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Sun Lei (孙磊) Peking University
Catastrophic errors of photo-z: biasing dark energy parameter estimates with cosmic shear Sun Lei (孙磊) Peking University Collaborators: Z.-H. Fan, C. Tao, J.-P. Kneib, S. Jouvel, A. Tilquin
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Cosmic Shear Tyson et al 2002
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Cosmic shear and the systematics
powerful ! measure: DA(z) & G(z) bias-free Hu Zhan (06) Knox, Song, & Zhan (06) But systematics control is crucial !! Huterer et al. (06)
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Catastrophic errors Loosely defined: e.g. | z_p - z_s | > 1
LSST without u band SNAP standard filters z_phot Catastrophic error Catastrophic error by A.Conolly by S.Jouvel z_spec Loosely defined: e.g. | z_p - z_s | > 1 Causes: e.g. Lyman break(~1000 A) & Balmer break (~4000 A) confused
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Catastrophic errors seen in a realistic galaxy z-distribution n(z)
Brodwin et al.03 (CFDF) Gavazzi & Soucail 06 (CFHT)
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How do the lensing signals depend on the source galaxy distribution n(z)
bias ! Refregier 2003 n(z) n(z) z
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SNAP : a space-based survey
survey geometry area: 1000 deg² number densigy: 100 gal/arcmin² depth: zmed = 1.26 Its weak lensing design: Employ 5 tomographic z bins: fidicual n(z) of galaxy: with = 2, =1.5
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Lensing tomography: how many redshift bins to use?
wa w0
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SNAP Photo-z simulation results: with its standard 9 filter set
To characterize true n(z) of : fcata=1 % at z_spec ~ 0.4 z_phot ~ 3.5 with zm = 0.4, = 0.1, Acata determined by fcata.
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To estimate the bias on cosmological paramters:
n(z) C for signal ‘S’ ‘Bin-0’: M S for model ‘M’ To estimate the bias on cosmological paramters: Extension of Fisher matrix: Chi-square fitting analysis:
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Biases on dark energy equation of state (w0, wa):
² fitting: Fisher matrix approximation: fiducial values biased values Assume a 7-param fiducial model [m, w0, wa, 8, h, b, n], with a Gaussian priors (pi)=0.05 applied on all hidden params except (b)=0.01.
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To fight against catastrophic failure: spectroscopic calibration
Sampling N spectra out of our simulated 1300 galaxies whose photo-zs fall in z_phot = [3, 4]
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To fight against catastrophic failure: spectroscopic calibration
for signal ‘S’ for model ‘M’ ' M (one realization of calibration) If Nspec is not enough : there is residual fcata = ' , so still bias the parameter estimate!
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To fight against catastrophic failure: spectroscopic calibration
Sampling 100 spectra (with 100 realizations) 5 z-bins with all Cij: 5 z-bins with auto Cii only: wa w0 w0 Scatter of bias is large: significant compared to statistical errors Notable descrepancy between results of fit / Fisher when residual (f – f ‘) is large
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To fight against catastrophic failure: spectroscopic calibration
Sampling 500 spectra (with 100 realizations) 5 z-bins with all Cij: 5 z-bins with auto Cii only: wa w0 w0 Scatter of bias is small: getting insignificant Descrepancy between fit / Fisher is vanishing since residual (f – f ‘) keeps small
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To fight against catastrophic failure: spectroscopic calibration
How many spectra is sufficient ? 2(w0-wa) (w0-wa) A calibration size of spetra at z ~ [3,4] is necessary Might not be easy at such high-z but hopeful
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To fight against catastrophic failure: other methods
including u band : fcata: ~1% ~ 0.1 % But technical difficulty exists…
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To fight against catastrophic failure: other methods
Cutting out galaxies at z < 0.5 & z>2.5 : re-define 5 narrower z-bins consider original 3 z-bins left But with notable statistical loss…
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summary Catastrophic error is frequently seen in photo-z catalogs and is an important source biasing the galaxy z-distribution. The bias induced by catastrophic errors on DE parameter estimate from cosmic shear: SNAP with std-type filters: ~1 % fcata significant compared to statistical error in tomography 5-z bins case To resist the bias by catastrophic errors: * spectroscopic calibration useful, needs a relatively large sample at high-z * Including u band useful, may be not easy for space-based telescope e.g. SNAPu : ~ 0.1% fcata bias much smaller than statistical error * Cutting out galaxies with suspicious z useful, with a price paid for statistical loss
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Thank you!
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