Changeset 1172 in Sophya for trunk/DocHFI_L2


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Timestamp:
Sep 1, 2000, 3:20:13 PM (25 years ago)
Author:
ansari
Message:

MAJ du WBS L2 , R. Ansari 31/8/2000

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1 edited

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  • trunk/DocHFI_L2/wbsl2.tex

    r1168 r1172  
    2424
    2525%  Symboles en bold
    26 \newcommand{\bnu}{\boldsymbol{\nu}}
    27 \newcommand{\bbold}{\boldsymbol{b}}
     26\newcommand{\bnu}{ {\boldsymbol{\nu}} }
     27\newcommand{\bbold}{\boldsymbol{b} }
    2828\newcommand{\dbold}{\boldsymbol{d}}
    2929
     
    4747}
    4848
    49 \titlepfd{PL-HFI-LAL-PW-L2002}{1.2}
     49\titlepfd{PL-HFI-LAL-PW-L2003}{1.2}
    5050
    5151\end{titlepage}
     
    5858\item Version 1.1 (April 2000 - CVS version 1.2) \\
    5959Draft updated using the document prepared at ISCTM and IfA (Edinburgh)
    60 \item Version 1.2 (August 2000 - CVS version 1.6) \\
     60\item Version 1.2 (August 2000 - CVS version 1.7) \\
    6161Inclusion of a section describing notation and conventions,
    6262flow charts. A more detailed description of deliverables is also included.
     
    104104\end{itemize}
    105105
    106 The package \gph{424} should provide a resonably fast and simple
    107 method for reconstructing 2-D maps from cleaned TOI's (from
     106The package \gph{424} should provide a reasonably fast and simple
     107method for reconstructing 2-D maps from cleaned TOI's (output of
    108108\gph{422} and \gph{423}), removing systematic effects (destriping)
    109109and deconvolving the antenna beam pattern. An iterative method
     
    112112complementary functionalities needed for reconstructing
    113113polarisation maps, using data from polarised channels.
    114 The optimal 2-D map reconstruction packages (\gph{426})
     114The optimal 2-D map reconstruction and analysis package (\gph{426})
    115115will implement the best feasible method for analysing the whole
    116116data set from the HFI instrument and building the full sky frequency
     
    145145\ngph{423}     &    5    &     \ngph{428}     &   30    \\
    146146%
    147 \ngph{424}     &   15    &     \ngph{429}     &   10    \\
     147\ngph{424}     &   20    &     \ngph{429}     &   10    \\
    148148%
    149 \ngph{425}     &   15    &                    &         \\
     149\ngph{425}     &   10    &                    &         \\
    150150%               &           &           &       \\
    151151%
     
    162162\end{table}
    163163
    164 \section{HFI data processing steps}
     164\newpage
     165
     166\section{HFI data sets and processing steps}
    165167The major steps for processing Planck-HFI data are briefly described here.
    166168For the sake of clarity, we define here the notation and conventions used
     
    174176axis $\overrightarrow{\Omega}$ direction $(\theta, \phi)$ and the
    175177roll angle $\psi$. The beam direction and orientation can be computed from
    176 the spacecraft attitude ($\overrightarrow{\Omega}, \psi$ using
     178the spacecraft attitude ($\overrightarrow{\Omega}, \psi$) using
    177179the focal plane geometry.
    178 The spin velocity would be denoted $\omega_z$ or $\omega_{\psi}$. \\
     180The spin velocity is denoted $\omega_z$ or $\omega_{\psi}$. \\
    179181A given sky direction is denoted $(\alpha,\delta)$ in equatorial coordinates,
    180182$(l,b)$ in Galactic coordinates or $(\lambda,\beta)$ in ecliptic coordinate.
     
