScanIntent" in {{listobs}} is shown as "SrcType" in {{sdlist}} (CALIBRATE_something to CALON, ON_SOURCE to PSON, OFF_SOURCE to PSOFF, etc.), and CASA SPWs correspond to ASAP "IF"s. | ||
<source lang="python"> | <source lang="python"> | ||
| Line 413: | Line 407: | ||
Let's start by checking the Tsys. | Let's start by checking the Tsys. | ||
We use the task {{gencal}} to extract the Tsys into a CASA calibration table. | We use the task {{gencal}} to extract the Tsys into a CASA calibration table. | ||
This table is only used for plotting and for letting CASA figure out the mapping between the science and Tsys SPW's (see [[#Tsys_Calibration|"Tsys Calibration" section]]). | |||
<source lang="python"> | <source lang="python"> | ||
| Line 473: | Line 468: | ||
== Tsys Calibration == | == Tsys Calibration == | ||
We calibrate the data into brightness temperature in units of K, using the equation Ta* = Tsys*(ON-OFF)/OFF, where ON and OFF are the data on-source (i.e., during the raster scanning) and off-source (on | We calibrate the data into brightness temperature in units of K, using the equation Ta* = Tsys*(ON-OFF)/OFF, where ON and OFF are the data on-source (i.e., during the raster scanning) and off-source (on a reference position where only background emission exists), respectively. | ||
The calibration is done by the task {{sdcal2}}. | The calibration is done by the task {{sdcal2}}. | ||
It requires the list of the "science" SPW's and Tsys SPW's, and the correspondence between them. | It requires the list of the "science" SPW's and Tsys SPW's, and the correspondence between them. | ||
We can tell from the listobs (or sdlist) output that Tsys SPW's 9, 11, 13, and 15 correspond to "science" SPW's 17, 19, 21, and 23, respectively; but the function tsysspwmap helps to map Tsys SPW's to science SPW's in an automated way: | We can tell from the {{listobs}} (or {{sdlist}}) output that Tsys SPW's 9, 11, 13, and 15 correspond to "science" SPW's 17, 19, 21, and 23, respectively; but the function tsysspwmap helps to map Tsys SPW's to science SPW's in an automated way: | ||
<source lang="python"> | <source lang="python"> | ||
| Line 483: | Line 478: | ||
tsysmap = tsysspwmap(vis='uid___A002_X85c183_X36f.ms', | tsysmap = tsysspwmap(vis='uid___A002_X85c183_X36f.ms', | ||
tsystable='uid___A002_X85c183_X36f.ms.tsys') | tsystable='uid___A002_X85c183_X36f.ms.tsys') | ||
</source> | |||
The obtained variable tsysmap is a list which looks like as follows. The ''N''-th (counted from 0) item indicates the Tsys SPW corresponding to the SPW ID ''N'', e.g., the 23rd item is 15, thus the Tsys SPW 15 corresponds to the science SPW 23. | |||
<pre style="background-color: #fffacd;"> | |||
[0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 9, 11, 11, 13, 13, 15, 15, 9, 9, 11, 11, 13, 13, 15, 15] | |||
</pre> | |||
Now this information needs to be translated into a dictionary variable which {{sdcal2}} requires. The mapping between the science SPW's (17, 19, 21, and 23) and Tsys SPW's is given by the following piece of code: | |||
<source lang="python"> | |||
# In CASA | |||
spwmap = {} | spwmap = {} | ||
for i in [17, 19, 21, 23]: | for i in [17, 19, 21, 23]: | ||
| Line 491: | Line 497: | ||
</source> | </source> | ||
The obtained correspondence between Tsys and science SPW's | The obtained correspondence between Tsys and science SPW's is stored in the dictionary spwmap which looks like the following: | ||
<pre style="background-color: #fffacd;"> | |||
{9: [17], 11: [19], 13: [21], 15: [23]} | |||
</pre> | |||
This is given to sdcal2, along with the comma-separated lists of SPW's. | |||
An important parameter of the task is calmode. | An important parameter of the task is calmode. | ||
In case of the science dataset | In case of the science dataset uid___A002_X85c183_X36f, calmode should be set to 'ps,tsys,apply'. | ||
'ps' means that the data at dedicated reference position are used as "OFF" for the OFF subtraction, (ON-OFF)/OFF. | 'ps' means that the data at dedicated reference position are used as "OFF" for the OFF subtraction, (ON-OFF)/OFF. | ||
'tsys' is to calibrate the data using Tsys. | 'tsys' is to calibrate the data using Tsys. | ||
'apply' is to apply | 'apply' is to apply both calibrations above (OFF-subtraction and Tsys). | ||
<source lang="python"> | <source lang="python"> | ||
| Line 527: | Line 539: | ||
</source> | </source> | ||
For amplitude calibrator datasets, | '''Note:''' For ''amplitude calibrator datasets'', (as opposed to science target maps) the calmode option for sdcal2 should be 'otfraster,tsys,apply' ('otfraster' instead of 'ps'). | ||
'otfraster' tells the task to use | 'otfraster' tells the task to use both ends of each raster row as "OFF" data (as opposed to a dedicated "OFF" sky measurement). | ||
This is because temporal fluctuation of atmospheric emission is the dominant source of noise in radio continuum observations, and hence OFF needs to be as close as possible to ON. | This is because temporal fluctuation of atmospheric emission is the dominant source of noise in radio continuum observations, and hence the "OFF" needs to be as close as possible to the "ON" in time (and spatial location). | ||
== Application of Non-Linearity Correction Factor == | == Application of Non-Linearity Correction Factor == | ||
In the period of Early Science Cycle 1/2, single-dish data taken with the ACA correlator suffer from non-linearity which originates in the digital signal processing. | In the period of Early Science Cycle 1/2, single-dish data taken with the ACA correlator suffer from non-linearity which originates in the digital signal processing. | ||
Its impact was thoroughly studied both experimentally and theoretically, and it was concluded that | Its impact was thoroughly studied both experimentally and theoretically, and it was concluded that multiplication by a correction factor of 1.25 yields an amplitude accuracy of +/-5%. | ||
This is done by the task {{sdscale}}. A new ASAP dataset with additional suffix '.nlc' (for Non-Linearity Correction) will be created for each antenna. | This correction is done by the task {{sdscale}}. A new ASAP dataset with additional suffix '.nlc' (for Non-Linearity Correction) will be created for each antenna. | ||
<source lang="python"> | <source lang="python"> | ||
| Line 545: | Line 557: | ||
</source> | </source> | ||
An upgrade of the ACA correlator hardware and software is expected to solve the non-linearity issue. | |||
Thus this step will become unnecessary in the near future. | Thus this step will become unnecessary for data taken in the near future. | ||
== Baseline Subtraction (only for Science Datasets) == | == Baseline Subtraction (only for Science Datasets) == | ||
We will | '''Note:''' this step is appropriate for spectral line observations (science datasets) but should not be done for the continuum observations (amplitude calibrator datasets) -- ''it would eliminate the continuum emission!'' | ||
With the option "maskmode='auto'", the task automatically finds line features from individual spectra | We will subtract spectral baselines using the task {{sdbaseline}}. | ||
and | |||
A caveat | A tweak (removing flagged rows) is needed before proceeding, to avoid an issue in CASA 4.3 (which has been fixed in CASA 4.4). | ||
<source lang="python"> | |||
# In CASA | |||
for ant in ['DA61', 'PM03', 'PM04']: | |||
tb.open('uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc' % ant, nomodify=False) | |||
subtb = tb.query('FLAGROW==1') | |||
flaggedrows = subtb.rownumbers() | |||
if len(flaggedrows) > 0: tb.removerows(flaggedrows) | |||
subtb.close() | |||
tb.flush() | |||
tb.close() | |||
</source> | |||
Now we are ready to execute {{sdbaseline}}. | |||
With the option "maskmode='auto'", the task automatically finds line features from individual spectra and excludes them from baseline fitting. | |||
A caveat is that the line finding may not work very well in some cases, including this dataset | |||
(see [[#.28Optionally.29_Subtract_a_Residual_Background_from_the_Image|"Subtract a Residual Background from the Image" section]] below). | |||
<source lang="python"> | <source lang="python"> | ||
| Line 586: | Line 614: | ||
</source> | </source> | ||
== Convert Single-Dish Data back to MS Format == | |||
== Convert Single-Dish Data back to MS == | |||
