First Summary of Neptune Beam Measurements

Similar documents
The predicted performance of the ACS coronagraph

NHSC/PACS Webinar. Aperture and pointing corrections for point sources

Calibrating VISTA Data

PACS SED and large range scan AOT release note PACS SED and large range scan AOT release note

DESIGN NOTE: DIFFRACTION EFFECTS

TIRCAM2 (TIFR Near Infrared Imaging Camera - 3.6m Devasthal Optical Telescope (DOT)

Science Detectors for E-ELT Instruments. Mark Casali

arxiv: v1 [astro-ph.im] 26 Mar 2012

An integral eld spectrograph for the 4-m European Solar Telescope

Some plots from March 2007 tests related to bolometer PSF

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for CHOP/NOD Mode. PACS-301 Level 0 to 1 processing

Properties of a Detector

Extracting Photometry from SPIRE Maps

PACS data reduction for the PEP deep extragalactic survey

New Bad Pixel Mask Reference Files for the Post-NCS Era

Observation Data. Optical Images

SPIRE Broad-Band Photometry Extraction

SOAR Integral Field Spectrograph (SIFS): Call for Science Verification Proposals

BAFFLES DESIGN OF THE PROBA-V WIDE FOV TMA

Mini Workshop Interferometry. ESO Vitacura, 28 January Presentation by Sébastien Morel (MIDI Instrument Scientist, Paranal Observatory)

a simple optical imager

Confocal Imaging Through Scattering Media with a Volume Holographic Filter

Exoplanet transit, eclipse, and phase curve observations with JWST NIRCam. Tom Greene & John Stansberry JWST NIRCam transit meeting March 12, 2014

Hewett 1 Imaged by Amateur

New Bad Pixel Mask Reference Files for the Post-NCS Era

CHAPTER 6 Exposure Time Calculations

Image Slicer for the Subaru Telescope High Dispersion Spectrograph

MIRI The Mid-Infrared Instrument for the JWST. ESO, Garching 13 th April 2010 Alistair Glasse (MIRI Instrument Scientist)

Southern African Large Telescope. RSS UW Commissioning Activities,

WFC3 TV3 Testing: IR Channel Nonlinearity Correction

The Issues of Measurement of Optical Hazard Using Photometers EMRP JRP ENG05 Metrology for Solid State Lighting

Wavelength Calibration Accuracy of the First-Order CCD Modes Using the E1 Aperture

What an Observational Astronomer needs to know!

AMIPAS. Advanced Michelson Interferometer for Passive Atmosphere Sounding. Concepts and Technology for Future Atmospheric Chemistry Sensors

QUICK-START GUIDE TO HERSCHEL PACS THE PHOTOMETER. Katrina Exter HERSCHEL-HSC-DOC-2151, version 1.0, February 28, 2017

The Wide Field Imager

GLAO instrument specifications and sensitivities. Yosuke Minowa

Tunable narrow-band filter for imaging polarimetry

Radiometric Solar Telescope (RaST) The case for a Radiometric Solar Imager,

GMT Instruments and AO. GMT Science Meeting - March

Improved Spectra with a Schmidt-Czerny-Turner Spectrograph

erosita mirror calibration:

Commissioning Report for the ATCA L/S Receiver Upgrade Project

Sea Surface Backscatter Distortions of Scanning Radar Altimeter Ocean Wave Measurements

Measurements of Small Vertical Beamsize using a Coded Aperture at Diamond Light Source. C. Bloomer G. Rehm J.W. Flanagan

A Millimeter and Submillimeter Kinetic Inductance Detector Camera

Open Research Online The Open University s repository of research publications and other research outputs

Exo-planet transit spectroscopy with JWST/NIRSpec

FLAT FIELD DETERMINATIONS USING AN ISOLATED POINT SOURCE

Reflectors vs. Refractors

High Power Pulsed Laser Diodes 850-Series

APO TripleSpecTool User s Guide

Antennas. Greg Taylor. University of New Mexico Spring Astronomy 423 at UNM Radio Astronomy

Antennas. Greg Taylor. University of New Mexico Spring Astronomy 423 at UNM Radio Astronomy

NHSC/PACS Web Tutorials Running the PACS Spectrometer pipeline for unchopped line mode. PACS-303 Level 0 to 2 processing

Flux Calibration Monitoring: WFC3/IR G102 and G141 Grisms

Imaging Simulations with CARMA-23

WFC3 SMOV Programs 11436/8: UVIS On-orbit PSF Evaluation

Observational Astronomy

Southern African Large Telescope. RSS CCD Geometry

PACS Benchmarking: Comparison with Ancillary Data Sets II Spitzer MIPS. Roberta Paladini - NHSC/Caltech

Nature Methods: doi: /nmeth Supplementary Figure 1. Resolution of lysozyme microcrystals collected by continuous rotation.

