sz power spectrum from self- consistent x-ray...

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SZ power spectrum from self- consistent X-ray analysis Pierre Delsart * , Domingos Barbosa°, Alain Blanchard * * IRAP - Toulouse, France ° Instituto de Telecomunicaçoes - Aveiro, Portugal [email protected] 17/02/2012 - Planck 2012 Conference

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Page 1: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

SZ power spectrum from self-consistent X-ray analysis

Pierre Delsart*, Domingos Barbosa°, Alain Blanchard*

* IRAP - Toulouse, France

° Instituto de Telecomunicaçoes - Aveiro, Portugal

[email protected]

17/02/2012 - Planck 2012 Conference

Page 2: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

Outline

X-ray results

Modelling of SZ contribution

Results on SZ power spectrum

Conclusion

2

Page 3: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

Population very sensitive to the mass & growth factor

Modeling by mass function (Press & Schechter 1974)

Need mass Mv =4π

3R3

v!ρ

Dependent of the cosmology (Ωm,σ8...)

N(M) =!

Mf(")

d#

dM

X-ray resultsMotivation

3

Page 4: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

4

The temperature function

From the mass function

From the observations

N(> kBT ) =!

kTi>kT

1

V (kTi)

!2(> kBT ) =!

Ti>T

1

V 2(kBT )

N(> kBT ) =

! +!

M(T )N(m)dm

X-ray results

Page 5: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

X-ray resultsThe samples

(see http://bax.ast.obs-mip.fr, Vikhlinin et al.2009, Ebeling et al.2007, Ebeling et al.2010)

Page 6: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

X-ray results

T = ATM (hMv)2/3

!!m

"(!m, z)

178

"1/3

(1 + z) (1 + z)!

6

Page 7: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

Using all samples

SMT

Tinker

7

X-ray results

(Delsart & Blanchard, in prep.)

Page 8: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Modelling of SZ contribution

Cl = f(x)2! zmax

0dz

dV

dzdΩ

! Mmax

Mmin

dMdN(M, z)

dM|yl(M, z)|2

yl !! +!

0T (r)ne(r)

sin(lr/DA)

lr/DAr2dr

Need gas profil

Use of a scaling relation T-M

Page 9: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Modelling of SZ contributionGas profil and scaling law

Simple β-model β=0.8

Exponential cut in radius

! exp

("r2

r2v

).

ξ = 0.6withTgas = !TX

Page 10: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Modelling of SZ contribution

Reichard et al.2009

Das et al.2010

Keissler et al.2011Reichard et al.2011

Page 11: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Results on the SZ power spectrumDependency on cosmological parameters

Keep the self-consistency with X-ray

Page 12: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Results on the SZ power spectrumDependency on scaling law and gas profil parameters

Effect of redshift evolution

Page 13: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Results on the SZ power spectrumSZ flux cut-off

(see Delsart et al., A&A 2010, 524, A81)

Y ! !ATMfBM5/3v h8/3

!!m

"

178

"(1 + z)1+!D!2

Page 14: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Results on the SZ power spectrumTotal CMB power spectrum

(Delsart, Barbosa & Blanchard, in prep.)

Page 15: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

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Conclusion

Strongly dependant of gas profil parameters

Evolution is one of possible solution to explain decrement in the SZ part

X-ray observations suggest evolution in T-M

Evolution measured and constrained

Errors on the modelling due to cosmological parameters are reasonable

Page 16: SZ power spectrum from self- consistent X-ray analysisevents.iasfbo.inaf.it/planck-2012/talks/con/Delsart_talk_Planck...° Instituto de Telecomunicaçoes - Aveiro, Portugal pierre.delsart@irap.omp.eu

Thank you for your attention