Now the calibrated data need to be coverted back to MS, because the imaging task ({{sdimaging}}) only accepts MS. | Now the calibrated data need to be coverted back to the CASA MS format, because the imaging task ({{sdimaging}}) only accepts MS. | ||
The CASA task {{sdsave}} will do this. | The CASA task {{sdsave}} will do this. | ||
| Line 596: | Line 622: | ||
# In CASA | # In CASA | ||
for ant in ['DA61', 'PM03', 'PM04']: | for ant in ['DA61', 'PM03', 'PM04']: | ||
sdsave(infile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc' % ant, | sdsave(infile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl' % ant, | ||
outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.ms' % ant, | outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl.ms' % ant, | ||
spw='17,19,21,23', | |||
outform='MS2') | outform='MS2') | ||
</source> | </source> | ||
| Line 605: | Line 632: | ||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
concat(vis=['uid___A002_X85c183_X36f.ms.DA61.asap.cal.nlc.ms', | concat(vis=['uid___A002_X85c183_X36f.ms.DA61.asap.cal.nlc.bl.ms', | ||
'uid___A002_X85c183_X36f.ms.PM03.asap.cal.nlc.ms', | 'uid___A002_X85c183_X36f.ms.PM03.asap.cal.nlc.bl.ms', | ||
'uid___A002_X85c183_X36f.ms.PM04.asap.cal.nlc.ms'], | 'uid___A002_X85c183_X36f.ms.PM04.asap.cal.nlc.bl.ms'], | ||
concatvis='uid___A002_X85c183_X36f.ms.cal') | concatvis='uid___A002_X85c183_X36f.ms.cal') | ||
</source> | </source> | ||
| Line 613: | Line 640: | ||
We do not concatenate separate Execution Blocks, because we need to determine and apply day-by-day Jy/K conversion factor. | We do not concatenate separate Execution Blocks, because we need to determine and apply day-by-day Jy/K conversion factor. | ||
Note that one of the antennas, PM02, had a problem in the first baseband (SPW 17) on 2014-07-05, and its impact may not be specific to one SPW | Note that one of the antennas, PM02, had a problem in the first baseband (SPW 17) on 2014-07-05, and its impact may not be specific to this one SPW (e.g., it may have resulted in poor pointing calibration). | ||
Therefore the PM02 data should be excluded from the concatenation | Therefore the PM02 data should be excluded from the concatenation for the affected datasets: uid___A002_X8602fa_Xc3 (amplitude calibrator), | ||
uid___A002_X8602fa_X2ab (science), and uid___A002_X8602fa_X577 (science). | uid___A002_X8602fa_X2ab (science), and uid___A002_X8602fa_X577 (science). | ||
= Image the Amplitude Calibrator and Measure the Value of Jy/K = | = Optionally Image the Amplitude Calibrator and Measure the Value of Jy/K = | ||
At this stage you should have run all 9 science datasets through their respective scriptForSDCalibration.py, i.e., | |||
all 9 datasets have been calibrated into units of Kelvins. The next step is to apply Jy/K conversion factors that have been derived from observations of an amplitude calibrator (one Jy/K value determined per day and per SPW). The resulting Jy/K values are given at the end of this section. | |||
If you want to know details of how the Jy/K values are determined, a summary is given below. Otherwise, you can skip ahead to the next section [[M100_Band3_SingleDish_4.3#Convert the Science Target Units from Kelvin to Jansky]] to continue the calibration. | |||
< | Determination of the Jy/K conversion factor is achieved by imaging a source whose continuum flux is known and measuring the observed brightness temperature. One observation of this source - the amplitude calibrator - was made per day, giving a total of four datasets: | ||
# | <pre style="background-color: #E0FFFF;"> | ||
#Amplitude Calibrator | |||
uid___A002_X85c183_X895 Observed from 2014-07-01T23:35:23.1 to 2014-07-02T00:07:54.6 (UTC) DA61, PM03, PM04 | |||
uid___A002_X8602fa_Xc3 Observed from 2014-07-05T23:21:25.6 to 2014-07-05T23:53:41.0 (UTC) PM02, PM03, PM04 | |||
uid___A002_X864236_Xe1 Observed from 2014-07-07T22:27:35.4 to 2014-07-07T23:01:05.7 (UTC) PM03, PM04 | |||
uid___A002_X86fcfa_X3ae Observed from 2014-07-17T21:48:30.0 to 2014-07-17T22:20:52.2 (UTC) DV10, PM03, PM04 | |||
</pre> | |||
The true size of the beam (point spread function), on which the Jy/K value depends, in a map is determined be several ingredients. | |||
* The intrinsic beam size is determined by the antenna diameter and optics (and of course wavelength). Here we assume the intrinsic beam size of 1.13*lambda/D, where D=12 [m] is the diameter of the antennas, and the factor 1.13 is derived from the optics design of the ALMA 12-m antennas. | |||
* The effective beam size is broadened by the following causes: | |||
** The scanning pattern used to observe the map (i.e., sample spacing in both directions). | |||
** The method used to grid the individual spectra into a map/cube. | |||
The Analysis Utilities provides several tools to get estimates of these. | |||
If you wish to try this out for yourself, you will first need to download the raw amplitude calibrator data file M100_Band3_TP_ampcal_UncalibratedData.tgz. How to obtain the data is described at [[M100_Band3#Obtaining the Data]]. Once you have unpacked the data you will have a directory called M100_Band3_TP_ampcal_UncalibratedData. In this directory, execute the scripts for individual datasets ([[media:A002_X85c183_X895.ms.scriptForSDCalibration.py|A002_X85c183_X895.ms.scriptForSDCalibration.py]], [[media:A002_X8602fa_Xc3.ms.scriptForSDCalibration.py|A002_X8602fa_Xc3.ms.scriptForSDCalibration.py]], [[media:A002_X864236_Xe1.ms.scriptForSDCalibration.py|A002_X864236_Xe1.ms.scriptForSDCalibration.py]], and [[media:A002_X86fcfa_X3ae.ms.scriptForSDCalibration.py|A002_X86fcfa_X3ae.ms.scriptForSDCalibration.py]]) to calibrate all four calibrator datasets (e.g., execfile('A002_X85c183_X895.ms.scriptForSDCalibration.py') in CASA). Then, run the script "[[media:ScriptForImagingAmpCalAndDerivingJyPerK.py|ScriptForImagingAmpCalAndDerivingJyPerK.py]]", which uses for-loops to image the amplitude calibrator and calculate the Jy/K values (run execfile('ScriptForImagingAmpCalAndDerivingJyPerK.py') in CASA). | |||
# In | |||
The resulting Jy/K values are as follows. Note that the values for individual antennas are averaged for each day, each SPW, because the antennas used for the Science observations were not necessarily available for the corresponding amplitude calibrator observations. | |||
The | |||
<pre style="background-color: #E0FFFF;"> | <pre style="background-color: #E0FFFF;"> | ||
| Line 767: | Line 681: | ||
= Convert the Science Target Units from Kelvin to Jansky = | = Convert the Science Target Units from Kelvin to Jansky = | ||
The science data, | The science data, which have been calibrated into brightness temperature in units of K, are now converted into Jy units by multiplying the Jy/K factors derived above. | ||
This step is done by the script " | This step is done by the script "[[media:ScriptForJyPerKConversion.py|ScriptForJyPerKConversion.py]]" (run execfile('ScriptForJyPerKConversion.py') in CASA). | ||
Define the lists of SPWs and corresponding Jy/K factors | Define the lists of SPWs and corresponding Jy/K factors to process the data using for-loops. | ||
<source lang="python"> | <source lang="python"> | ||
| Line 779: | Line 693: | ||
# List the Jy/K values (corresponding to the list of the science spws above) | # List the Jy/K values (corresponding to the list of the science spws above) | ||
# that were the output from | # that were the output from ScriptForImagingAmpCalAndDerivingJyPerK.py | ||
jyperklist0701 = [41.37, 42.39, 43.45, 42.82] | jyperklist0701 = [41.37, 42.39, 43.45, 42.82] | ||
jyperklist0705 = [40.99, 42.74, 40.08, 42.09] | jyperklist0705 = [40.99, 42.74, 40.08, 42.09] | ||
| Line 826: | Line 740: | ||
Now all the science datasets have been calibrated into Jy units. | Now all the science datasets have been calibrated into Jy units. | ||
The next (final) step is to image the science data. | The next (final) step is to image the science data. | ||
This step is done by the script " | This step is done by the script "[[media:ScriptForImagingScienceTarget.py|ScriptForImagingScienceTarget.py]]" (run execfile('ScriptForImagingScienceTarget.py') in CASA). | ||
Define the list of the calibrated science datasets, which the CASA task {{sdimaging}} accepts. | Define the list of the calibrated science datasets, which the CASA task {{sdimaging}} accepts. | ||
| Line 836: | Line 750: | ||
Obtain the data sampling and determine the cell spacing and map size based on the mean frequency of the target SPW. | Obtain the data sampling and determine the cell spacing and map size based on the mean frequency of the target SPW. | ||