Properties of Structured Light

ARRAY CONTROLLER REQUIREMENTS

ACIS ( , ) total e e e e-11 1.

Optical design of Dark Matter Telescope: improving manufacturability of telescope

Kepler photometric accuracy with degraded attitude control: Simulation of White Paper Attitude

Multi aperture coherent imaging IMAGE testbed

SUPPLEMENTARY INFORMATION Polarization response of nanowires à la carte

Intra-Pixel Sensitivity Variation and Charge Transfer Inefficiency Results of CCD Scans

or 640 x 480 pixels x 17 u Average Transmission 96% or 88% Depends on front surface coating (AR or DLC)

CCD reductions techniques

WFC3 Thermal Vacuum Testing: UVIS Science Performance Monitor

EE119 Introduction to Optical Engineering Fall 2009 Final Exam. Name:

Acquisition. Some slides from: Yung-Yu Chuang (DigiVfx) Jan Neumann, Pat Hanrahan, Alexei Efros

COS Near-UV Flat Fields and High S/N Determination from SMOV Data

Flat Fields. S. Eikenberry Obs Tech

NANO 703-Notes. Chapter 9-The Instrument

Astronomy 341 Fall 2012 Observational Astronomy Haverford College. CCD Terminology

WFC3 Thermal Vacuum Testing: UVIS Broadband Flat Fields

Spectral Line Bandpass Removal Using a Median Filter Travis McIntyre The University of New Mexico December 2013

NIRCam optical calibration sources

High collection efficiency MCPs for photon counting detectors

METimage Calibration & Performance Verification. Xavier Gnata ICSO 2016

The Heterodyne Instrument for the Far-Infrared (HIFI) and its data

Nanonics Systems are the Only SPMs that Allow for On-line Integration with Standard MicroRaman Geometries

Introduction to Interferometry. Michelson Interferometer. Fourier Transforms. Optics: holes in a mask. Two ways of understanding interferometry

Guide to observation planning with GREAT

PROPERTY OF THE LARGE FORMAT DIGITAL AERIAL CAMERA DMC II

MTF and PSF measurements of the CCD detector for the Euclid visible channel

Photometry of the variable stars using CCD detectors

WFC3 SMOV Program 11433: IR Internal Flat Field Observations

High End / Low Cost Pulsed Laser Diodes 905D1SxxUA-Series

Performance status of IASI on MetOp-A and MetOp-B

EE119 Introduction to Optical Engineering Spring 2003 Final Exam. Name:

Observing*Checklist:*A3ernoon*

A Metalens with Near-Unity Numerical Aperture

Epic Detector Matrices

Performance Comparison of Spectrometers Featuring On-Axis and Off-Axis Grating Rotation

5 x 5 pixel field of view II I. II 25 (+4) x 1 Pixel psuedo-slit

Transcription:

First Summary of Neptune Beam Measurements Background subtraction with modified telescope normalization for asymmetric chopping sans nod works very well; offset in Gaussian fit is <.1 of peak value in the blue and <. in the red band S/N sufficient to analyze data per individual detector Relative pointing errors of fitted peak position between different OBSIDs (1σ): (y), 1 (z) Relative pointing errors of fitted peak position within each raster (1σ):. (y),.5 (z) Pointing errors limit precision of derived beam parameters; combining all 7() rasters helps 1

Results for Spectrally Collapsed Data Mean of spectral detectors within one spaxel, bad pixels discarded Fitted -d Gaussian to raster for each spaxel Peak is fitted flux for perfectly centered spaxel as fraction of telescope flux on spaxel Flux is peak FWHMy FWHMz

Beam Parameters per Spectrally Collapsed Spaxel, Averaged over Blue Rasters [arcsec] 1 [arb. units] 1 sigmaflux meanflux.719139 FWHMy FWHMz Peak Flux 5 15 5 5 15 5 3

Beam Parameters per Spectrally Collapsed Spaxel, Averaged over 7 Red Rasters 1 [arcsec] 1 [arb. units] 1 1 sigmaflux meanflux 3.9171 FWHMy FWHMz Peak Flux 5 15 5 5 15 5

1 Beam Parameters per Spectrally Collapsed Spaxel, Individually for 7 Red Raster Wavelengths [arcsec] 1 [arcsec] 1 1 FWHMy FWHMz 5 15 5 5 15 5 Solid lines: parameters for each collapsed spaxel at wavelengths 1, 15, 13, 15, 15, 1, 17 microns. Dashed lines: scaled versions of mean (over all wavelengths) parameters for each collapsed spaxel. Scaling factors.9, 1.5, 1.15 (y) and.9, 1.5, 1.15 (z) 5

