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Clean up Jee&Tyson citation
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jmeyers314 committed Jun 13, 2017
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Expand Up @@ -240,21 +240,20 @@ \subsection{OpSim Analysis}
to the rotator tracking the sky during exposures, being subject to cable wrap
limits, and occasionally resetting to 0-degrees for filter changes.

Using techniques similar to \citet{Jee&Tyson2011}, Jee and Tyson did a study of
the shear residual systematics due to known LSST CCD brighter-fatter anisotropy
in 100 revisits to a single field with random angular orientations and seeing
sampled from the expected distribution. The Data Management (DM) pipeline will
use a model of the charge transport in the CCD to re-map pixel shapes, sizes,
and areas in pixel level data processing. The needed factor of 10 suppression
of the CCD-based shear systematic residuals (post pixel remap pipeline
correction) was obtained, reaching the SRD floor on cosmic shear systematics
(presented at weak lensing systematics workshop, Dec 2015)
\footnote{\url{https://indico.bnl.gov/conferenceDisplay.py?confId=1604}}. Of
course, the requirements for spatial dithering for shear systematics residuals
depend on the precision of the pixel processing for removal of the CCD based
additive shear systematic. We assume that this pixel level remap in the DM
pipeline cannot correct to better than 3 times the rms errors in the lab tests
for dynamic and static CCD systematics.
\citet{Jee&Tyson2011} did a study of the shear residual systematics due to known
LSST CCD brighter-fatter anisotropy in 100 revisits to a single field with
random angular orientations and seeing sampled from the expected distribution.
The Data Management (DM) pipeline will use a model of the charge transport in
the CCD to re-map pixel shapes, sizes, and areas in pixel level data processing.
The needed factor of 10 suppression of the CCD-based shear systematic residuals
(post pixel remap pipeline correction) was obtained, reaching the SRD floor on
cosmic shear systematics (presented at weak lensing systematics workshop, Dec
2015)\footnote{\url{https://indico.bnl.gov/conferenceDisplay.py?confId=1604}}.
Of course, the requirements for spatial dithering for shear systematics
residuals depend on the precision of the pixel processing for removal of the CCD
based additive shear systematic. We assume that this pixel level remap in the
DM pipeline cannot correct to better than 3 times the rms errors in the lab
tests for dynamic and static CCD systematics.

The distribution of parallactic angles is similarly shown in
\autoref{fig:WL_AngularSpread_ParallacticAngle} and
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