This part is in principle the same as the corresponding procedure in the "Image the Amplitude Calibrator and Measure the Value of Jy/K" section. | This part is in principle the same as the corresponding procedure in the [[#Optionally_Image_the_Amplitude_Calibrator_and_Measure_the_Value_of_Jy.2FK|"Optionally Image the Amplitude Calibrator and Measure the Value of Jy/K" section]]. | ||
Please refer to the script "[[media:ScriptForImagingAmpCalAndDerivingJyPerK.py|ScriptForImagingAmpCalAndDerivingJyPerK.py]]" used there. | |||
<source lang="python"> | <source lang="python"> | ||
| Line 861: | Line 776: | ||
Now the data are imaged. | Now the data are imaged. | ||
The velocity channel maps of the CO J=1-0 line (restfreq='115. | The velocity channel maps of the CO J=1-0 line (restfreq='115.271201800GHz') are created as a data cube which covers the velocity range of 1400-1700 km/s at a spacing of 5 km/s (start='1400km/s', width='5km/s', nchan=70). | ||
Note | '''Note:''' The Jy/K value depends on the parameters of gridding convolution (i.e., "gridfunction", "cell", and function-specific parameters ["convsupport" for gridfunction='SF']). | ||
That is, the same gridding parameters should be used for both amplitude calibrator and science images -- otherwise the calibration into Jy unit becomes invalid. | That is, the same gridding parameters should be used for both amplitude calibrator and science images -- otherwise the calibration into Jy unit becomes invalid. | ||
| Line 877: | Line 792: | ||
veltype='radio', | veltype='radio', | ||
outframe='lsrk', | outframe='lsrk', | ||
restfreq='115. | restfreq='115.271201800GHz', | ||
gridfunction='SF', | gridfunction='SF', | ||
convsupport=6, | convsupport=6, | ||
| Line 886: | Line 801: | ||
cell=str(cell)+'arcsec', | cell=str(cell)+'arcsec', | ||
overwrite=True, | overwrite=True, | ||
outfile=' | outfile='M100_TP_CO_cube.image') | ||
</source> | </source> | ||
| Line 894: | Line 809: | ||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
imhead(imagename=' | imhead(imagename='M100_TP_CO_cube.image', | ||
mode='put', | mode='put', | ||
hdkey='bunit', | hdkey='bunit', | ||
| Line 906: | Line 821: | ||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
viewer(' | viewer('M100_TP_CO_cube.image') | ||
</source> | </source> | ||
If you plot the line profile using the viewer, you may notice that the background (i.e., | If you plot the line profile using the viewer, you may notice that the background (i.e., line-free channels) level is slightly negative. | ||
To correct this, spectral baselines are subtracted from the image using the task {{imcontsub}}. | |||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
imcontsub(imagename=' | imcontsub(imagename='M100_TP_CO_cube.image', | ||
linefile=' | linefile='M100_TP_CO_cube.bl.image', | ||
contfile='M100.ignorethis.image', | contfile='M100.ignorethis.image', | ||
fitorder=1, | fitorder=1, | ||
| Line 927: | Line 842: | ||
The impact of this effect would be smaller if the line is brighter, or narrower w.r.t. the correlator bandwidth. | The impact of this effect would be smaller if the line is brighter, or narrower w.r.t. the correlator bandwidth. | ||
== | == Add Restoring Beam Header Information to the Science Image == | ||
The image does not have the beam size, which is necessary for combining the image with interferometric data, in the header. | The image does not have the beam size, which is necessary for combining the image with interferometric data, in the header. | ||
The beam size (including the broadening due to gridding convolution and data sampling) is calculated using the function sfBeam of the Analysis Utilities | The beam size (including the broadening due to gridding convolution and data sampling) is calculated using the function sfBeam of the Analysis Utilities and then written into the header using the functions of the ia tool. | ||
<source lang="python"> | <source lang="python"> | ||
| Line 944: | Line 859: | ||
diameter=diameter) | diameter=diameter) | ||
ia.open(' | ia.open('M100_TP_CO_cube.bl.image') | ||
ia.setrestoringbeam(major=str(sfBeam)+'arcsec', minor=str(sfBeam)+'arcsec', pa='0deg') | ia.setrestoringbeam(major=str(sfBeam)+'arcsec', minor=str(sfBeam)+'arcsec', pa='0deg') | ||
ia.done() | ia.done() | ||
| Line 959: | Line 874: | ||
<source lang="python"> | <source lang="python"> | ||
# In CASA | # In CASA | ||
os.system('rm -rf * | os.system('rm -rf *M100_TP_CO_cube.bl.image.mom0') | ||
immoments(imagename=' | immoments(imagename='M100_TP_CO_cube.bl.image', | ||
moments=[0], | moments=[0], | ||
axis='spectral', | axis='spectral', | ||
chans='8~61', | chans='8~61', | ||
outfile=' | outfile='M100_TP_CO_cube.bl.image.mom0') | ||
viewer(' | viewer('M100_TP_CO_cube.bl.image.mom0') | ||
</source> | </source> | ||
== Combination with 12m and 7m Array Data == | |||
If you wish to learn how to combine the Total Power data with interferometric 12m and 7m data, see the guide for Data Combination [[M100_Band3_Combine_4.3]] | |||
{{Checked 4.3.0}} | |||
Latest revision as of 20:27, 26 August 2015
- This guide requires CASA 4.3 and assumes that you have downloaded M100_Band3_TP_UncalibratedData.tgz as described in M100_Band3#Obtaining_the_Data
- Details of the ALMA observations are described at M100_Band3
- This portion of the guide covers calibration and imaging starting from the raw visibility data.
Overview
This portion of CASA Guide will cover the data reduction of the Total Power (TP) array observations of M100. The data consist of "amplitude calibrator" datasets (containing observational data of the quasar 3C279) and "science" datasets containing data for the science target M100. The data are reduced in the following steps:
- Both the amplitude calibrator and science datasets are calibrated into units of Kelvins.
- The radio continuum emission from 3C279 in the amplitude calibrator data are used to derive the Jansky/Kelvin (Jy/K) factors for individual days and frequencies (spectral windows).
- Using the derived Jy/K values, the science data are calibrated into Jy/beam units.
- The calibrated science data are imaged into a data cube.
The combination of the resultant image with the interferometric (12-m array and 7-m array) data is explained in a separate page M100_Band3_Combine_4.3.
This guide is designed for CASA 4.3.0.
Confirm Your Version of CASA
This guide has been written for CASA release 4.3.0. Please confirm your version before proceeding.
# In CASA
version = casadef.casa_version
print "You are using " + version
if (version < '4.3.0'):
print "YOUR VERSION OF CASA IS TOO OLD FOR THIS GUIDE."
print "PLEASE UPDATE IT BEFORE PROCEEDING."
else:
print "Your version of CASA is appropriate for this guide."
Import "Analysis Utilities"
The Analysis_Utilities package will be used for the following processes. Import the package and instantiate the stuffForScienceDataReduction class therein.
# In CASA
import analysisUtils as aU
es = aU.stuffForScienceDataReduction()
Summary of Datasets
The observations were made on the 1st, 5th, 7th, and 17th July 2014, using two or three 12-m antennas and the ACA correlator. The table below indicates the ID's of the Execution Blocks, their start and end times, and the antennas in the array. There are nine science datasets (i.e., two or three per day).
#Science uid___A002_X85c183_X36f Observed from 2014-07-01T21:51:26.2 to 2014-07-01T22:40:28.4 (UTC) DA61, PM03, PM04 uid___A002_X85c183_X60b Observed from 2014-07-01T22:43:50.0 to 2014-07-01T23:32:39.6 (UTC) DA61, PM03, PM04 uid___A002_X8602fa_X2ab Observed from 2014-07-05T23:58:03.6 to 2014-07-06T00:46:52.0 (UTC) PM02, PM03, PM04 uid___A002_X8602fa_X577 Observed from 2014-07-06T00:55:17.8 to 2014-07-06T01:44:07.3 (UTC) PM02, PM03, PM04 uid___A002_X864236_X2d4 Observed from 2014-07-07T23:03:48.1 to 2014-07-07T23:53:47.9 (UTC) PM03, PM04 uid___A002_X864236_X693 Observed from 2014-07-07T23:56:09.6 to 2014-07-08T00:46:07.1 (UTC) PM03, PM04 uid___A002_X86fcfa_Xd9 Observed from 2014-07-17T20:55:15.5 to 2014-07-17T21:44:06.1 (UTC) DV10, PM03, PM04 uid___A002_X86fcfa_X664 Observed from 2014-07-17T22:24:17.3 to 2014-07-17T23:13:08.0 (UTC) DV10, PM03, PM04 uid___A002_X86fcfa_X96c Observed from 2014-07-17T23:23:37.0 to 2014-07-18T00:12:25.3 (UTC) DV10, PM03, PM04
Here we define the list of the Execution Block ID's of the science datasets, to facilitate data reduction using for-loops.