    202204\subsection{Processing steps}
    203205
    204 The level 2 uses the instrument and spacecraft data obtained
    205 from level 1 {\bf DS1} and the instrument calibration data
    206 base {\bf DSCal}. calibration data base contains the
    207 focal plane geometry, detector response and readout
    208 characteristics, beam patterns, filters and polariser
    209 response. The main processing steps for HFI-L2 are
     206The level 2 uses input data from three different sources:
     207\begin{itemize}
     208\item {\bf DS1:} Instrument and spacecraft data obtained
     209from level 1.
     210\item {\bf DSCal:} HFI calibration data base:
     211\begin{itemize}
     212\item Spacecraft and focal plane geometry
     213\item beam patterns
     214\item filters and polariser frequency response
     215\item detector and readout electronic characteristics.
     216\end{itemize}
     217\item {\bf DSExt:} Prior knowlegde of microwave and infrared
     218sky and sources:
     219\begin{itemize}
     220\item Known microwave and infrared source catalogue
     221\item Partial sky maps in different HFI frequency bands
     222(low resolution and/or incomplete sky coverage)
     223\end{itemize}
     224\end{itemize}
     225
     226The main processing steps for HFI-L2 are
    210227briefly described here:
    211228
     
    230247sampling frequency for each component
    231248\begin{itemize}
    232 \item Raw Time Ordered bolometer signals : $b_{raw}^j(t1)$
    233 \item Time Ordered House-keeping data : $HSK(t2)$
     249\item Raw Time Ordered bolometer signals : $\bbold_{raw}^j(t_1)$
     250\item Time Ordered House-keeping data : $HSK(t_2)$
    234251\item Associated orbit and attitude data : Space craft
    235 position $ \boldmath{P}_{xyz}(t3) $, spin axis direction
    236 $\overrightarrow{\Omega}(t3) - (\theta, \phi)(t3)$ and the
    237 roll angle $\psi(t3)$.
     252position $ \boldmath{P}_{xyz}(t_3) $, spin axis direction and
     253spin velocity
     254$\overrightarrow{\Omega}(t_3) \equiv (\theta, \phi, \omega_z)(t_3)$
     255and the roll angle $\psi(t_3)$.
    238256\end{itemize}
    239257
     
    244262\begin{center}
    245263\framebox{
    246 $ \boldmath{L2-2} : \text{DS1} \oplus \text{DSCal} \longrightarrow \text{DS2-2} $
    247 } (non polarised channels) \\
     264$ \boldmath{L2-2} : \text{DS1} \oplus \text{DSCal} \oplus \text{DSExt}
     265\longrightarrow \text{DS2-2} $
     266\makebox[3cm]{(non polarised)} } \\[2 mm]
    248267\framebox{
    249 $ \boldmath{L2-3} : \text{DS1} \oplus \text{DSCal} \longrightarrow \text{DS2-3} $
    250 } (polarised channels)
     268$ \boldmath{L2-3} : \text{DS1} \oplus \text{DSCal} \oplus \text{DSExt}
     269\longrightarrow \text{DS2-3} $
     270\makebox[3cm]{(polarised)} }
    251271\end{center}
    252272In addition to cleaned and calibrated bolometer signals
     
    257277\begin{itemize}
    258278\item Cleaned and calibrated Time Ordered bolometer signals : $\bbold_{c}^j(t_1)$
    259 \item Data quality flag : $qf_{c}^j(t_1)$
     279\item Data quality flag : $\boldsymbol{qf}_{c}^j(t_1)$
    260280\item Reconstructed astrometric calibration parameters \\
    261 The pointing direction and beam orientation $(\alpha , \delta)^j(t1) \gamma(t1)$
     281The pointing direction and beam orientation
     282$(\alpha , \delta)^j(t_1) , \gamma^j(t_1)$
    262283for each detector at any given time can be computed using these parameters.
    263284\item Detector response and photometric calibration parameters
    264285\item Low frequency drifts and noise statistics
    265286\item Reconstructed lobe
    266 \item Size reduced TOI's through appropriate processings such as phase
    267 binning
     287\item Phase-binned or co-added rings
    268288\item Time Ordered House-keeping data : $HSK(t_2)$
    269 \item Associated orbit and attitude data :
    270 $\{ \boldmath{P}_{xyz}(t3) , \overrightarrow{\Omega}(t3) , \psi(t3) \} $
     289\item Orbit and attitude data :
     290$\{ \boldmath{P}_{xyz}(t_3) , \overrightarrow{\Omega}(t_3) , \psi(t_3) \} $
    271291\end{itemize}
    272292
     
