gong-bo zhao icg, portsmouth may, 2010 play with camb/cosmomc
TRANSCRIPT
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Gong-Bo ZhaoICG, Portsmouth
May, 2010
Play with CAMB/CosmoMC
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Why CAMB/CosmoMC?
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Very efficientWell-structured (modulised) -- easy to
tweak and hackWell-supported – cosmocoffee.infoPopular – mainstream numeric tool in
cosmology
ICG PhD lectures May, 2010
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This 4.5-hr course is to …
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Show you how to run CAMB/CosmoMCLink CAMB equations to Ma&Bertschinger ‘96
Show several useful examples of hacking CAMB -- dynamical dark energy, modified gravity
Guide you how to modify CAMB/CosmoMC for your own research purpose
Show you useful numerical tricks extensively used in CAMB
ICG PhD lectures May, 2010
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This course is not on …
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Theory (see Kazuya, Rob and Cyril’s lectures)Fortran programming (See Numerical Recipe)
ICG PhD lectures May, 2010
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Warming-ups
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Download, compile and run CAMBcamb.infomake clean; make all./camb params.ini
Change model parameters in params.ini and make CMB, P(k) plots change cosmo. paramsadd neutrinosdo CMB lensingdo vector and tensor modescompare with Wayne Hu’s plots athttp://background.uchicago.edu/~whu/metaanim.html
ICG PhD lectures May, 2010
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Analyze the code using “understand for fortran”
http://www.scitools.com/download/(choose the free 15-day trial version)
Look into the code…
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Structure of CAMB
Messy? Not really!!
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Structure of CAMB
preparation
core
output results
8 ICG PhD lectures May, 2010
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Structure of CAMB_GetResults
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Structure of CMBmain
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Structure of CMBmain
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CAMB language A,B,C
12€
Background : grho = 8πGρa2, adotoa =a'
a=
da /dτ
a, tau = conformal time
δT μν : dgrho = 8πGa2 ρ i
i
∑ δi, dgq = 8πGa2 (ρ i
i
∑ + pi)v i
clxc = δc, clxb = δb, clxq = δDE
δGμν : etak = ηk, z = h' /(2k), sigma =h'+6η '
2k
ICG PhD lectures May, 2010
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CAMB vs. M+B ’96 astro-ph/9506072
€
η'k = dgq/2 η 'k 2 = 4πGa2(ρ + P )θ
clxcdot = − kz δ 'c = −1
2h'
z = (0.5dgrho/k +ηk)/adotoa k 2η −1
2
a'
ah' = 4πGa2δT0
0
sigma = z +1.5dgq/k 2 σ =h'+6η '
2k
Differential equations to evolve in CAMBDifferential equations to evolve in CAMB
Constraint equations (algebraic)Constraint equations (algebraic)
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Hacking 1: Dynamical DE
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Task: Default CAMB only works for constant w.
Modify it to implement the CPL parametrisa-tion, i.e. w(a)=w0+wa(1-a)
and calculate the luminosity distance, CMB and P(k) for a model of {-1.5, +(-)0.4}. Compare your spectra with that of the LCDM model.
ICG PhD lectures May, 2010
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Start the game!
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Spot the dark energy stuff in CAMBWe need w(a), dw/da, Int {[1+w(a)]dlna} Files to hack: equations.f90, inidriver.F90Subroutine/functions to hack: dtauda, fderivs, outputChange the background and the DE perturbation equations!!
