euclid nir image simulation
play

Euclid NIR image simulation Gregor Seidel Max Planck Institute for - PowerPoint PPT Presentation

Euclid Consortium Euclid NIR image simulation Gregor Seidel Max Planck Institute for Astronomy Heidelberg EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12 Euclid imagem Consortium what: (1)image / point source simulation


  1. Euclid Consortium Euclid NIR image simulation Gregor Seidel Max Planck Institute for Astronomy Heidelberg EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  2. Euclid imagem Consortium ● what: (1)image / point source simulation and testing pipeline (2)written in C++, Linux, command line user interface ● dependencies: dependencies: libfftw3-dev libcfitsio3-dev libpng12-dev libcairo2-dev libreadline6- dev libpstreams-dev libpthread-stubs0-dev ● initial purpose: determine limiting magnitudes for flat-spectrum point sources (1)gauge influence of individual instrument model parameters (2)optimise requirements on instrument performance margins ● goal: complete NIR imaging module for end to end simulation pipeline EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  3. Euclid simulation pipeline Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  4. Euclid source image Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  5. Euclid source image Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids Skylens+imagem: single H-band detector, using 3 dithers EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  6. Euclid source image Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids Skylens+imagem: single H-band detector, using 3 dithers EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  7. Euclid source image Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids Skylens+imagem: single H-band detector, using 3 dithers EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  8. Euclid source image Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids Skylens+imagem: single H-band detector, using 3 dithers EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  9. Euclid source image Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids Skylens+imagem: single H-band detector, using 3 dithers EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  10. Euclid source Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids imagem: H band window 100x100 pixels Sérsic galaxy, realistic PSF from spectrum (Elisabete Da Cunha) EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  11. Euclid source Consortium ● input fluxes from: (1) Skylens (Massimo Meneghetti, Peter Melchior): raytracing simulation ● accounts for lensing input from cosmological ● simulations Sérsic or HUDF galaxies ● deconvolution through ● wavelet decomposition (2) Sérsic models for galaxies, galaxy and star catalogues (3) Point source grids imagem: Y band grid of 10 x 10 point sources convolved with PSF and background added EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  12. Euclid optics & filter throughput Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  13. Euclid optics & filter throughput Consortium throughputs and spectral energy distribution to ● (1) convert apparent magnitude to flux (2) superimpose wavelength dependent PSF (see below) for arbitrary filters ● (1) get, for any band, 5-sigma limiting magnitudes (2) adjust Y, J, H exposure times to equal limiting magnitude for all bands EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  14. Euclid optical PSF Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  15. Euclid optical PSF Consortium detailed treatment of the optical PSF using PSF database (Frank Grupp, ● Rory Holmes) oversampled PSFs for Y-, J-, H-band filters and 9 field positions from ● 920nm to 2000nm in ~14nm steps ... combined H-band PSF PSFs (shown at 1.4um, 1.6um, 2um) at field position 1, central 522x522 1μm 2 sub-pixels, logarithmic scaling EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  16. Euclid optical PSF Consortium generation of synthetic PSFs of either ● (1) double Gaussian or ... (2) ring shape determination of EE50 and EE80 radii ● signal-to-noise tests: ● ● point source S/N not sensitive to PSF wings ● Size of faint sources comparable to pixel size ● S/N driven by flux on central pixel EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  17. Euclid intrapixel response Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  18. Euclid intrapixel response Consortium the quantum efficiency can vary on the ● surface of each pixel 0.8% error in 3 dithers depending on the shape and strength of the ● variation, the photometry then varies with the sub-pixel position of a source result: intra-pixel variation < 5.5% to obtain ● photometric error < 0.8% in 3 dithers 5% intra-pixel variation measured intra-pixel response variations (N. Barron) 1-dither photometric precision for 5% intra-pixel response variation and varying FWHM of the AOCS + detector (not optical) PSF EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  19. Euclid flat, dark & readnoise Consortium ⋅ background + source system response optical PSF ∗ incident flux AOCS PSF pixel size pixelised flux intra-pixel response flat-field cosmic rays electron image exposure time dark-map Poisson noise dither readout-noise pixel crosstalk data analysis e - /ADU conversion pipelines further dithers drizzled image weight maps catalogues S/N tests dithering strategy EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

  20. Euclid flat, dark & readnoise Consortium varying quantum efficiency, dark ● current and readout noise per pixel can generate histograms from ● existing detector maps or a given mean and standard deviation can generate maps from given ● histograms flatfielding, dark current ● subtraction and weight image for each dither; weights taken into account for drizzling => operability criterium ● operability (logscale) EUCLID CSWG + OUSIM meeting Barcelona Gregor Seidel 10/07/12

Download Presentation
Download Policy: The content available on the website is offered to you 'AS IS' for your personal information and use only. It cannot be commercialized, licensed, or distributed on other websites without prior consent from the author. To download a presentation, simply click this link. If you encounter any difficulties during the download process, it's possible that the publisher has removed the file from their server.

Recommend


More recommend