Results for Individual Detectors Data from each physical detector analyzed individually, including bad pixels Fitted -d Gaussian to raster for each detector For better S/N and reduction of pointing error effects, means taken over results from all (7) rasters. Not really justified in the red band where beams increase with wavelength! For detectors with little spread in y-direction, broadening of beam from spectral collapse (instead of individual treatment) negligible, but well visible in corner near spaxel 5 (a.k.a. spaxel, if you start counting at ), particularly in the blue band. In the red band you may argue it s not worth the effort.

Beam Parameters for Individual Detectors - Blue [arcsec] [arcsec] FWHMy FWHMy FWHMz FWHMz 5 15 5 Dots: individual detectors, averaged over rasters. Vignetted spaxels have largest scatter in y! Lines: Means of individual detectors in one spaxel, averaged over rasters 5 15 5 Dots: spectrally collapsed spaxels, averaged over rasters. Lines: Means of individual detectors in one spaxel, averaged over rasters 7

Beam Parameters for Individual Detectors - Red 1 [arcsec] 1 [arcsec] 1 1 FWHMy FWHMz 5 15 5 Dots: individual detectors, averaged over 7 rasters. Vignetted spaxels have less scatter in y than in blue band. Lines: Means of individual detectors in one spaxel, averaged over rasters 5 15 5 Dots: spectrally collapsed spaxels, averaged over 7 rasters. Lines: Means of individual detectors in one spaxel, averaged over rasters. Difference less pronounced than in blue

Pointing - Blue Absolute pointing of fitted peak position of collapsed spaxels for each of the rasters Blue: Relative pointing of fitted peak position of collapsed spaxels for each of the rasters, shifted such that mean position of each raster is (, ). Red: Mean of rasters as best guess for focal plane geometry of PACS-S 9

Pointing - Red Absolute pointing of fitted peak position of collapsed spaxels for each of the rasters Blue: Relative pointing of fitted peak position of collapsed spaxels for each of the rasters, shifted such that mean position of each raster is (, ). Red: Mean of rasters as best guess for focal plane geometry of PACS-S

Focal Plane Geometry per Detector - Blue Relative pointing of fitted peak position of individual detectors, collectively shifted for each of the rasters by the same vector as for collapsed spaxels, then averaged per individual detector over the rasters. Best guess for focal plane geometry of PACS-S per individual detector 11

Focal Plane Geometry per Detector - Red Relative pointing of fitted peak position of individual detectors, collectively shifted for each of the rasters by the same vector as for collapsed spaxels, then averaged per individual detector over the rasters. Best guess for focal plane geometry of PACS-S per individual detector 1

FOV Homogeneity To check whether the flux of a point source, collectively measured by the PACS IFU/detectors, is independent of the position of the point source within the IFU, we add up the normalized signals from all spaxels and plot the result as a function of raster pointing. The flatness of the response is best at medium wavelengths, where a point source is providing a sufficiently homogeneous illumination across a spaxel, while the wings don t fall off the IFU too badly, yet. At short wavelengths, the intra-pixel response becomes apparent, which drops off toward the edges. 13

FOV Relative Response Maps µm µm 73µm 75µm µm 9µm (contour levels % of peak value) 1

FOV Relative Response Maps 15µm 13µm 15µm 15µm 1µm 17µm (contour levels % of peak value) 15

Point Source Correction Factor Lines: from A&A paper Dots: from accumulated 3x3 and 5x5 spaxel fluxes vs. fitted peak flux on central spaxel. Question: why more discrepancy in red than in blue? 1

Inter-Spaxel Flatfield (Point Source Flux) 1 1 1 sigmaflux meanflux.719139 1 sigmaflux meanflux 3.9171 Flux (arb. units) blue Flux (arb. units) red 5 15 5 5 15 5 Spaxel number (starting at 1) Spaxel number (starting at 1) Purple dots: fitted peak flux Green dots: fitted peak flux FWHMy FWHMz 17

Telescope Background Flux Model Use point source correction from A&A paper to link observed Neptune peak flux on central spaxel to full Neptune flux from ESA_3 model Fit derived telescope signal (in Jy) on central spaxel with Fischer et al. dusty surface emissivity and telescope temperature + colder graybody term for straylight in cryostat Allow different response to chopped signal vs. static signal (time constants) on red vs. blue detectors flux/spaxel [Jy] measured/model 5 15 1..... StandardDeviationdiff fitted 3.53117 15 1 1 1 1 wavelength 1