    278298noise, main lobe and far side lobe effects, \ldots).
    279299An iterative, sub-optimal processing method is foreseen for
    280 L2-4 and L2-5 (\gph424 and \gph425).
     300L2-4 and L2-5 (\gph{424} and \gph{425}).
    281301\begin{center}
    282302\framebox{
    283 $ \boldmath{L2-2} : \text{DS2-2} \oplus \text{DSCal} \longrightarrow \text{DS2-4} $
    284 } \\
     303$ \boldmath{L2-2} : \text{DS2-2} \oplus \text{DSCal} \oplus \text{DSExt}
     304\longrightarrow \text{DS2-4} \makebox[3cm]{(non polarised)} $
     305} \\[2mm]
    285306\framebox{
    286 $ \boldmath{L2-5} : \text{DS2-3} \oplus \text{DSCal} \longrightarrow \text{DS2-5} $
     307$ \boldmath{L2-5} : \text{DS2-3} \oplus \text{DSCal} \oplus \text{DSExt}
     308\longrightarrow \text{DS2-5} \makebox[3cm]{(polarised)} $
    287309}
    288310\end{center}
     
    290312maps are the main outputs of {\bf L2-4} and {\bf L2-5}:
    291313\begin{itemize}
    292 \item Reprocessed, calibrated Time Ordered bolometer signals : $\bbold_{rc}^j(t_1)$
    293 \item Full sky maps , temperature and polarisation maps (\gph425)
    294 $\boldsymbol{I}\bnu (\alpha,\delta)$, $\boldsymbol{Q}\bnu (\alpha,\delta)$,
    295 $\boldsymbol{U}\bnu (\alpha,\delta)$.
     314\item Reprocessed, calibrated Time Ordered bolometer signals :
     315$\bbold_{rc}^j(t_1)$
     316\item Full sky maps , temperature and polarisation maps (\gph{425})
     317$\boldsymbol{I}^\bnu (\alpha,\delta)$, $\boldsymbol{Q}^\bnu (\alpha,\delta)$,
     318$\boldsymbol{U}^\bnu (\alpha,\delta)$.
    296319\end{itemize}
    297320
    298321\item {\bf L2-6} More complex methods for 2-D map reconstruction and
    299 data analysis are performed at the next step (\bf L2-6 , \gph426)
     322data analysis are performed at the next step ({\bf L2-6} , \gph{426})
    300323\begin{center}
    301324\framebox{
    302 $ \boldmath{L2-6} : \text{DS2-2} \oplus \text{DS2-3} \oplus \text{DSCal} \longrightarrow \text{DS2-6} $
     325$ \boldmath{L2-6} : \text{DS2-2} \oplus \text{DS2-3} \oplus \text{DSCal}
     326\oplus \text{DSExt} \longrightarrow \text{DS2-6} $
    303327}
    304328\end{center}
     
    308332\begin{center}
    309333\framebox{
    310 $ \boldmath{L2-7} : \text{DS2-2} \oplus \text{DS2-3} \oplus \text{DSCal} \longrightarrow \text{DS2-7} $ (ECSC)
     334$ \boldmath{L2-7} : \text{DS2-2} \oplus \text{DS2-3} \oplus \text{DSCal}
     335\oplus \text{DSExt} \longrightarrow \text{DS2-7} $ \makebox[2cm]{(ECSC)} 
    311336}
    312337\end{center}
    313338
    314 The \bf{DS2-2} and  \bf{DS2-3} are used to produce the source catalogue 
     339The {\bf DS2-2} and  {\bf DS2-3} are used to produce the source catalogue 
    315340containing the source positions, brightness and local
    316 sky maps in each frequency bands \bf{DS2-7} :
     341sky maps in each frequency bands {\bf DS2-7} :
    317342\begin{itemize}
    318343\item Source catalogue: $\{ (\alpha,\delta)_i , F_i^{\bnu 1} ,
    319344F_i^{\bnu 2} , \ldots \}$
    320 \item local sky maps: $\{ lm_i(x,y)^{\bnu 1}, lm_i(x,y)^{\bnu 2}, ldots \}$
    321 \end{itemize}
    322 
    323 \end{itemize}
     345\item local sky maps: $\{ lm_i(x,y)^{\bnu 1}, lm_i(x,y)^{\bnu 2}, \ldots \}$
     346\end{itemize}
     347
     348\end{itemize}
     349
     350\newpage
    324351 
    325352\section{GPH421: RTA/QLA Real Time Assesment, Quick Look Analysis}
     
