spectrometer simulation

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A. Ealet Berkeley, december 2002 1 Spectrometer simulation ote in http://www.astrsp-mrs/snap/spectro/spectrosim.ps Why we need it now What should be simulated How to do it Work plan Conclusion A.Bonissent A.Ealet C.Macaire E.Prieto A.Tilquin

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Why we need it now What should be simulated How to do it Work plan Conclusion. Spectrometer simulation. A.Bonissent A.Ealet C.Macaire E.Prieto A.Tilquin. Note in http://www.astrsp-mrs/snap/spectro/spectrosim.ps. - PowerPoint PPT Presentation

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Page 1: Spectrometer  simulation

A. Ealet Berkeley, december 2002 1

Spectrometer simulation

Note in http://www.astrsp-mrs/snap/spectro/spectrosim.ps

● Why we need it now● What should be simulated● How to do it● Work plan● Conclusion

A.BonissentA.EaletC.MacaireE.PrietoA.Tilquin

Page 2: Spectrometer  simulation

A. Ealet Berkeley, december 2002 2

● Previous stage, only laboratory tests and

simulation of slicer alone have been performed.

● This is sufficient to ensure that an instrument can be built with adequate performance.

● Now to study the real performances on the full instrument, we need a complete simulation

Past

Page 3: Spectrometer  simulation

A. Ealet Berkeley, december 2002 3

● Needed in the present phase for

– Optimizing the design: balance cost and simplicity (reliability) for best possible physics

– compute realistic efficiency – evaluate tolerance– evaluate calibration procedure– produce realistic data to develop and test data

processing algorithms

● At term, it will be used in detailed MC studies for physic analysis

Why

Page 4: Spectrometer  simulation

A. Ealet Berkeley, december 2002 4

Specifications

OK ?

Optical design

Optical simulation

No

Optomechanical simulation

Library of psf

yes

Optimisation process

Page 5: Spectrometer  simulation

A. Ealet Berkeley, december 2002 5

● At the end of phase A, we need a Final design of the instrument with estimated (and justified) performances

● Simulation and data reduction software for evaluation should be ready well before

simulation spring 2003data reduction prototype spring 2004

Développement plan

Page 6: Spectrometer  simulation

A. Ealet Berkeley, december 2002 6

● Full SNAP simulation

SN simulation

analysis

propagation

Data reduction

instrument

Detector pixel data

physic

Data cube

Lightcurvespectra

Lightcurvespectra

Cosmo models

Physic parameters

Page 7: Spectrometer  simulation

A. Ealet Berkeley, december 2002 7

● Spectrometer simulation

telescope

optical sim

readout

pixellisation

slicer

spectrograph

fit Data cubei,j,adc

Parameterization constants

x,y,

x,ypsf1

x,y,psf2

x,y,psf3

i,j,Qij

i,j,Qij

Pixel parameterization

Page 8: Spectrometer  simulation

A. Ealet Berkeley, december 2002 8

TF of amplitude from object plane to pupil plane then to imageApply geometry and phase (zernike) on pupilApply geometry on imageCompute intensity to evaluate efficiencyInterpolate position x,y at each step (need parametrisation)

Output is position on the detector for each point and wavelength with an associated PSF

Very long and CPU intensive

Method

Telescopext,yt,

Slicerxs,ys

Slitxf,yf

prismxl,yl

Detectorxd,yd

pei

Compute Psf and transmission at each x,y,

pupilxp,yp

TF

p peipei ppsf

TFTF TF TF

Page 9: Spectrometer  simulation

A. Ealet Berkeley, december 2002 9

Psf shape and size depends on x,y,(small amount of) energy is lost by diffractionGeometry affects performance

psf

slice

Page 10: Spectrometer  simulation

A. Ealet Berkeley, december 2002 10

0.9 m

1.7 m

Slice 0

Slice 2

Page 11: Spectrometer  simulation

A. Ealet Berkeley, december 2002 11

Zernike Polynomia

from Zeemax are used to introduce aberrations

Depend of,x,y

They need to be extrapolate on each point of the image plan

Use Neural Network technique to do extrapolation

Zernike polynomial of slicer for = 1.7 m

Page 12: Spectrometer  simulation

A. Ealet Berkeley, december 2002 12

psf

slice

Efficiency study

Gobal efficiencyTelescope+slicer+spectrograph

Page 13: Spectrometer  simulation

A. Ealet Berkeley, december 2002 13

R=/pixel

Simulation checking: spectral resolution

Page 14: Spectrometer  simulation

A. Ealet Berkeley, december 2002 14

➢ DESIGN OPTIMISATION➢ Test optic➢ Play with optic to study tolerance➢ Efficiency/nb of pixel ➢ Visible/IR efficiency vs spectral resolution/detector➢ optimise spatial resolution => detector noise optimisation➢ Reduce Nb of mirrors : better transmission but may need

more space, more complex optics

● TEST DATA– Slit effect : Position of SN in slice => translation of spectrum;– SN may cover several slices : need to add translated

spectra– Optical distorsions– Pixellization– Dithering– Detector and electronics : efficiency, noise, cosmics ...

Used for :

Page 15: Spectrometer  simulation

A. Ealet Berkeley, december 2002 15

Distorsions on the detector

U s

patia

l dim

ensi

on

V spectral dimension

Detector pixelsdo not coincide with = Cte or x = Cte

20 pixel/slice

Page 16: Spectrometer  simulation

A. Ealet Berkeley, december 2002 16

Full simulation of slicer unit OK

Full simulation of telescope and spectrometer OK

Interpolate for intermediate points using Neural Network technique. OK

library of PSF for a grid of x,y,; under work

From library of PSF+ geometry (x,y,-> detector indices) to be done

Pixellisation : integrate over pixels Add dark current, readout noise etc... Include galaxy

Dithering (spatial, spectral) If useful, we may use general purpose code developed by CRAL (SNIFS,

SN factory).

Current Status

Page 17: Spectrometer  simulation

A. Ealet Berkeley, december 2002 17

● Detailed simulation of the spectrometer is needed in this phase to quantify performances

● CPU intensive : not appropriate for physics

simulation ● Parametric simulation under development, based on

the library of PSF should be appropriate for a full SNAP simulation (not for SNAPfast).

Conclusion

Page 18: Spectrometer  simulation

A. Ealet Berkeley, december 2002 18

Spectrograph: Performances

telescope

Relay optics

Slicer

Optic straylight diffra.

Spectro

Mirrors prism dichroic

Detector

Vis / NIR

#elements

4 1 3 1 1 2 1 1 1 1

Efficiency/ 0.98 0.98 0.98 0.99 0.95 0.98 0.81 0.95 0.9

0.6

(0.8)

cumulative 0.92 0.90 0.85 0.84 0.80 0.77 0.62 0.59 0.53

0.35

(0.47)

Gain on mirror transmission, loose on diffraction/prism (complete simulation)Globally equivalent

Page 19: Spectrometer  simulation

A. Ealet Berkeley, december 2002 19

Design issues

•Spectral resolution : optimization visible /IR( R(IR [1-1.4] m) < 100 but don’t need to join the 2 detectors )

•Polarization: specification needed – impact on spectrograph•Design

•Spatial resolution : 0.15”. Issue vs the radiation rate

•Wavelength range 1.7 m short for the Si line , 1.8 mm betterbut detector cut issue , issue on temperature