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Lensed CMB power spectra from all-sky correlation functions(5)

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Weak lensing of the CMB changes the unlensed temperature anisotropy and polarization power spectra. Accounting for the lensing effect will be crucial to obtain accurate parameter constraints from sensitive CMB observations. Methods for computing the lensed

4

whereJn(x)isaBesselfunctionofordern.Notethatthetrace-freetermisanalyticatr=0duetothesmall-rbehaviourofJ2(lr).FollowingRef.[1],letusdenote α(x)·α(x′) byCgl(r)sothat

Cgl(r)=

1

sothat

αi(x)αj(x′) =

1

dll3ClψJ2(lr),

(13)

ClΘeil·r eil·[α(x) α(x)] ,2(2π)

(15)

wherewehaveassumedthattheCMBandlensingpotentialareindependent(i.e.weareneglectingthelargescale

correlationthatarisesfromtheintegrated-Sachs-Wolfee ectandhasonlyatinye ectonthelensedCMB).SinceweareassumingαisaGaussian eld,l·[α(x) α(x′)]isaGaussianvariateandtheexpectationvalueinEq.(15)reducesto

′1

eil·[α(x) α(x)] =exp

l2[σ2(r)+cos2(φl φr)Cgl,2(r)],(16)2wherewehaveusedliljr ir j =l2cos2(φl φr)/2andde nedσ2(r)≡Cgl(0) Cgl(r).Here,e.g.φlistheanglebetweenlandthex-axis.Thecos2(φl φr)terminEq.(16)isdi culttohandleanalytically.Instead,weexpandtheexponentialandintegratetermbyterm.ExpandingtosecondorderinCgl,2,we nd

1122 (r)=l4Cgll4Cgl(17)ξ,2(r)J0(lr)+,2(r)J4(lr).1616Expandingtothisorderissu cienttogetthelensedpowerspectrumtosecondorderinClψ;higherordertermsin

Cgl,2onlycontributeattheO(10 4)levelonthescalesofinterest.Notethattheexp( l2σ2/2)termiseasilyhandledwithoutresortingtoaperturbativeexpansioninClψ.Sinceσ2issigni cantlylessthanCgl,2(asshowninFig.2),theperturbativeexpansioninCgl,2convergesmuchfasterthanoneinσ2.Equation(17)extendstheresultofRef.[1]tosecondorderinCgl,2.

1.

Polarization

Thepolarizationcalculationisalsostraightforwardinthe at-skylimit[14].Weusethespin 2polarizationP≡Q+iU,whereQandUaretheStokes’parametersmeasuredwithrespecttothe xedbasiscomposedofthexand yaxes.ExpandingP(x)intermsoftheFouriertransformsofitselectric(E)andmagnetic(B)parts,wehave

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