# In CASA
basename_science = ['uid___A002_X85c183_X36f', 'uid___A002_X85c183_X60b',
'uid___A002_X8602fa_X2ab', 'uid___A002_X8602fa_X577',
'uid___A002_X864236_X2d4', 'uid___A002_X864236_X693',
'uid___A002_X86fcfa_Xd9', 'uid___A002_X86fcfa_X664',
'uid___A002_X86fcfa_X96c']
Calibration into Brightness Temperature in Kelvins
In this section, the data are calibrated into brightness temperature in units of K.
This is done in the steps that are described below, using uid___A002_X85c183_X36f as an example. If you wish to simply calibrate the data without working through the steps, you can instead execute the script A002_X85c183_X36f.ms.scriptForSDCalibration.py using the execfile command.
# In CASA
execfile('A002_X85c183_X36f.ms.scriptForSDCalibration.py')
The other datasets also need to be calibrated using the following scripts; A002_X85c183_X60b.ms.scriptForSDCalibration.py, A002_X8602fa_X2ab.ms.scriptForSDCalibration.py, A002_X8602fa_X577.ms.scriptForSDCalibration.py, A002_X8602fa_X2d4.ms.scriptForSDCalibration.py, A002_X864236_X693.ms.scriptForSDCalibration.py, A002_X86fcfa_Xd9.ms.scriptForSDCalibration.py, A002_X86fcfa_X664.ms.scriptForSDCalibration.py, and A002_X86fcfa_X96c.ms.scriptForSDCalibration.py. The following piece of code executes these scripts.
# In CASA
for basename in basename_science:
scriptname = basename[6:]+'.ms.scriptForSDCalibration.py'
if basename == 'uid___A002_X85c183_X36f':
print 'Calibration procedure for %s is described in the Guide.' % basename
print 'Please go through the Guide, '
print 'or run execfile("%s") instead.' % scriptname
else:
print 'Calibrating %s ...' % basename
execfile(scriptname)
Import the Data
The first thing to do is to convert the dataset into the CASA Measurement Set (MS) format. The raw data have been provided to you in the ASDM (ALMA Science Data Model). It is the native format of the data produced by the observatory but cannot be processed by CASA. The conversion from ASDM to MS is done with the task importasdm.
# In CASA
importasdm('uid___A002_X85c183_X36f',
asis='Antenna Station Receiver Source CalAtmosphere CalWVR',
bdfflags=False)
The converted dataset (with a suffix ".ms") is created. Then some sort of flags embedded in the binary files in the ASDM dataset (so-called "BDF flags") are transferred to MS using the command bdflags2MS.
# In CASA
os.system(os.environ['CASAPATH'].split()[0] + \
'/bin/bdflags2MS -f "COR DELA INT MIS SIG SYN TFB WVR ZER" ' + \
'uid___A002_X85c183_X36f uid___A002_X85c183_X36f.ms')
Initial Inspection
The usual first step is then to get some basic information about the data. We do this using the task listobs, which will output a detailed summary of each dataset supplied.
# In CASA
listobs(vis='uid___A002_X85c183_X36f.ms',
listfile='uid___A002_X85c183_X36f.ms.listobs')
The output will be sent to the CASA logger, and also written in a file named uid___A002_X85c183_X36f.ms.listobs. You can print the contents of the file to the terminal by typing:
# In CASA
os.system('cat uid___A002_X85c183_X36f.ms.listobs')
Alternatively you can use your favorite pager or editor, instead of "cat" command.
Here is an abridged example extracted from the output from listobs for uid___A002_X85c183_X36f:
Fields: 2
ID Code Name RA Decl Epoch SrcId nRows
0 none J1215+1654 12:15:03.979140 +16.54.37.95680 J2000 0 14661
1 none M100 12:22:54.360000 +15.48.50.60000 J2000 1 61653
Spectral Windows: (25 unique spectral windows and 2 unique polarization setups)
SpwID Name #Chans Frame Ch0(MHz) ChanWid(kHz) TotBW(kHz) CtrFreq(MHz) BBC Num Corrs
0 WVR#NOMINAL 4 TOPO 184550.000 1500000.000 7500000.0 187550.0000 0 XX
1 ALMA_RB_03#BB_1#SW-01#FULL_RES 124 TOPO 91955.512 -15625.000 1937500.0 90994.5750 1 XX YY
2 ALMA_RB_03#BB_1#SW-01#CH_AVG 1 TOPO 90978.950 1734375.000 1734375.0 90978.9500 1 XX YY
3 ALMA_RB_03#BB_2#SW-01#FULL_RES 124 TOPO 93893.012 -15625.000 1937500.0 92932.0750 2 XX YY
4 ALMA_RB_03#BB_2#SW-01#CH_AVG 1 TOPO 92924.262 1937500.000 1937500.0 92924.2625 2 XX YY
5 ALMA_RB_03#BB_3#SW-01#FULL_RES 124 TOPO 102033.637 15625.000 1937500.0 102994.5750 3 XX YY
6 ALMA_RB_03#BB_3#SW-01#CH_AVG 1 TOPO 102986.762 1937500.000 1937500.0 102986.7625 3 XX YY
7 ALMA_RB_03#BB_4#SW-01#FULL_RES 124 TOPO 104033.637 15625.000 1937500.0 104994.5750 4 XX YY
8 ALMA_RB_03#BB_4#SW-01#CH_AVG 1 TOPO 104986.762 1937500.000 1937500.0 104986.7625 4 XX YY
9 ALMA_RB_03#BB_1#SW-01#FULL_RES 128 TOPO 101942.187 -15625.000 2000000.0 100950.0000 1 XX YY
10 ALMA_RB_03#BB_1#SW-01#CH_AVG 1 TOPO 100926.562 1781250.000 1781250.0 100926.5625 1 XX YY
11 ALMA_RB_03#BB_2#SW-01#FULL_RES 128 TOPO 103757.337 -15625.000 2000000.0 102765.1500 2 XX YY
12 ALMA_RB_03#BB_2#SW-01#CH_AVG 1 TOPO 102741.712 1781250.000 1781250.0 102741.7125 2 XX YY
13 ALMA_RB_03#BB_3#SW-01#FULL_RES 128 TOPO 111814.962 15625.000 2000000.0 112807.1500 3 XX YY
14 ALMA_RB_03#BB_3#SW-01#CH_AVG 1 TOPO 112783.712 1781250.000 1781250.0 112783.7125 3 XX YY
15 ALMA_RB_03#BB_4#SW-01#FULL_RES 128 TOPO 113689.962 15625.000 2000000.0 114682.1500 4 XX YY
16 ALMA_RB_03#BB_4#SW-01#CH_AVG 1 TOPO 114658.712 1781250.000 1781250.0 114658.7125 4 XX YY
17 ALMA_RB_03#BB_1#SW-01#FULL_RES 4080 TOPO 101945.850 -488.281 1992187.5 100950.0000 1 XX YY
18 ALMA_RB_03#BB_1#SW-01#CH_AVG 1 TOPO 100949.756 1992187.500 1992187.5 100949.7559 1 XX YY
19 ALMA_RB_03#BB_2#SW-01#FULL_RES 4080 TOPO 103761.000 -488.281 1992187.5 102765.1500 2 XX YY
20 ALMA_RB_03#BB_2#SW-01#CH_AVG 1 TOPO 102764.906 1992187.500 1992187.5 102764.9059 2 XX YY
21 ALMA_RB_03#BB_3#SW-01#FULL_RES 4080 TOPO 111811.300 488.281 1992187.5 112807.1500 3 XX YY
22 ALMA_RB_03#BB_3#SW-01#CH_AVG 1 TOPO 112806.906 1992187.500 1992187.5 112806.9059 3 XX YY
23 ALMA_RB_03#BB_4#SW-01#FULL_RES 4080 TOPO 113686.300 488.281 1992187.5 114682.1500 4 XX YY
24 ALMA_RB_03#BB_4#SW-01#CH_AVG 1 TOPO 114681.906 1992187.500 1992187.5 114681.9059 4 XX YY
Sources: 48
ID Name SpwId RestFreq(MHz) SysVel(km/s)
0 J1215+1654 0 - -
0 J1215+1654 25 - -
0 J1215+1654 26 - -
0 J1215+1654 27 - -
0 J1215+1654 1 - -
0 J1215+1654 2 - -
0 J1215+1654 3 - -
0 J1215+1654 4 - -
0 J1215+1654 5 - -
0 J1215+1654 6 - -
0 J1215+1654 7 - -
0 J1215+1654 8 - -
0 J1215+1654 9 - -
0 J1215+1654 10 - -
0 J1215+1654 11 - -
0 J1215+1654 12 - -
0 J1215+1654 13 - -
0 J1215+1654 14 - -
0 J1215+1654 15 - -
0 J1215+1654 16 - -
0 J1215+1654 17 100950 0
0 J1215+1654 18 100950 0
0 J1215+1654 19 102794.1 0
0 J1215+1654 20 102794.1 0
0 J1215+1654 21 112794.1 0
0 J1215+1654 22 112794.1 0
0 J1215+1654 23 114669.1 0
0 J1215+1654 24 114669.1 0
1 M100 0 - -
1 M100 25 - -
1 M100 26 - -
1 M100 27 - -
1 M100 9 - -
1 M100 10 - -
1 M100 11 - -
1 M100 12 - -
1 M100 13 - -
1 M100 14 - -
1 M100 15 - -
1 M100 16 - -
1 M100 17 100950 0
1 M100 18 100950 0
1 M100 19 102794.1 0
1 M100 20 102794.1 0
1 M100 21 112794.1 0
1 M100 22 112794.1 0
1 M100 23 114669.1 0
1 M100 24 114669.1 0
Antennas: 3:
ID Name Station Diam. Long. Lat. Offset from array center (m) ITRF Geocentric coordinates (m)
East North Elevation x y z
0 DA61 A075 12.0 m -067.45.17.9 -22.53.21.4 -4.5609 -499.7012 23.0322 2225072.419944 -5440148.858968 -2481499.171703
1 PM03 T701 12.0 m -067.45.18.8 -22.53.22.2 -29.1265 -522.7875 22.2052 2225045.995589 -5440149.141967 -2481520.118569
2 PM04 T703 12.0 m -067.45.16.2 -22.53.23.9 42.8797 -575.6910 21.7763 2225104.700870 -5440102.471978 -2481568.689518
From this output you can for example see the followings.
