Software Modelling of IFU Spectrometers

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Alistair C. H. Glasse, Gillian S. Wright (UK ATC, JWST-MIRI),. Suzanne Ramsay ... ADASS XVII - September, 2007. 3. Why do we need instrument simulators?
Software Modelling of IFU Spectrometers Nuria P. F. Lorente UK Astronomy Technology Centre Royal Observatory, Edinburgh, UK

Alistair C. H. Glasse, Gillian S. Wright (UK ATC, JWST-MIRI), Suzanne Ramsay Howat (UK ATC, KMOS), Chris J. Evans (UK ATC, EELT)

1 ADASS XVII - September, 2007

Why do we need instrument simulators?

2 ADASS XVII - September, 2007

Why do we need instrument simulators? z

Increasing scale and complexity of telescopes and instruments with time

3 ADASS XVII - September, 2007

Why do we need instrument simulators? z z

Increasing scale and complexity of telescopes and instruments with time We need to know how design and construction changes may potentially affect the science we can do with the instrument

4 ADASS XVII - September, 2007

Why do we need instrument simulators? z z

z

Increasing scale and complexity of telescopes and instruments with time We need to know how design and construction changes may potentially affect the science we can do with the instrument Development of data reduction and analysis software requires test data

5 ADASS XVII - September, 2007

Why do we need instrument simulators? z z

z z

Increasing scale and complexity of telescopes and instruments with time We need to know how design and construction changes may potentially affect the science we can do with the instrument Development of data reduction and analysis software requires test data An understanding of the data products will help in designing effective calibration strategies

6 ADASS XVII - September, 2007

Why do we need instrument simulators? z z

z z z

Increasing scale and complexity of telescopes and instruments with time We need to know how design and construction changes may potentially affect the science we can do with the instrument Development of data reduction and analysis software requires test data An understanding of the data products will help in designing effective calibration strategies Synthetic data products are an effective communication tool in a distributed scientific and engineering environment

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JWST-MIRI MRS

• Launch in 2013 • Positioned at L2 • 4 instruments on board

8 ADASS XVII - September, 2007

JWST-MIRI MRS • Collaborative project between • Consortium of 21 institutes under ESA • NASA • Imager, coronograph, low-resolution spectrometer, IFU medium resolution spectrometer

• Launch in 2013 • Positioned at L2 • 4 instruments on board

9 ADASS XVII - September, 2007

JWST-MIRI MRS • 4 spectral channels (5 – 28 microns) • FoV 3.70x3.70arcsec – 7.74x7.93 arcsec • Spectral resolution ~3000

• One IFU slicer per channel • All channels are observed simmultaneously • Dichroic filters divide each IFU channel into 3 subbands • Data from pairs of channels are captured on two 1024x1024 pixel detectors • Expected sensitivity 1.21e-20 Wm^-2, 6.4microns, 5.610e-20 W^m-2 at 22.5 microns

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Specsim: Modelling the Field of View Specsim GUI

11 ADASS XVII - September, 2007

Specsim: Modelling the Field of View Specsim GUI

Sky Background

12 ADASS XVII - September, 2007

Specsim: Modelling the Field of View Specsim GUI

Targets

Sky Background

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Specsim: Modelling the Field of View Specsim GUI

Targets

Sky Background

14 ADASS XVII - September, 2007

Specsim: Modelling the Field of View Specsim GUI

Targets

Sky Background

15 ADASS XVII - September, 2007

Specsim: Modelling the Field of View Specsim GUI

Targets

Sky Background Sky Model

16 ADASS XVII - September, 2007

Specsim: Modelling the IFU Spectrometer

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Specsim: Modelling the IFU Spectrometer

Transmission Function Definitions 18 ADASS XVII - September, 2007

Specsim: Modelling the IFU Spectrometer

Transmission Function Definitions 19 ADASS XVII - September, 2007

Specsim: Modelling the IFU Spectrometer

Cosmic Rays Noise Exposure Length

Transmission Function Definitions 20 ADASS XVII - September, 2007

Specsim: Modelling the IFU Spectrometer

Cosmic Rays Noise Exposure Length

Transmission Function Definitions 21 ADASS XVII - September, 2007

JWST-MIRI MRS Modelling Observations of a YSO

(Glasse et al., in prep. 2007) 22 ADASS XVII - September, 2007

JWST-MIRI MRS Modelling Observations of a YSO

Spitzer IRS spectrometer (Lahuis et al., 2006)