    341368steps for GPH422 is given in figure \ref{fig422}.
    342369
    343 \begin{figure}[htbp]
     370\begin{figure}[h]
    344371\mbox{\hspace*{1cm} \includegraphics[width=7cm]{gph422_1.eps}
    345372      \includegraphics[width=7cm]{gph422_2.eps} }
     
    377404\end{itemize}
    378405
    379 \item[]\gph{422.4}  Astrometric calibration \\
    380 Astrometric calibration using known point sources,
    381 bright sources from the ECSC and galaxy crossing in TOI.
     406\item[]\gph{422.4}  Astrometric calibration
     407\begin{itemize}
     408\item[]422.4.1 Reconstruction of beam direction and orientaion
     409for each detector using auxiliary spacecraft data
     410\item[]422.4.2 Astrometric calibration using galaxy crossing in TOI
     411\item[]422.4.3 Astrometric calibration using known point sources,
     412and bright sources from the ECSC.
     413\end{itemize}
    382414
    383415\item[]\gph{422.5}  Photometric calibration
     
    394426and galaxy crossing \gph{422.3.3}
    395427
    396 \item[]\gph{422.7}  Production of single pointing co-added rings
    397 or
     428\item[]\gph{422.7}  Production of single pointing size reduced TOI's
     429through coadding or phase binning (co-added or phase-binned rings)
    398430 
    399 \item[]\gph{422.9}  Deliverables: Cleaned, calibrated TOI's :
    400 \begin{itemize}
    401 \item $(\alpha, \delta)$, roll angle, calibrated signal 
    402 \item Noise statistics
    403 \item Offset/drifts
    404 \item Co-added rings
     431\item[]\gph{422.9}  Deliverables: {\bf DS2-2} Cleaned, calibrated TOI's :
     432\begin{itemize}
     433\item Cleaned and calibrated Time Ordered bolometer signals : $\bbold_{c}^j(t_1)$
     434\item Data quality flag : $\boldsymbol{qf}_{c}^j(t_1)$
     435\item Reconstructed astrometric calibration parameters \\
     436The pointing direction and beam orientation
     437$(\alpha , \delta)^j(t_1) , \gamma^j(t_1)$
     438for each detector at any given time can be computed using these parameters.
     439\item Detector response and photometric calibration parameters
     440\item Low frequency drifts and noise statistics
     441\item Reconstructed lobe
     442\item Phase-binned or co-added rings
     443\item Time Ordered House-keeping data : $HSK(t_2)$
     444\item Orbit and attitude data :
     445$\{ \boldmath{P}_{xyz}(t_3) , \overrightarrow{\Omega}(t_3) , \psi(t_3) \} $
    405446\end{itemize}
    406447
     
    409450\section{GPH423: Polarised TOI processing}
    410451
    411 \gph{423.1} Additional TOI processing, as required to
    412 reconstruct Stokes I,Q,U parameters from detector signals
    413 in polarised channels.
     452\gph{423.1} Additional TOI processing or adapted versions of \gph{422}
     453package modules, as required to reconstruct Stokes I,Q,U parameters
     454from detector signals in polarised channels.
     455\begin{itemize}
     456\item[]\gph{423.4}  Astrometric calibration
     457\item[]\gph{423.5}  Photometric calibration
     458\item[]\gph{422.6}  Reconstruction of beam pattern seen by each detector
     459\item[]\gph{423.7}  Production of single pointing size reduced TOI's
     460through coadding or phase binning (co-added or phase-binned rings)
     461\item[]\gph{422.9}  Deliverables: {\bf DS2-3} Cleaned, calibrated TOI's :
     462Reconstructed stokes parameters $\boldsymbol{I}(t_1)$ ,
     463$\boldsymbol{Q}(t_1)$ , $\boldsymbol{U}(t_1)$ in addition to the
     464already listed {\bf DS2-2} data components.
     465\end{itemize}
    414466
    415467\section{GPH424: 2-D map reconstruction}
     