- From "Data records" section (not shown here): The execution consists of 15 scans with various scan intents.
- Scans 1 and 2 are pointing and sideband gain ratio calibrations (done interferometrically), which need to be done prior to observing the target, on the quasar J1215+1654.
- Scans 3 and 4 are interferometric delay and system noise temperature (Tsys) measurements also on J1215+1654 (they are in principle unnecessary; just a hack to make things happen on the telescope control software).
- Scans 6, 7, 9, 10, 12, 13, and 15, whose scan intents contain "OBSERVE_TARGET", are for raster mapping of the target M100. The associated spectral window (SPW) ID's are 0 and 17-24.
- Scans 5, 8, 11, and 14 with scan intents "CALIBRATE_ATMOSPHERE" are Tsys measurements for M100. The SPW ID's for Tsys scans are 0 and 9-16.
- From "Spectral Windows" section:
- SPW 0 contains the Water Vapor Radiometer (WVR) data, which are taken for all scans, but which are not used here.
- SPW's 1, 3, 5, and 7 are placed on standard continuum frequencies and are used for the pointing scan only.
- SPW's 9, 11, 13, and 15 cover the same frequency range as the science SPW's (see the next bullet) and are used to measure the Tsys used for calibration. They have 128 spectral channels (15.6 MHz spacing) in 2000 MHz bandwidth.
- SPW's 17, 19, 21, and 23 cover the frequency ranges used for the actual science observations. They have 4080 spectral channels (488 kHz spacing) in 1992 MHz bandwidth. Hereafter these SPW's are referred to as "science" SPW's. The target line, CO J=1-0, is placed in SPW 23, the corresponding Tsys is taken from SPW 15.
- The remaining, even-number SPW's contain channel-averages of the actually used SPW's (e.g., SPW 24 corresponds to SPW 23 averaged into one channel).
- From "Antennas" section: Three 12-m antennas (DA61, PM03, and PM04) were used for the observations.
The scan pattern of the raster mapping can be visualized by issueing the following command. A plot will be shown in a window and also saved as a PNG file uid___A002_X85c183_X36f.ms.sampling.png.
<figure id="X36f.TPSampling.png">
</figure>
# In CASA
aU.getTPSampling(vis='uid___A002_X85c183_X36f.ms',
showplot=True,
plotfile='uid___A002_X85c183_X36f.ms.sampling.png')
Convert MS into Single-Dish Data Format
To calibrate the data, we need the data to be in the single-dish scantable (ASAP) format. Most of the tasks that we will use for calibration are inherited from the ASAP package, which has been incorporated into CASA. The ASAP package uses a different data format, so from a global point of view, what we are going to do is, first convert the MS to the ASAP format, then run the necessary calibration tasks, then convert the data back to the MS format. An effort for transition from ASAP to MS is ongoing; in a future version of CASA this step will become unnecessary.
We use the task sdsave to do this. The option outform, which specifies the format of the output data, is left as the default value 'ASAP'. We will split the data by antennas by using the option splitant=True.
# In CASA
sdsave(infile='uid___A002_X85c183_X36f.ms',
splitant=True,
outfile='uid___A002_X85c183_X36f.ms.asap',
overwrite=True)
As three antennas were used in the observation, three corresponding ASAP datasets (uid___A002_X85c183_X36f.ms.DA61.asap, uid___A002_X85c183_X36f.ms.PM03.asap, and uid___A002_X85c183_X36f.ms.PM04.asap) are generated. As usual, we will first obtain information about the content of the datasets, using the task sdlist (which plays the same role as listobs).
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdlist(infile='uid___A002_X85c183_X36f.ms.%s.asap' % ant,
outfile='uid___A002_X85c183_X36f.ms.%s.asap.sdlist' % ant)
Here is an example of the output for uid___A002_X85c183_X36f.ms.DA61.asap. The displayed information is in principle the same as what you got from listobs (except for reduced number of antennas), although sdlist uses different expression (inherited from ASAP) from that of listobs (CASA native) -- e.g., "ScanIntent" in listobs is shown as "SrcType" in sdlist (CALIBRATE_something to CALON, ON_SOURCE to PSON, OFF_SOURCE to PSOFF, etc.), and CASA SPWs correspond to ASAP "IF"s.
