Title: Simulating Gravitational Lensing of the CMB
1Simulating Gravitational Lensing of the CMB
Sudeep Das with David Spergel, Paul Bode and
Chris Hirata
Princeton University
June 8, 2007
2Outline
- Why is CMB Lensing interesting?
- Some basics
- Why large sky?
- The simulation
- Results
- Future directions
3Why interesting? Some basics Why
curved sky? Simulation
Future directions
The three Rs of the CMB
Redshift Remoteness Randomness
4Why interesting? Some basics Why
curved sky? Simulation
Future directions
The three Rs of the CMB
A source at a well known Redshift.
- For lensing of the CMB the source redshift is
accurately known. - One of the main uncertainties in conventional
weak lensing studies is the lack of accuracy in
source redshifts.
5Why interesting? Some basics Why
curved sky? Simulation
Future directions
The three Rs of the CMB
A source which is most Remote.
- CMB can act as a source for lensing by high
redshift objects. - Lensing of the CMB by quasars and sub-mm
galaxies have the potential of telling us about
the less understood halo properties of these
objects.
6Why interesting? Some basics Why
curved sky? Simulation
Future directions
The three Rs of the CMB
A source which is Random.
- The hot and cold patches of the CMB are
featureless. They have no intrinsic shape. - In conventional weak lensing with galaxies,
their intrinsic ellipticity is a source of
systematic noise.
7Why interesting? Some basics Why
curved sky? Simulation
Future directions
Detectable
3.4 ? detection with WMAPNVSS. Smith et al.
arXiv0705.3980v1
With upcoming surveys like ACT, PLANCK, SPT the
effect should be detectable at high significance
in cross correlation with large scale structure
tracers.
8Why interesting? Some basics Why
curved sky? Simulation
Future directions
Lensing remaps points
- Typical deflection is non-trivial ( 2.7 arcmin)
- Deflections are coherent over few degrees.
9Why interesting? Some basics Why
curved sky? Simulation
Future directions
Lensing smoothes features
- Power from large scales (l60) in the
deflection field gets aliased into smaller scales
(l1000) in the CMB.
10Why interesting? Some basics Why
curved sky? Simulation
Future directions
Catching all those modes
- A lot of power from large scale modes in the
deflection field - couples to small scale modes in the CMB.
11Why interesting? Some basics Why
curved sky? Simulation
Future directions
Large Scale Structure Simulation
For z lt 4.0
We use a Tree Particle Mesh (TPM) light-cone
simulation. Bode, P., Ostriker, J.P.
2003, ApJS, 145, 1 Lbox 1000 h-1 Mpc N
10243 (mp 6.72 1010Msun /h).
For z gt 4.0
- LSS planes are generated as Gaussian random
realizations from a theoretical power spectrum.
12Why interesting? Some basics Why
curved sky? Simulation
Future directions
Large Scale Structure Cosmology
The cosmological parameters used are ?b
0.044, ?m 0.216, ?? 0.74, h 0.72, n
s 0.95 and ?8 0.77.
13Why interesting? Some basics Why
curved sky? Simulation
Future directions
Large Scale Structure Projection
onto sphere
At each TPM step,
Particles in a z- slice are projected onto the
octant of a HEALpix sphere.
Euler rotated and centroided on the North Pole.
A disc is taken out and the surface mass density
(?) on it saved.
14100 TPM discs are further binned up into 10
planes. Both an effective and a multiple plane
ray tracing are performed.
15Why interesting? Some basics Why
curved sky? Simulation
Future directions
Connecting ??? ?????
Multiple Planes
Effective Approximation
16Why interesting? Some basics Why
curved sky? Simulation
Future directions
Power Spectrum of ?
17Why interesting? Some basics Why
curved sky? Simulation
Future directions
Getting the deflection field ?
The Poisson equation is inverted to get the
lensing potential,
Then the deflection angle, ?r ??is then
calculated as,
18Why interesting? Some basics Why
curved sky? Simulation
Future directions
Remapping points
Given the deflection angle field,
rays are propagated using the curved sky
remapping equations,
Lewis, A. Phys. Rev. D71 (2005) 083008
19Why interesting? Some basics Why
curved sky? Simulation
Future directions
The Need to Interpolate
Rays will end up off-centered on subsequent
slices and on the CMB. Both r ? and TCMB have
to be sampled on an irregular grid.
20Why interesting? Some basics Why
curved sky? Simulation
Future directions
Non-Isolatitude Spherical Harmonic Transform
(NISHT)
Hirata et al., PRD, 70, 103503, (2004).
21Unlensed CMB Gnomonic Projection
NSIDE4096. 0.856 arcmin.
22Lensed CMB Gnomonic Projection
NSIDE4096. 0.856 arcmin.
23Difference Map Gnomonic Projection
NSIDE4096. 0.856 arcmin.
24Why interesting? Some basics Why
curved sky? Simulation
Future directions
Power Spectra
Power Spectra
The theory curves are spectra from CAMB with
mode-coupling due to a tapered polar cap window.
www.camb.info
25Why interesting? Some basics Why
curved sky? Simulation
Future directions
Power Spectra
Power Spectra
Structure at zgt4 has a nontrivial contribution to
the lensed signal.
26Why interesting? Some basics Why
curved sky? Simulation
Future directions
Utility
- Most of the forthcoming surveys will concentrate
on the cross- correlation between gravitational
lensing of the CMB and tracers of large scale. - The current method provides a natural way to
simulate such studies. - The halos can be saved and populated with
tracers (LRGs, SZ clusters etc.) - Optical lensing (galaxy shear) studies can be
simulated with the same LSS and cross correlated
with the lensed CMB.
27Why interesting? Some basics Why
curved sky? Simulation
Future directions
LRG Maps
In collaboration with Charlie Conroy we are
populating the simulation with LRGs with an HOD
based approach. Conroy et. al, Astrophys. J.
647 (2006) 201-214
28Why interesting? Some basics Why
curved sky? Simulation
Future directions
The Atacama Cosmology Telescope.
Achieved first light on June 8, 2007 pointing at
Jupiter.
ACT will be looking at the SDSS stripe 82 where
we have LRG data.
29Why interesting? Some basics Why
curved sky? Simulation
Future directions
Final Words
- Extension to full sky.
- Internally consistent LRG and SZ maps.
- Shear Maps for the same LSS.
- Use them as training sets for detection
algorithms. - Thanks to
- David Spergel (advisor), Paul Bode, Chris Hirata,
Charlie Conroy.
30Why interesting? Some basics Why
curved sky? Simulation
Future directions
NISHT Errors
In the simulation we sample at 4 times the
Nyquist rate and use a Polynomial of order K10.
1e-2
1e-5
Maximum Error in each Fourier Mode
1e-8
LNyquist/LSampling
Hirata et al., PRD, 70, 103503, (2004).