Weak Lensing Tomography Sarah Bridle University College London.
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Transcript of Weak Lensing Tomography Sarah Bridle University College London.
- Slide 1
- Weak Lensing Tomography Sarah Bridle University College London
- Slide 2
- 3d vs 2d (tomography) Non-Gaussian -> higher order statistics Low redshift -> dark energy versus
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- Weak Lensing Tomography 1.In principle (perfect zs) Hu 1999 astro-ph/9904153 2.Photometric redshifts Csabai et al. astro-ph/0211080 3.Effect of photometric redshift uncertainties Ma, Hu & Huterer astro-ph/0506614 4.Intrinsic alignments 5.Shear calibration
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- 1. In principle (perfect zs) Qualitative overview Lensing efficiency and power spectrum Dependence on cosmology Power spectrum uncertainties Cosmological parameter constraints
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- 1. In principle (perfect zs) Core reference Hu 1999 astro-ph/9904153 See also Refregier et al astro-ph/0304419 Takada & Jain astro-ph/0310125
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- Cosmic shear two point tomography
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- (Hu 1999)
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- Lensing efficiency (Hu 1999) Equivalently: g i (z l ) = z l n i (z s ) D l D ls / D s dz s i.e. g is just the weighted D l D ls / D s
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- Can you sketch g 1 (z) and g 2 (z)? (Hu 1999) g i (z) = z s n i (z s ) D l D ls / D s dz s
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- Lensing efficiency for source plane?
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- (Hu 1999)
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- Sensitivity in each z bin
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- NOT
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- (Hu 1999) Why is g for bin 2 higher? A. More structure along line of sight B. Distances are larger g i (z d ) = z s 1 n i (z s ) D d D ds / D s dz s
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- * *
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- Lensing power spectrum (Hu 1999)
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- Lensing power spectrum Equivalently: P ii (l) = g i (z l ) 2 P(l/D l,z) dD l /D l 2 i.e. matter power spectrum at each z, weighted by square of lensing efficiency (Hu 1999)
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- Measurement uncertainties 1/2 = rms shear (intrinsic + photon noise) n i = number of galaxies per steradian in bin i (Hu 1999) Cosmic Variance Observational noise
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- (Hu 1999)
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- Sensitivity in each z bin
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- NOT
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- (Hu 1999)
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- Dependence on cosmology Refregier et al SNAP3 ?? A. m = 0.35 w=-1 B. m = 0.30 w=-0.7
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- Approximate dependence Increase 8 A. P B. P Increase z s A. P B. P Increase m A. P B. P Increase DE ( K =0) A. P B. P Increase w A. P B. P Huterer et al
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- Effect of increasing w on P Distance to z A. Decreases B. Increases
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- Perlmutter et al.1998 Fainter Further away Decelerating Accelerating m =1, no DE m =1, DE =0) == ( m = 0.3, DE = 0.7, w DE =0)
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- Perlmutter et al.1998 EdS OR w=0 w=-1 Fainter, further Brighter, closer
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- Effect of increasing w on P Distance to z A. Decreases B. Increases When decrease distance, lensing effect decreases Dark energy dominates A. Earlier B. Later
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- Effect of increasing w on P Distance to z A. Decreases B. Increases When decrease distance, lensing decreases Dark energy dominates A. Earlier B. Later Growth of structure A. Suppressed B. Increased Lensing A. Increases B. Decreases Net effects: Partial cancellation decreased sensitivity Distance wins
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- Approximate dependence Increase 8 A. P B. P Increase z s A. P B. P Increase m A. P B. P Increase DE ( K =0) A. P B. P Increase w A. P B. P Huterer et al
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- Approximate dependence Increase 8 A. P B. P Increase z s A. P B. P Increase m A. P B. P Increase DE ( K =0) A. P B. P Increase w A. P B. P Huterer et al Note modulus
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- Which is more important? Distance or growth? Simpson & Bridle
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- Dependence on cosmology Refregier et al SNAP3 ?? A. m = 0.35 w=-1 B. m = 0.30 w=-0.7
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- (Hu 1999)
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- See Heavens astro-ph/0304151 for full 3D treatment (~infinite # bins)
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- (Hu 1999)
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- Parameter estimation for z~2 (Hu 1999)
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- Predict the direction of degeneracy in w versus m plane
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- Refregier et al SNAP3
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- (Hu 1999)
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- Takada & Jain
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- (Hu 1999)
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- Covariance matrix P 12 is correlated with P 11 and P 22 (ignoring trispectrum contributions) Takada & Jain
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- How many redshift bins to use? Ma, Hu & Huterer 5 is enough Modified from
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- Higher order statistics
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- Takada & Jain
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- Geometric information Jain & Taylor; Kitching et al. Slide stolen from Tom Kitching www.astro.dur.ac.uk/Cosmology/SISCO/edin_talks/Kitching.PPT
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- Slide stolen from presentation by Andy Taylor www.shef.ac.uk/physics/idm2004/talks/monday/originals/taylor_andy.ppt
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- Slide stolen from presentation by Andy Taylor www.shef.ac.uk/physics/idm2004/talks/monday/originals/taylor_andy.ppt
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- Slide stolen from presentation by Andy Taylor www.shef.ac.uk/physics/idm2004/talks/monday/originals/taylor_andy.ppt
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- Slide stolen from presentation by Andy Taylor www.shef.ac.uk/physics/idm2004/talks/monday/originals/taylor_andy.ppt
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- Some additional tomographic methods Cross-correlation cosmography Bernstein & Jain astro-ph/0309332 Galaxy-lensing cross correlation Hu & Jain astro-ph/0312395 Reconstruction of distance and growth Song; Knox & Song