    417469This package contains all the necessary modules for
    418470single frequency 2-D map reconstruction using the cleaned
    419 TOI's from \gph{422} and \gph{423}. However \gph{424}
    420 should only implement simple versions of 2-D map making
    421 and systematic removal algorithms, as opposed to
    422 \gph{424} which must provide a global, optimal 2-D map
    423 reconstruction with systematic effects assessment.
     471TOI's from \gph{422} and \gph{423}. It is not intended to implement
     472the optimal 2-D map reconstruction and data analysis method
     473in this package, which is the task of \gph{426}.
     474An iterative processing method is foreseen for estimating
     475and removing the different systematic effects (low frequency
     476drift, noise, main lobe effect and contamination due to side
     477lobes, using redundancies from the scan strategy and the detectors
     478in a given frequency channel, as well as prior knowledge of microwave
     479and infrared sky. 
     480A very simplified representaion of data flow and processing
     481steps for GPH424 is given in figure \ref{fig424}.
     482\begin{figure}[h]
     483\mbox{\hspace*{2cm} \includegraphics[height=11cm]{gph424_1.eps} }
     484\caption{Data flow and processing steps for GPH424}
     485\label{fig424}
     486\end{figure}
     487
    424488
    425489\begin{itemize}
    426 \item[]\gph{424.1} 1D $\rightarrow$ 2D Projector
    427 \item[]\gph{424.2} Estimation and subtraction of systematic effects 
    428 \begin{itemize}
    429 \item[]424.2.1 Low frequency noise estimation
    430 \item[]424.2.2 far side determination using moon/earth during 
    431 commissioning phases.
    432 \item[]424.2.3 far side lobe subtraction
    433 \item[]424.2.4 use of redundancy to produce independent maps for
    434 assessment of noise contributions
    435 \end{itemize}
    436 
    437 \item[]\gph{424.3} Main lobe
    438 \begin{itemize}
    439 \item[]424.3.1 supplementing source extraction from TOI with
     490
     491\item[]\gph{424.1} Estimation and subtraction of low frequency drifts
     492\begin{itemize}
     493\item[] 424.1.1 Estimation of low frequency drifts using sky scan
     494redundancies (crossings)
     495\item[] 424.1.2 Estimation of low frequency drifts using different
     496detectors in a frequency channel
     497\item[] 424.1.3 Low frequency drift estimation and removal using
     498prior knowledge of microwave and infrared sky (CMB dipole, galaxy, \ldots)
     499\item[] 424.1.4 Iterative low frequency drift estimation and removal
     500using reconstructed sky maps
     501\end{itemize}
     502
     503\item[]\gph{424.2} Side lobe effects
     504\begin{itemize}
     505\item[] 424.2.1 side determination using moon/earth during 
     506commissioning phases
     507\item[] 424.2.2 Iterative side determination using reconstructed
     508sky maps
     509\item[] 424.2.3 Side lobe effect subtraction
     510\end{itemize}
     511
     512\item[]\gph{424.3} Main lobe
     513\begin{itemize}
     514\item[]424.3.1 reconstruction of beam pattern from maps using
     515known point and bright ECSC sources.
     516\item[]424.3.2 supplementing source extraction from TOI with
    440517use of sources selected from frequency maps
    441 \item[]424.3.2 reconstruction of beam pattern from maps using
    442 known point and bright ECSC sources.
    443 \end{itemize}
    444 
    445 
    446 \item[]\gph{424.4} Astrometric calibration using known and
     518\end{itemize}
     519
     520\item[]\gph{424.4} 2-D map reconstruction
     521\begin{itemize}
     522\item[]424.4.1 Local (postage stamp) maps reconstruction
     523\item[]424.4.2 Ring shaped sky strips map reconstruction, using
     524a set of cleaned TOI's from neighbour scans
     525\item[]424.4.3 Full sky map reconstruction by combining the
     526ring shaped sky maps from GPH424.4.2
     527\end{itemize}
     528
     529\item[]\gph{424.5} Astrometric and geometric calibration
     530\begin{itemize}
     531\item[] 424.5.1 Refinement of astrometric calibration using known and
    447532bright ECSC sources.
    448 \item[]\gph{424.5} Photometric calibration
    449 \item[]\gph{424.6} Postage stamp maps for compact sources
    450 
    451 \item[]\gph{424.9} Deliverables: Full sky maps \\
    452 \begin{itemize}
    453 \item Sky maps per frequency channels $map_\nu (\alpha, \delta) $
    454 \item Reprocessed TOI's
     533\item[] 424.5.2 Reconstruction of focal plane geometry and
     534comparison with calibration data base
     535\item[] 424.5.3 Reconstruction of spacecraft attitude and comparison
     536with corresponding data from {\bf DS1} and {\bf DS2-2}.
     537\end{itemize}
     538
     539\item[]\gph{424.6} Photometric calibration
     540
     541\item[]\gph{424.7} Estimation of systematic effect and noise
     542characteristics on reconstructed maps. One way to achieve this is the
     543reconstruction of frequency maps using subsets of detectors in a
     544frequency channel.
     545
     546\item[]\gph{424.9} Deliverables: {\bf DS2-4} Full sky frequency channel
     547maps and reprocessed TOI's
     548\begin{itemize}
     549\item Full sky maps per frequency channels:
     550$\boldsymbol{I}^\bnu (\alpha,\delta)$
     551\item Beam patterns per detector and per frequency channel
     552\item Noise covariance matrix
     553\item Reprocessed, calibrated Time Ordered bolometer signals :
     554$\bbold_{rc}^j(t_1)$
    455555\end{itemize}
    456556
     
