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PISCO Redshifts: SimulationsPowerPoint Presentation

PISCO Redshifts: Simulations

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### PISCO Bandpasses Glassat the Focal Planes

The LPPC Contingent

Chris Stubbs

(Harvard Physics, Astronomy)

Tony Stark

(SAO)

James Battat

(Harvard Astronomy)

Passbands

Will High

(Harvard Physics)

Photometric redshifts

The Problem

- Measure the distance to as many galaxy clusters as possible, as efficiently as possible
- Redshift == distance given knowledge (read: assumptions) of geometry of universe

- Solution already exists:
- The photometric redshift principle: Use
- broadband, differential photometry
- presumed knowledge of convenient source spectra
- and knowledge of filter transmission curves

- … to arrive at redshifts z to |dz| < 0.1
- Spectra of Luminous Red Galaxies increase ~monotonically in well understood way… 4000A break

- The photometric redshift principle: Use
- Our problem: we know our filters’ bandwidths and central wavelengths change as a function of field position! How does this affect redshift recovery?
- Our tool: simulated observations of LRGs using expected filter curves

Rule of thumb: Glass

Dichroics pass red

No Photons Here! Glass

No Photons Here! Glass

Multiply those curves appropriately

With CCD Quantum Efficiency Glass

- Not yet accounted for:
- Glass & other optics
- Atmosphere
- Possible y band at 1 micron

Multiply by MIT/LL high resistivity CCD transmission curves

Transmission

r

i

g

z

Wavelength (Angstrom)

Dichroic Info Glass

- Company: Barr Associates
- Cost:
- BS I $12k
- BS II $11k
- BS III $11k

- Delivery: 12-14 weeks (including substrate procurement time of 8-10 weeks)
- Barr can make effective index of refraction as high as 2.0 to minimize the effect of angle of incidence on the transmission/reflection properties (see next slide)

CWL = cut-on wavelength Glass

Ratio of cwl at some angle to cwl at 0 degrees.

Increasing n (the effective index of refraction) decreases the effect of AOI (shallower slope)

Position Dependence Glass

- Dichroics in highly collimated beam
- Angle at dichroic → position in focal plane
- But different angles have different cut-on wavelengths! Therefore…

- Bandpasses depend on position in focal plane
- Effective wavelength λeff changes
- Bandwidth changes
- Both ill behaved across field

- Study how well we recover redshift assuming
- Naïve bandpasses = transmission at center of field, assumed to hold everywhere
- Correct bandpasses = true transmission, which changes with field position

How We Measure Redshift Glass

- Observe redshifted Luminous Red Galaxy (LRG) spectrum with correct bandpasses
- Estimate AB mags using naïve and correct bandpasses
- Fit colors: LRG color ↔ LRG redshift
- kcorrect
- Use both naïve and correct bandpasses

true LRG

observed

Photon Flux Density

r

i

g

z

Wavelength (Angstrom)

We Measure Photo-z’s: GlassNaïve

z in = 0.4

z out = 0.438

z in = 0.8

z out = 0.835

Black = output spectrum

z in = 1.1

z out = 1.174

z in = 1.4

z out = 1.412

r

i

Gray = input spectrum

z

g

We Measure Photo-z’s: GlassCorrect

z in = 0.4

z out = 0.403

z in = 0.8

z out = 0.804

Black = output spectrum

z in = 1.1

z out = 1.128

z in = 1.4

z out = 1.408

r

i

Gray = input spectrum

z

g

Photo-z Errors: GlassNaïve

Underestimated

z in = 0.4

err = 3.9e-2

z in = 0.8

err = 3.7e-2

Overestimated

z in = 1.1

err = 1.3e-1

z in = 1.4

err = 1.1e-1

Photo-z Errors: GlassCorrect

Underestimated

z in = 0.4

err = 3.1e-3

z in = 0.8

err = 6.2e-3

Overestimated

z in = 1.1

err = 5.0e-2

z in = 1.4

err = 9.5e-2

Worst Photo-z Errors Glass

i → z

g → r

r → i

z → …

Naive passband

photo-z error (max absolute deviation)

Correct passbands

z in

g AB Mag Errors: GlassNaïve

Brighter

z in = 0.4

err = 8.3e-2

z in = 0.8

err = 1.3e-1

Dimmer

z in = 1.1

err = 1.5e-1

z in = 1.4

err = 8.4e-2

g AB Mag Errors: GlassCorrect

Brighter

z in = 0.4

err = 4.4e-2

z in = 0.8

err = 8.8e-2

Dimmer

z in = 1.1

err = 1.0e-1

z in = 1.4

err = 4.0e-2

Worst g AB Mag Errors Glass

i → z

g → r

r → i

z → …

g AB mag error (max absolute deviation)

Naive passband

Correct passbands

z in

g – r Color Errors: GlassNaïve

Bluer

z in = 0.4

err = 3.7e-2

z in = 0.8

err = 8.9e-2

Redder

z in = 1.1

err = 5.8e-2

z in = 1.4

err = 5.7e-2

g – r Color Errors: GlassCorrect

Bluer

z in = 0.4

err = 1.2e-2

z in = 0.8

err = 4.9e-2

Redder

z in = 1.1

err = 2.8e-2

z in = 1.4

err = 8.8e-2

Worst g – r Color Errors Glass

i → z

g → r

r → i

z → …

g – r error (max absolute deviation)

Naive passband

Correct passbands

z in

g – i Color Errors: GlassNaïve

Bluer

z in = 0.4

err = 1.3e-1

z in = 0.8

err = 1.4e-1

Redder

z in = 1.1

err = 1.8e-1

z in = 1.4

err = 9.3e-2

g – i Color Errors: GlassCorrect

Bluer

z in = 0.4

err = 3.8e-2

z in = 0.8

err = 4.9e-2

Redder

z in = 1.1

err = 9.4e-2

z in = 1.4

err = 3.6e-2

Worst g – i Color Errors Glass

i → z

g → r

r → i

z → …

g – i error (max absolute deviation)

Naive passband

Correct passbands

z in

Worst Color Errors Glass

NOTE THE SCATTER

Naive passband

g – r error

Correct passband

Wake et al, 2006

astro-ph/0607629

z in

What’s Next? Glass

- Add y band? 1 micron, a la Pan-STARRS
- Increase sophistication of photo-z module
- More templates
- Priors

Summary Glass

- PISCO achieves broad optical bandpasses in an original way that is more efficient
- Downside: bandpasses become weakly position dependent
- Outlook for photo-z’s:
- Hurts us most at z < 1.0, but in a clean way
- At z > 1.0, 4000A break leaving bands, situation messier
- Incorporate these facts into analysis (= calibrate)

- Contact Will at [email protected]

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