# In CASA
os.system('cat uid___A002_X85c183_X36f.ms.DA61.asap.sdlist')
--------------------------------------------------------------------------------
Scan Table Summary
--------------------------------------------------------------------------------
Project: uid://A002/X82e287/X3
Obs Date: 2014/07/01/21:49:32
Observer: cvlahakis
Antenna Name: ALMA//DA61@A075
Data Records: 41726 rows
Obs. Type: CALIBRATE_POINTING#ON_SOURCE,CALIBRATE_WVR#ON_SOURCE
Beams: 1
IFs: 25
Polarisations: 2 (linear)
Channels: 4080
Flux Unit: K
Abscissa: Channel
Selection: none
Scan Source Time range Int[s] Record SrcType FreqIDs MolIDs
Beam Position (J2000)
--------------------------------------------------------------------------------
1 J1215+1654 2014/07/01/21:51:26.28 - 21:53:29.48 1.01574 2029 [PSON:CALON] [0, 1, 2, 3, 4, 5, 6, 7, 8] [0]
0 J2000 12:15:03.989 +16.54.37.559
2 J1215+1654 2014/07/01/21:55:24.90 - 21:56:25.45 0.49753 2070 [PSON:CALON, PSOFF:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:15:03.988 +16.54.37.560
3 J1215+1654 2014/07/01/21:56:27.21 - 21:56:53.05 0.500364 594 [PSOFF:CALON, PSON:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:15:03.988 +16.54.37.561
4 J1215+1654 2014/07/01/21:56:56.52 - 21:57:17.88 1.76957 194 [PSON:CALON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:15:03.988 +16.54.37.560
5 M100 2014/07/01/21:58:22.41 - 21:58:47.39 0.500364 594 [PSOFF:CALON, PSON:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:23:13.286 +15.48.50.161
6 M100 2014/07/01/21:59:41.64 - 22:07:36.12 1.01591 7720 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.286 +15.48.50.162
7 M100 2014/07/01/22:07:54.69 - 22:09:19.80 1.01608 1390 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.285 +15.48.50.164
8 M100 2014/07/01/22:09:38.49 - 22:10:03.47 0.500364 594 [PSOFF:CALON, PSON:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:23:13.285 +15.48.50.165
9 M100 2014/07/01/22:10:25.58 - 22:18:18.96 1.01586 7717 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.285 +15.48.50.165
10 M100 2014/07/01/22:18:38.66 - 22:20:39.48 1.01599 1965 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.285 +15.48.50.168
11 M100 2014/07/01/22:20:57.16 - 22:21:23.00 0.500364 594 [PSOFF:CALON, PSON:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:23:13.285 +15.48.50.174
12 M100 2014/07/01/22:21:44.13 - 22:29:38.62 1.01584 7716 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.285 +15.48.50.169
13 M100 2014/07/01/22:30:23.68 - 22:32:24.51 1.01599 1965 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.284 +15.48.50.173
14 M100 2014/07/01/22:33:29.37 - 22:33:54.35 0.500364 594 [PSOFF:CALON, PSON:CALON] [0, 9, 10, 11, 12, 13, 14, 15, 16] [0]
0 J2000 12:23:13.284 +15.48.50.175
15 M100 2014/07/01/22:34:19.84 - 22:40:28.35 1.01584 5990 [PSOFF, PSON] [0, 17, 18, 19, 20, 21, 22, 23, 24] [0, 1, 2, 3, 4]
0 J2000 12:23:13.284 +15.48.50.179
--------------------------------------------------------------------------------
FREQUENCIES: 9
ID IFNO(SPW) #Chans Frame Ch0[MHz] ChanWid[kHz] Center[MHz] POLNOs
0 0 4 TOPO 183925 2500000 187675 [0]
1 1 124 TOPO 91955.5125 -15625 90994.575 [0, 1]
2 2 1 TOPO 90978.95 -1734375 90978.95 [0, 1]
3 3 124 TOPO 93893.0125 -15625 92932.075 [0, 1]
4 4 1 TOPO 92924.2625 -1937500 92924.2625 [0, 1]
5 5 124 TOPO 102033.637 15625 102994.575 [0, 1]
6 6 1 TOPO 102986.762 1937500 102986.762 [0, 1]
7 7 124 TOPO 104033.637 15625 104994.575 [0, 1]
8 8 1 TOPO 104986.762 1937500 104986.762 [0, 1]
9 9 128 TOPO 101942.187 -15625 100950 [0, 1]
10 10 1 TOPO 100926.562 -1781250 100926.562 [0, 1]
11 11 128 TOPO 103757.337 -15625 102765.15 [0, 1]
12 12 1 TOPO 102741.712 -1781250 102741.712 [0, 1]
13 13 128 TOPO 111814.962 15625 112807.15 [0, 1]
14 14 1 TOPO 112783.712 1781250 112783.712 [0, 1]
15 15 128 TOPO 113689.962 15625 114682.15 [0, 1]
16 16 1 TOPO 114658.712 1781250 114658.712 [0, 1]
17 17 4080 TOPO 101945.85 -488.28125 100950 [0, 1]
18 18 1 TOPO 100949.756 -1992187.5 100949.756 [0, 1]
19 19 4080 TOPO 103761 -488.28125 102765.15 [0, 1]
20 20 1 TOPO 102764.906 -1992187.5 102764.906 [0, 1]
21 21 4080 TOPO 111811.3 488.28125 112807.15 [0, 1]
22 22 1 TOPO 112806.906 1992187.5 112806.906 [0, 1]
23 23 4080 TOPO 113686.3 488.28125 114682.15 [0, 1]
24 24 1 TOPO 114681.906 1992187.5 114681.906 [0, 1]
--------------------------------------------------------------------------------
MOLECULES:
ID RestFreq Name
0 [] []
1 [1.0095e+11] [Manual_window(ID=0)]
2 [1.027941e+11] [Manual_window(ID=0)]
3 [1.127941e+11] [Manual_window(ID=0)]
4 [1.146691e+11] [CO_v_0_1_0(ID=3768098)]
--------------------------------------------------------------------------------
Inspect the System Noise Temperature
Let's start by checking the Tsys. We use the task gencal to extract the Tsys into a CASA calibration table. This table is only used for plotting and for letting CASA figure out the mapping between the science and Tsys SPW's (see "Tsys Calibration" section).
# In CASA
gencal(vis='uid___A002_X85c183_X36f.ms',
caltable='uid___A002_X85c183_X36f.ms.tsys',
caltype='tsys')
The generated Tsys calibration table can be plotted using the task plotbandpass and the checkCalTable function of the Analysis Utilities. The generated plots are saved in the directories uid___A002_X85c183_X36f.ms.tsys.plots.overlayTime and uid___A002_X85c183_X36f.ms.tsys.plots.
<figure id="X36f.Tsys.overlayTime.png">
</figure>
<figure id="X36f.Tsys.overlayAntenna.png.png">
</figure>
# In CASA
plotbandpass(caltable='uid___A002_X85c183_X36f.ms.tsys',
overlay='time',
xaxis='freq',
yaxis='amp',
subplot=22,
buildpdf=False,
interactive=False,
showatm=True,
pwv='auto',
chanrange='5~123',
showfdm=True,
field='',
figfile='uid___A002_X85c183_X36f.ms.tsys.plots.overlayTime/uid___A002_X85c183_X36f.ms.tsys')
es.checkCalTable('uid___A002_X85c183_X36f.ms.tsys',
msName='uid___A002_X85c183_X36f.ms',
interactive=False)
A Priori Flagging
Now we do some a-priori flagging of the edge channels. Although the "science" SPW's have 1992 MHz bandwidths with 4080 spectral channels, their edge channels are very noisy, because each intermediate frequency signal path (baseband) is equipped with a bandpass filter of ~1.8 GHz width. We flag 120 channels on each side of the "science" SPW's. As a result 3840 channels (1875 MHz bandwidth), i.e., the same number of channels and bandwidth as FDM SPW's in the 12-m array data, remain in each SPW.
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdflag(infile='uid___A002_X85c183_X36f.ms.%s.asap' % ant,
mode='manual',
spw='17:0~119;3960~4079,19:0~119;3960~4079,21:0~119;3960~4079,23:0~119;3960~4079',
overwrite = True)
Tsys Calibration
We calibrate the data into brightness temperature in units of K, using the equation Ta* = Tsys*(ON-OFF)/OFF, where ON and OFF are the data on-source (i.e., during the raster scanning) and off-source (on a reference position where only background emission exists), respectively. The calibration is done by the task Template:Sdcal2. It requires the list of the "science" SPW's and Tsys SPW's, and the correspondence between them. We can tell from the listobs (or sdlist) output that Tsys SPW's 9, 11, 13, and 15 correspond to "science" SPW's 17, 19, 21, and 23, respectively; but the function tsysspwmap helps to map Tsys SPW's to science SPW's in an automated way:
# In CASA
from recipes.almahelpers import tsysspwmap
tsysmap = tsysspwmap(vis='uid___A002_X85c183_X36f.ms',
tsystable='uid___A002_X85c183_X36f.ms.tsys')
The obtained variable tsysmap is a list which looks like as follows. The N-th (counted from 0) item indicates the Tsys SPW corresponding to the SPW ID N, e.g., the 23rd item is 15, thus the Tsys SPW 15 corresponds to the science SPW 23.
[0, 1, 2, 3, 4, 5, 6, 7, 8, 9, 9, 11, 11, 13, 13, 15, 15, 9, 9, 11, 11, 13, 13, 15, 15]
Now this information needs to be translated into a dictionary variable which Template:Sdcal2 requires. The mapping between the science SPW's (17, 19, 21, and 23) and Tsys SPW's is given by the following piece of code:
# In CASA
spwmap = {}
for i in [17, 19, 21, 23]:
if not tsysmap[i] in spwmap.keys():
spwmap[tsysmap[i]] = []
spwmap[tsysmap[i]].append(i)
The obtained correspondence between Tsys and science SPW's is stored in the dictionary spwmap which looks like the following:
{9: [17], 11: [19], 13: [21], 15: [23]}
This is given to sdcal2, along with the comma-separated lists of SPW's. An important parameter of the task is calmode. In case of the science dataset uid___A002_X85c183_X36f, calmode should be set to 'ps,tsys,apply'. 'ps' means that the data at dedicated reference position are used as "OFF" for the OFF subtraction, (ON-OFF)/OFF. 'tsys' is to calibrate the data using Tsys. 'apply' is to apply both calibrations above (OFF-subtraction and Tsys).