    461561for processing polarised TOI's for producing polarisation
    462562sky maps are grouped in this package.
    463 Compared with \gph424 ,
    464 \begin{itemize}
    465 \item[]\gph{425.9} Deliverables: Full sky polarisation maps \\
    466 \begin{itemize}
    467 \item Sky maps per frequency channels $map_\nu (\alpha, \delta) $
    468 \item Reprocessed TOI's
     563The reconstructed sky maps from \gph{424} can be used
     564to assess systematic effects in polarised channel TOI's
     565by combining signal from multiple detectors.
     566
     567\begin{itemize}
     568\item[]\gph{425.1} Estimation and subtraction of low frequency drifts
     569\item[]\gph{425.2} Side lobe effects
     570\item[]\gph{425.3} Main lobe
     571\item[]\gph{425.6} Photometric calibration
     572\item[]\gph{425.8} Reconstruction of stokes (I,Q,U) parameter along the scan
     573\item[]\gph{425.9} Deliverables: {\bf DS2-5} Full sky polarisation maps
     574and reprocessed TOI's
     575\begin{itemize}
     576\item Sky maps per frequency channels: \\
     577$\boldsymbol{I}^\bnu (\alpha,\delta), \boldsymbol{Q}^\bnu (\alpha,\delta),
     578\boldsymbol{U}^\bnu (\alpha,\delta)$
     579\item Beam patterns per detector and per frequency channel
     580\item Noise covariance matrix
     581\item Reprocessed, calibrated Time Ordered bolometer signals :
     582$\bbold_{rc}^j(t_1)$
    469583\end{itemize}
    470584 
     