ICG PhD lectures May, 2010
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Background evolution
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For constant w (default CAMB) grhoa2=grhoa2+grhov*a2**2For functional w (hacked) grhoa2=grhoa2+grhov*Funcofw(a,..)*a2
€
ρX = ρ X0 exp{−3
1
a
∫ [1+ w(a')]d ln a'}
ICG PhD lectures May, 2010
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function Funcofw(a,deriv) implicit none real(dl) a, Funcofw, a0 real(dl) w0, wa integer deriv if (a .lt. 1.d-8) then a0 = 1.d-8 else a0 = a end if
if (deriv==0) then Funcofw = w0+wa*(1.d0-a0) else if (deriv ==1) then Funcofw = -wa*a0 else if (deriv ==2) then Funcofw = a0**(2.d0 - 3.d0*(1.d0+w0+wa))*exp(3.d0*wa*(a0-1.d0)) end if end function Funcofw
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Output
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In inidriver.F90
open(unit=50,file=‘dL_SN.dat’) do i=1, 1000 zz(i)=1.7d0+dble(i-1)/dble(1000-1) write(50,'(100e15.6)') zz(i),
5*log10((1+zz(i)) & **2*AngularDiameterDistance(zz(i)))+25 end doclose(50)
ICG PhD lectures May, 2010
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DE perturbation equations
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ayprime(EV%w_ix)= -3*adotoa*(cs2_lam-Funcofw(a,0))*(clxq+3*adotoa*& (1+Funcofw(a,0))*vq/k) -(1+Funcofw(a,0))*k*vq -& (1+Funcofw(a,0))*k*z -3*adotoa*adotoa*Funcofw(a,1)*vq/k
ayprime(EV%w_ix+1) = -adotoa*(1-3*cs2_lam)*vq + k*cs2_lam*clxq/(1+Funcofw(a,0))
ICG PhD lectures May, 2010
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Output Dark Energy perturbation DE(), vDE() at k=10-3 Mpc-1
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Note that in CAMB language DE = y(EV%w_ix) vDE = y(EV%w_ix+1)
Uncomment the stuff in cmbmain.f90,
EV%q=1.d-3; EV%q2=EV%q**2 tol1=tol/exp(AccuracyBoost-1) do j=1,6000 tauend = taustart * exp(j/6000._dl*log(CP%tau0/taustart)) call
GaugeInterface_EvolveScal(EV,tau,y,tauend,tol1,ind,c,w) write (*,’(4E15.5)') tauend,1/y(1)-1, y(EV%w_ix) ,y(EV
%w_ix+1) end do stop
ICG PhD lectures May, 2010
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Weller and Lewis, 2003
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Singularity?!
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Output CMB Cl’s for the model w0=-1.5, wa=+1.0 to see what happens.
This singularity stems from the fact that w crosses -1. Technically, it’s due to the term of dw/dz/(1+w).
No-Go Theorem: The w for single fluid (scalar field) cannot cross -1 in GR! For proof, see Appendix of astro-ph/0703202.
Solution: astro-ph/0507482 (quintom scenario),
or arXiv:0808.3125 (PPF implementation) ICG PhD lectures May, 2010
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Generalize our hacked code to make it work for an
arbitrary w(z).
One further step?
Leave it to you guys to play with it for fun!!
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Hacking 2: TO BE OR NOT TO BE ??-- MODIFY CAMB TO WORK IN MODIFIED GRAVITY
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Task
Default CAMB only works in GR. Modify it to implement MG. Reproduce the plots on my website.
http://userweb.port.ac.uk/~zhaog/MGCAMB.html
ICG PhD lectures May, 2010
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Universe is Accelerating
Scalar-tensor gravity(e.g. Chameleon, f(R)…)
DGP, Degravitation
…
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Dark Matter
Atoms
€
Λ ?!
Indistinguishable at the background levelNeed to study the structure growth to break the degeneracy
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Linear perturbation in FRW universe
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General RelativityModified Gravity
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What to do technically?
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Given (a,k) and (a,k)we need to solve
k2(a,k) 4G a2(a,k)
in the synchronous gauge, which is used in CAMB.Note that
ICG PhD lectures May, 2010
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So we have
Finally, we have (for details, see Appendix of 0809.3791),
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Note that in default CAMB, overdensity for different speciesand metric perturbation in synchronous gauge are actually evolved, and other Einstein equations are used as constraint equations (see this slide).
In MG, we need to evolve and and get from constraint equations.
To add one more variable to evolve in CAMB, we need to define it, set initial condition for it, and change fderivs and output properly.
See how to modify the code in the lecture.
ICG PhD lectures May, 2010
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€
μ(a,k) =1+ α 1k
2as
1+ α 2k2as
, γ(a,k) =1+ β1k
2as
1+ β 2k2as
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Fit your own parameters using CosmoMC
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CosmoMC fits your model parameters to data by exploring the parameter space in a smart way (Metropolis-Hastings algorithm). It calls CAMB to calculate the theoretical spectra of a model, and compare to data.
ICG PhD lectures May, 2010
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How to add your own parameter to CosmoMC?
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Tell CosmoMC your parameters’ names in CMB_Cls_simple.f90
Define them in cmbtype.f90Map them in params_CMB.f90Change the # of parameters in settings.f90Done!!See the example in the lecture!!
ICG PhD lectures May, 2010
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Astro-ph/0511625
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Useful references
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Camb.info; cosmologist.info/cosmomc/Cosmocoffee.infoM+B: astro-ph/9506072Jussi’s ICG lectures: www.icg.port.ac.uk/~valiviij/Numerical Recipe: www.nr.comPlotting software: OriginPro, Matlab, IDL, gnuplot
ICG PhD lectures May, 2010
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Have fun!!
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