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdcal2(infile='uid___A002_X85c183_X36f.ms.%s.asap' % ant,
calmode='ps,tsys,apply',
spw='9,11,13,15,17,19,21,23',
tsysspw='9,11,13,15',
spwmap=spwmap,
outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal' % ant,
overwrite=True)
A new ASAP dataset with additional suffix '.cal' is generated for each antenna. Before proceeding to the next step, we can plot the calibrated spectra using the SDcheckSpectra function of the Analysis Utilities. PNG files will be created in, e.g., uid___A002_X85c183_X36f.ms.DA61.asap.cal.plots directory. You will find the CO line in SPW 23 of the science datasets.
<figure id="X36f.spw23.cal.png">
</figure>
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
es.SDcheckSpectra('uid___A002_X85c183_X36f.ms.%s.asap.cal' % ant,
spwIds='17,19,21,23',
interactive=False)
Note: For amplitude calibrator datasets, (as opposed to science target maps) the calmode option for sdcal2 should be 'otfraster,tsys,apply' ('otfraster' instead of 'ps'). 'otfraster' tells the task to use both ends of each raster row as "OFF" data (as opposed to a dedicated "OFF" sky measurement). This is because temporal fluctuation of atmospheric emission is the dominant source of noise in radio continuum observations, and hence the "OFF" needs to be as close as possible to the "ON" in time (and spatial location).
Application of Non-Linearity Correction Factor
In the period of Early Science Cycle 1/2, single-dish data taken with the ACA correlator suffer from non-linearity which originates in the digital signal processing. Its impact was thoroughly studied both experimentally and theoretically, and it was concluded that multiplication by a correction factor of 1.25 yields an amplitude accuracy of +/-5%. This correction is done by the task sdscale. A new ASAP dataset with additional suffix '.nlc' (for Non-Linearity Correction) will be created for each antenna.
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdscale(infile='uid___A002_X85c183_X36f.ms.%s.asap.cal' % ant,
outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc' % ant,
factor=1.25)
An upgrade of the ACA correlator hardware and software is expected to solve the non-linearity issue. Thus this step will become unnecessary for data taken in the near future.
Baseline Subtraction (only for Science Datasets)
Note: this step is appropriate for spectral line observations (science datasets) but should not be done for the continuum observations (amplitude calibrator datasets) -- it would eliminate the continuum emission!
We will subtract spectral baselines using the task sdbaseline.
A tweak (removing flagged rows) is needed before proceeding, to avoid an issue in CASA 4.3 (which has been fixed in CASA 4.4).
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
tb.open('uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc' % ant, nomodify=False)
subtb = tb.query('FLAGROW==1')
flaggedrows = subtb.rownumbers()
if len(flaggedrows) > 0: tb.removerows(flaggedrows)
subtb.close()
tb.flush()
tb.close()
Now we are ready to execute sdbaseline. With the option "maskmode='auto'", the task automatically finds line features from individual spectra and excludes them from baseline fitting. A caveat is that the line finding may not work very well in some cases, including this dataset (see "Subtract a Residual Background from the Image" section below).
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdbaseline(infile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc' % ant,
spw='17,19,21,23',
maskmode='auto',
thresh=5.0,
avg_limit=4,
blfunc='poly',
order=1,
outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl' % ant,
overwrite=True)
Datasets with yet another suffix ".bl" are generated. The spectra can be checked using SDcheckSpectra which we have already used in a previous step.
<figure id="X36f.spw23.cal.bl.png">
</figure>
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
es.SDcheckSpectra('uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl' % ant,
spwIds='17,19,21,23',
interactive=False)
Convert Single-Dish Data back to MS Format
Now the calibrated data need to be coverted back to the CASA MS format, because the imaging task (sdimaging) only accepts MS. The CASA task sdsave will do this.
# In CASA
for ant in ['DA61', 'PM03', 'PM04']:
sdsave(infile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl' % ant,
outfile='uid___A002_X85c183_X36f.ms.%s.asap.cal.nlc.bl.ms' % ant,
spw='17,19,21,23',
outform='MS2')
And concatenate the data which were split by antennas, using the task concat.
# In CASA
concat(vis=['uid___A002_X85c183_X36f.ms.DA61.asap.cal.nlc.bl.ms',
'uid___A002_X85c183_X36f.ms.PM03.asap.cal.nlc.bl.ms',
'uid___A002_X85c183_X36f.ms.PM04.asap.cal.nlc.bl.ms'],
concatvis='uid___A002_X85c183_X36f.ms.cal')
We do not concatenate separate Execution Blocks, because we need to determine and apply day-by-day Jy/K conversion factor.
Note that one of the antennas, PM02, had a problem in the first baseband (SPW 17) on 2014-07-05, and its impact may not be specific to this one SPW (e.g., it may have resulted in poor pointing calibration). Therefore the PM02 data should be excluded from the concatenation for the affected datasets: uid___A002_X8602fa_Xc3 (amplitude calibrator), uid___A002_X8602fa_X2ab (science), and uid___A002_X8602fa_X577 (science).
Optionally Image the Amplitude Calibrator and Measure the Value of Jy/K
At this stage you should have run all 9 science datasets through their respective scriptForSDCalibration.py, i.e., all 9 datasets have been calibrated into units of Kelvins. The next step is to apply Jy/K conversion factors that have been derived from observations of an amplitude calibrator (one Jy/K value determined per day and per SPW). The resulting Jy/K values are given at the end of this section.
If you want to know details of how the Jy/K values are determined, a summary is given below. Otherwise, you can skip ahead to the next section M100_Band3_SingleDish_4.3#Convert the Science Target Units from Kelvin to Jansky to continue the calibration.
Determination of the Jy/K conversion factor is achieved by imaging a source whose continuum flux is known and measuring the observed brightness temperature. One observation of this source - the amplitude calibrator - was made per day, giving a total of four datasets:
#Amplitude Calibrator uid___A002_X85c183_X895 Observed from 2014-07-01T23:35:23.1 to 2014-07-02T00:07:54.6 (UTC) DA61, PM03, PM04 uid___A002_X8602fa_Xc3 Observed from 2014-07-05T23:21:25.6 to 2014-07-05T23:53:41.0 (UTC) PM02, PM03, PM04 uid___A002_X864236_Xe1 Observed from 2014-07-07T22:27:35.4 to 2014-07-07T23:01:05.7 (UTC) PM03, PM04 uid___A002_X86fcfa_X3ae Observed from 2014-07-17T21:48:30.0 to 2014-07-17T22:20:52.2 (UTC) DV10, PM03, PM04
The true size of the beam (point spread function), on which the Jy/K value depends, in a map is determined be several ingredients.
- The intrinsic beam size is determined by the antenna diameter and optics (and of course wavelength). Here we assume the intrinsic beam size of 1.13*lambda/D, where D=12 [m] is the diameter of the antennas, and the factor 1.13 is derived from the optics design of the ALMA 12-m antennas.
- The effective beam size is broadened by the following causes:
- The scanning pattern used to observe the map (i.e., sample spacing in both directions).
- The method used to grid the individual spectra into a map/cube.
The Analysis Utilities provides several tools to get estimates of these.
If you wish to try this out for yourself, you will first need to download the raw amplitude calibrator data file M100_Band3_TP_ampcal_UncalibratedData.tgz. How to obtain the data is described at M100_Band3#Obtaining the Data. Once you have unpacked the data you will have a directory called M100_Band3_TP_ampcal_UncalibratedData. In this directory, execute the scripts for individual datasets (A002_X85c183_X895.ms.scriptForSDCalibration.py, A002_X8602fa_Xc3.ms.scriptForSDCalibration.py, A002_X864236_Xe1.ms.scriptForSDCalibration.py, and A002_X86fcfa_X3ae.ms.scriptForSDCalibration.py) to calibrate all four calibrator datasets (e.g., execfile('A002_X85c183_X895.ms.scriptForSDCalibration.py') in CASA). Then, run the script "ScriptForImagingAmpCalAndDerivingJyPerK.py", which uses for-loops to image the amplitude calibrator and calculate the Jy/K values (run execfile('ScriptForImagingAmpCalAndDerivingJyPerK.py') in CASA).
The resulting Jy/K values are as follows. Note that the values for individual antennas are averaged for each day, each SPW, because the antennas used for the Science observations were not necessarily available for the corresponding amplitude calibrator observations.