(Glasse et al., in prep. 2007) 23 ADASS XVII - September, 2007

JWST-MIRI MRS Modelling Observations of a YSO

Spitzer IRS spectrometer (Lahuis et al., 2006)

"IRS46 at 875 pc" N_TARGETS 1 { "Dither_A" 0 0.485 1.01 N_CONT 2 0 0.015 700.0 0 0.002 160.0 N_BROAD 2 0 -0.001 15.2 0.30 1 -0.014 N_NARROW 360 12.02300 -0.245 “NL1" 12.03510 -0.023 “NL2" ... }

ADASS XVII - September, 2007

(Glasse et al., in prep. 2007) 24

JWST-MIRI MRS Modelling Observations of a YSO

Spitzer IRS spectrometer (Lahuis et al., 2006) Point source

CO2 Gaussian absorption feature, and silicate spectrum

"IRS46 at 875 pc" N_TARGETS 1 { "Dither_A" 0 0.485 1.01 N_CONT 2 0 0.015 700.0 0 0.002 160.0 N_BROAD 2 0 -0.001 15.2 0.30 1 -0.014 N_NARROW 360 12.02300 -0.245 “NL1" 12.03510 -0.023 “NL2" ... }

ADASS XVII - September, 2007

Black-body continuum

360 narrow absorption lines (HCN etc.) (Glasse et al., in prep. 2007) 25

JWST-MIRI MRS Modelling Observations of a YSO

Spitzer IRS spectrometer (Lahuis et al., 2006) Point source

CO2 Gaussian absorption feature, and silicate spectrum

"IRS46 at 875 pc" N_TARGETS 1 { "Dither_A" 0 0.485 1.01 N_CONT 2 0 0.015 700.0 0 0.002 160.0 N_BROAD 2 0 -0.001 15.2 0.30 1 -0.014 N_NARROW 360 12.02300 -0.245 “NL1" 12.03510 -0.023 “NL2" ... }

Specsim synthetic spectrum

ADASS XVII - September, 2007

Black-body continuum

360 narrow absorption lines (HCN etc.) (Glasse et al., in prep. 2007) 26

JWST-MIRI MRS Modelling Observations of a YSO

1B 3B

4B

2B

Simulated detector image

Simulated white-light images

(Glasse et al., in prep. 2007) 27 ADASS XVII - September, 2007

VLT - KMOS

• NIR multi-object IFU spectrometer • 3 identical channels • 8 IFUs per channel • 14 slices of 14 pixels per IFU • 3 spectrographs • 2048 x 2048 pixel detector images

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VLT - KMOS “Emission line galaxy with 3 lines” N_TARGETS

1

{ “Galaxy continuum” 1

0.0 0.0 2.0 0.6 50

N_CONT 0

1

0.000003 2500.0

N_BROAD

0

N_NARROW 0 } “Emission line – different extent” 1

0.0 0.0 2.0 1.0 140.0

N_CONT

0

N_BROAD

0

N_NARROW 3 1.1 90.0

“Line1”

1.7 60.0

“Line2”

2.2 100.0

“Line3”

}

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VLT - KMOS

• White-light image of the galaxy

• Portion of the detector image • Note the spectral line and the galaxy continuum • Image of the galaxy at the wavelength of the emission line

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E-ELT

Investigating the effect of adaptive optics on image quality

Simulated field of view 31 ADASS XVII - September, 2007

E-ELT

Investigating the effect of adaptive optics on image quality

Seeing-limited PSF

Simulated field of view 32 ADASS XVII - September, 2007

E-ELT

Investigating the effect of adaptive optics on image quality

Seeing-limited PSF

Simulated white-light image, with no AO correction ADASS XVII - September, 2007

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E-ELT

Investigating the effect of adaptive optics on image quality

Ground-layer correction PSF

Simulated field of view 34 ADASS XVII - September, 2007

E-ELT

Investigating the effect of adaptive optics on image quality

Ground-layer correction PSF

Simulated white-light image with ground-layer correction ADASS XVII - September, 2007

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E-ELT

Investigating the effect of adaptive optics on image quality

Laser Tomography PSF

Simulated field of view 36 ADASS XVII - September, 2007

E-ELT

Investigating the effect of adaptive optics on image quality

Laser Tomography PSF

Simulated white-light image with laser-tomography correction ADASS XVII - September, 2007

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E-ELT

Investigating the effect of adaptive optics on image quality

• Seeing-limited field

• Ground layer correction only

• Laser-tomography 38 ADASS XVII - September, 2007