    478592breakdown structure can only be refined at a later stage,
    479593after preliminary studies of applicable methods.
    480 
    481 \begin{itemize}
    482 \item[]\gph{425.1} Optimal 2-D map reconstruction and analysis
     594One such promising method consist of
     595computing the $a_l^m$ coefficients of the
     596spherical harmonic decomposition of the signal, using
     597the Fourier coefficients of 1-D rings reconstructed from
     598cleaned TOI's. The estimation and removal of low frequency
     599drifts and lobe effects can be incorporated in the
     600processing.
     601
     602\begin{itemize}
     603\item[]\gph{426.1} Optimal 2-D map reconstruction and analysis
    483604for non polarised channels
    484 \item[]\gph{425.2} Optimal 2-D map reconstruction and analysis
     605\item[]\gph{426.2} Optimal 2-D map reconstruction and analysis
    485606for polarised channels
    486607
    487 \item[]\gph{425.9} Deliverables: Full sky maps \\
    488 \begin{itemize}
    489 \item Full sky maps for each frequency channels $map_\nu (\alpha, \delta) $
    490 \item Reprocessed, cleanead TOI's
    491 \item Beam patterns per detector and per frequency channel
    492 \item Estimation of systematics
    493 \end{itemize}
    494 
    495 \end{itemize}
    496 
    497 \section{GPH426: Global polarised 2-D map reconstruction}
    498 
    499 This module, a extended version of \gph{425} has to take
    500 into account specific constraints related to polarised TOI's
    501 and sky map reconstruction
    502 
    503 \begin{itemize}
    504 
    505 \item[]\gph{426.9} Deliverables: full sky maps for each
    506 polarisation component (I,Q,U) \\
    507 \begin{itemize}
    508 \item Full sky maps for each frequency channels $map_\nu (\alpha, \delta) $
    509 for each component (I,Q,U)
     608\item[]\gph{426.9} Deliverables: {\bf DS2-6} Full sky intensity
     609and polarisation maps
     610\begin{itemize}
     611\item Full sky maps for each frequency channels
     612\\ $\boldsymbol{I}^\bnu (\alpha,\delta), \boldsymbol{Q}^\bnu (\alpha,\delta),
     613\boldsymbol{U}^\bnu (\alpha,\delta)$
     614\item Noise and systematic effect maps and characteristics
    510615\item Reprocessed, cleanead TOI's for I,Q,U
    511 \item Noise and systematic effect maps and characteristics
    512616\end{itemize}
    513617
     
    518622
    519623\begin{itemize}
    520 
    521 \item[]\gph{427.9} Deliverables: Source catalogue \\
     624\item[]\gph{427.1} Source extraction, using the data from \gph{422}
     625 and \gph{423}
     626\item[]\gph{427.2} Astrometric calibration
     627\item[]\gph{427.3} Photometric calibration
     628\item[]\gph{427.4} Production of local frequency maps
     629\item[]\gph{427.9} Deliverables: {\bf DS2-7} Early Compact Source Catalogue
     630(ECSC)
    522631\begin{itemize}
    523632\item Astrometrically calibrated source positions and
    524 photometrically calibrated flux in each frequency band \\
    525 $$(\alpha, \delta)_i , F_i^\nu, i=1,..,N$$
    526 \item Llocal sky maps in each frequency bands for areas
    527 around all source positions.
     633photometrically calibrated flux in each frequency band: \\
     634$\{ (\alpha,\delta)_i , F_i^{\bnu 1} ,
     635F_i^{\bnu 2} , \ldots \}$
     636\item Local sky maps in each frequency bands for areas
     637around all source positions: \\
     638$\{ lm_i(x,y)^{\bnu 1}, lm_i(x,y)^{\bnu 2}, \ldots \}$
    528639\item Related software and documentation
    529640\end{itemize}
     
    601712\item[]\gph{429.4} Comparison of TOI data and maps between
    602713HFI and LFI for common 100GHz channel
    603 \item[]\gph{429.9} Deliverables: Full sky maps for each
    604 polarisation component (I,Q,U) \\
    605 \begin{itemize}
    606 \item Sky maps per frequency channels $map_\nu (\alpha, \delta) $
    607 for each component (I,Q,U)
     714\item[]\gph{429.9} Deliverables: ({\bf DS2}) The complete set of deliverables
     715from each L2 package: \\
     716{\bf DS2} = {\bf DS2-2} $\oplus$ {\bf DS2-3} $\oplus$ {\bf DS2-4}
     717$\oplus$ {\bf DS2-5}  $\oplus$ {\bf DS2-6}
     718
     719\begin{itemize}
     720\item Sky maps per frequency channels for each component (I,Q,U) : \\
     721$\boldsymbol{I}^\bnu (\alpha,\delta), \boldsymbol{Q}^\bnu (\alpha,\delta),
     722\boldsymbol{U}^\bnu (\alpha,\delta)$
    608723\item Reprocessed, cleanead TOI's for I,Q,U
    609724\item Noise and systematic effect maps and characteristics
    610725\item Photometric and Astrometric calibration
     726\item Beam patterns for each detector and for each frequency channel
    611727\item Associated software and documentation
    612728\end{itemize}
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