#Date Amp_Cal_Dataset SPW17 SPW19 SPW21 SPW23 2014-07-01 uid___A002_X85c183_X895 41.37 42.39 43.45 42.82 2014-07-05 uid___A002_X8602fa_Xc3 40.99 42.74 40.08 42.09 2014-07-07 uid___A002_X864236_Xe1 39.42 42.08 40.18 40.82 2014-07-17 uid___A002_X86fcfa_X3ae 43.49 43.70 42.01 43.04
Convert the Science Target Units from Kelvin to Jansky
The science data, which have been calibrated into brightness temperature in units of K, are now converted into Jy units by multiplying the Jy/K factors derived above. This step is done by the script "ScriptForJyPerKConversion.py" (run execfile('ScriptForJyPerKConversion.py') in CASA).
Define the lists of SPWs and corresponding Jy/K factors to process the data using for-loops.
# In CASA
# List the science spws
spwlist = [17, 19, 21, 23]
# List the Jy/K values (corresponding to the list of the science spws above)
# that were the output from ScriptForImagingAmpCalAndDerivingJyPerK.py
jyperklist0701 = [41.37, 42.39, 43.45, 42.82]
jyperklist0705 = [40.99, 42.74, 40.08, 42.09]
jyperklist0707 = [39.42, 42.08, 40.18, 40.82]
jyperklist0717 = [43.49, 43.70, 42.01, 43.04]
Make a copy of calibrated dataset, with an additional suffix ".jy", and multiply the Jy/K value for each SPW. This is done by the scaleAutocorr function of Analysis Utilities.
# In CASA
# Data taken on 2014-07-01
for name in ['uid___A002_X85c183_X36f', 'uid___A002_X85c183_X60b']:
os.system('rm -Rf %s.ms.cal.jy' % name)
os.system('cp -Rf %s.ms.cal %s.ms.cal.jy' % (name, name))
for (spw, jyperk) in zip(spwlist, jyperklist0701):
aU.scaleAutocorr(vis='%s.ms.cal.jy' % name, scale=jyperk, spw=spw)
# Data taken on 2014-07-05
for name in ['uid___A002_X8602fa_X2ab', 'uid___A002_X8602fa_X577']:
os.system('rm -Rf %s.ms.cal.jy' % name)
os.system('cp -Rf %s.ms.cal %s.ms.cal.jy' % (name, name))
for (spw, jyperk) in zip(spwlist, jyperklist0705):
aU.scaleAutocorr(vis='%s.ms.cal.jy' % name, scale=jyperk, spw=spw)
# Data taken on 2014-07-07
for name in ['uid___A002_X864236_X2d4', 'uid___A002_X864236_X693']:
os.system('rm -Rf %s.ms.cal.jy' % name)
os.system('cp -Rf %s.ms.cal %s.ms.cal.jy' % (name, name))
for (spw, jyperk) in zip(spwlist, jyperklist0707):
aU.scaleAutocorr(vis='%s.ms.cal.jy' % name, scale=jyperk, spw=spw)
# Data taken on 2014-07-17
for name in ['uid___A002_X86fcfa_Xd9', 'uid___A002_X86fcfa_X664',
'uid___A002_X86fcfa_X96c']:
os.system('rm -Rf %s.ms.cal.jy' % name)
os.system('cp -Rf %s.ms.cal %s.ms.cal.jy' % (name, name))
for (spw, jyperk) in zip(spwlist, jyperklist0717):
aU.scaleAutocorr(vis='%s.ms.cal.jy' % name, scale=jyperk, spw=spw)
Image the Science Target
Now all the science datasets have been calibrated into Jy units. The next (final) step is to image the science data. This step is done by the script "ScriptForImagingScienceTarget.py" (run execfile('ScriptForImagingScienceTarget.py') in CASA).
Define the list of the calibrated science datasets, which the CASA task sdimaging accepts.
# In CASA
sciencedata = [('%s.ms.cal.jy' % name) for name in basename_science]
Obtain the data sampling and determine the cell spacing and map size based on the mean frequency of the target SPW. This part is in principle the same as the corresponding procedure in the "Optionally Image the Amplitude Calibrator and Measure the Value of Jy/K" section. Please refer to the script "ScriptForImagingAmpCalAndDerivingJyPerK.py" used there.
# In CASA
fwhmfactor = 1.13
diameter = 12
xSampling, ySampling, maxsize = aU.getTPSampling(sciencedata[0], showplot=False)
spw = 23
msmd.open(sciencedata[0])
freq = msmd.meanfreq(spw)
msmd.close()
print "SPW %d: %.3f GHz" % (spw, freq*1e-9)
theorybeam = aU.primaryBeamArcsec(frequency=freq*1e-9,
fwhmfactor=fwhmfactor,
diameter=diameter)
cell = theorybeam/9.0
imsize = int(round(maxsize/cell)*2)
Now the data are imaged. The velocity channel maps of the CO J=1-0 line (restfreq='115.271201800GHz') are created as a data cube which covers the velocity range of 1400-1700 km/s at a spacing of 5 km/s (start='1400km/s', width='5km/s', nchan=70).
Note: The Jy/K value depends on the parameters of gridding convolution (i.e., "gridfunction", "cell", and function-specific parameters ["convsupport" for gridfunction='SF']). That is, the same gridding parameters should be used for both amplitude calibrator and science images -- otherwise the calibration into Jy unit becomes invalid.
# In CASA
sdimaging(infiles=sciencedata,
field='M100',
spw='%d' % spw, #sciencespw
nchan=70,
mode='velocity',
start='1400km/s',
width='5km/s',
veltype='radio',
outframe='lsrk',
restfreq='115.271201800GHz',
gridfunction='SF',
convsupport=6,
stokes='',
phasecenter='J2000 12h22m54.9 +15d49m15',
ephemsrcname='',
imsize=imsize,
cell=str(cell)+'arcsec',
overwrite=True,
outfile='M100_TP_CO_cube.image')
The produced image has the brightness unit of K in the image header, which is not correct. Modify the header using the task imhead.
# In CASA
imhead(imagename='M100_TP_CO_cube.image',
mode='put',
hdkey='bunit',
hdvalue='Jy/beam')
(Optionally) Subtract a Residual Background from the Image
Now you can browse the data cube using the viewer.
# In CASA
viewer('M100_TP_CO_cube.image')
If you plot the line profile using the viewer, you may notice that the background (i.e., line-free channels) level is slightly negative. To correct this, spectral baselines are subtracted from the image using the task imcontsub.
# In CASA
imcontsub(imagename='M100_TP_CO_cube.image',
linefile='M100_TP_CO_cube.bl.image',
contfile='M100.ignorethis.image',
fitorder=1,
chans='0~7;62~69')
os.system('rm -rf M100.ignorethis.image')
The main cause of the negative baseline is the following. The task sdbaseline with maskmode='auto' is supposed to find lines from the data and exclude the detected lines from baseline fitting. However, the CO line from M100 is not bright enough to be detected from individual spectra (1-s integration), and hence sdbaseline included the velocity ranges of the line into baseline fitting. The impact of this effect would be smaller if the line is brighter, or narrower w.r.t. the correlator bandwidth.
Add Restoring Beam Header Information to the Science Image
The image does not have the beam size, which is necessary for combining the image with interferometric data, in the header. The beam size (including the broadening due to gridding convolution and data sampling) is calculated using the function sfBeam of the Analysis Utilities and then written into the header using the functions of the ia tool.
# In CASA
minor, major, fwhmsfBeam, sfBeam = aU.sfBeam(frequency=freq*1e-9,
pixelsize=cell,
convsupport=6,
img=None, #to use Gaussian theorybeam
stokes='both',
xSamplingArcsec=xSampling,
ySamplingArcsec=ySampling,
fwhmfactor=fwhmfactor,
diameter=diameter)
ia.open('M100_TP_CO_cube.bl.image')
ia.setrestoringbeam(major=str(sfBeam)+'arcsec', minor=str(sfBeam)+'arcsec', pa='0deg')
ia.done()
Quick Look at the Results
Make a 0th moment (integrated intensity) map using the task immoments and browse it using the viewer.
<figure id="M100.CO.cube.bl.image.mom0.png">
</figure>
# In CASA
os.system('rm -rf *M100_TP_CO_cube.bl.image.mom0')
immoments(imagename='M100_TP_CO_cube.bl.image',
moments=[0],
axis='spectral',
chans='8~61',
outfile='M100_TP_CO_cube.bl.image.mom0')
viewer('M100_TP_CO_cube.bl.image.mom0')
Combination with 12m and 7m Array Data
If you wish to learn how to combine the Total Power data with interferometric 12m and 7m data, see the guide for Data Combination M100_Band3_Combine_4.3
Last checked on CASA Version 4.3.0.
