Dust and Lenses in Future Surveys
Árdís Elíasdóttir
Department of Astrophysical Sciences Princeton University
(ardis@astro.princeton.edu)
Strong Gravitational Lensing in the Next Decade
Cogne, Aosta Valley, Italy 25.06.2009
Department of Astrophysical Sciences www.astro.princeton.edu
Outline
• Extinction Curves
• The Lens Perspective
• Future Surveys
EXTINCTION CURVES
“The true harvest of my life is intangible - a little star dust caught, a portion of the rainbow I have clutched”
- Henry David Thoreau (1817-1862)
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Dusty Worlds
• Dust between the stars in galaxies causes the dimming of light from background sources
• Extinction curves measure this
dimming as a function of wavelength
• Traditionally measured by comparing two stars of the same spectral type
• Important for
• Galaxy formation studies
• Dark energy surveys
• Well determined for the Milky Way
• Very little known about extragalactic
dust extinction
The Galactic Extinction Curve
!
R
V= A(V )
E(B " V ) = A(V ) A(B) " A(V )
!
A( " )
A(V ) = a( " #1 ) + b( " #1 ) R V
(Cardelli et al. 1989)
• Empirically determined
• Mean value is R
V= 3.1 (blue)
• Extreme values: R
V= 1.8 (green) and R
V= 5.6-5.8 (red) ( Cardelli et al. 1989, Fitzpatrick et al. 1999,Udalski 2003 )
• Larger R
V-> larger dust grains
• Bump at 2175 Å (4.6 µm
-1) – Unknown origin
“Reddening”
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Other nearby galaxies
• LMC: Smaller bump and steeper rise into the UV ( Nandy et al. 1981 )
• SMC: No bump, well fitted by A(λ) ∝ 1/ λ ( Prevót et al. 1984 )
• M31: Average Galactic extinction law ( Bianchi et al.
1996 )
Pei (1992)
Other not-so-nearby galaxies
• From QSOs
• Galaxies
• SNe IA
– Lower R
Vvalues
• GRBs
– Predominantly SMC type
• Gravitational lenses
(York et al. 2006)(Noll et al. 2009)(ÁE et al. 2009) (Noterdaeme et al. 2009)
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The Lens Perspective
“You may look in front of you, and on both
sides, if you like," said the Sheep; "but you can't look all round you - unless you've got eyes at
the back of your head.”
- Lewis Carroll (1832-1898)
Gravitational Lenses
• Compare two images, where ideally one should suffer no extinction and the other go through the galaxy
• For more than doubly imaged quasars have the
possibility of getting more than one curve for the
lensing galaxy
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Extinction along both lines of sight
!
A
diff( " ) = A
B( " ) # A
A( " )
= ( E
B# E
A) [ R
Vdiffa( "
#1) + b( "
#1) ]
!
R
VdiffR
VB= 1+ E
A/ E
B1" E
A/ E
B1" R
VAR
VB#
$ % &
' ( ) 1+ *
!
E " E(B # V ) = A(B) # A(V )
( )
Galactic extinction:
The deviation of the real R V to the
deduced R V diff is
given by η, where:
Microlensing
• The lensing by stars or other objects in the lens galaxy
• Affects the continuum part of the emission
• Effects can look like ‘extinction’
• If the data are taken on a timescale smaller than
that of the microlensing signal, then any achromatic microlensing signal should, to first order, only affect the estimate of the intrinsic magnitude ratio
• Time variable data allows to correct for chromatic
microlensing
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Extinction in Lensing Galaxies
• SBS 0909+532
– Double
– z l = 0.83; z Q = 1.38
• Extinction:
– E(B-V) = 0.21 ± 0.02 – R V = 2.1 ± 0.9
⇒ A(V) ≈ 0.44
– Strong detection of the 2175 Å bump
(Motta et al. 2002)
Extinction in Lensing Galaxies
• MG0414+0534
– Quad
– Early type
– z l = 0.96; z Q = 2.64
• Extinction (for both A2-B and A2-C):
– A(V) = 0.9 ± 0.1 – R V = 2.7 ± 0.2
(ÁE et al. 2006)
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Moving towards surveys
“ There are three kinds of lies: lies, damned lies, and statistics. ”
- Mark Twain (1835-1910)
- Paraphrased from Benjamin Disraeli (1804-1881)
Future Surveys
• SNAP and LSST are proposed space/ground telescopes
• Both missions will provide an
extensive sample to study extinction and its evolution with redshift
100-1000 50.000
Wide (WL)
~10 5.000
Deep (SNIa)
Quasar Galaxy
(Marshall et al. 2005)
Compared to 10 systems in the VLT survey!
500 Supernova
4000 Quasar
SNAP
LSST
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Goals
• Measure typical reddening (E(B-V))
• Gives a lower limit
• Measure the steepness of the slope (R V )
• Important for dark energy surveys
⇒ Independent measurement of dust extinction
• Measure the frequency of the 2175 bump
• Can we find tracers for the bump?
• Is the bump created or destroyed?
Ideal LSST data
z=0 z=1 z=2
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Dealing with Biases - LSST
• Microlensing:
• Data will be obtained simultaneously in all bands
• LSST will provide time varying datasets
• Extinction along both lines of sight
• Will find lower limits on E(B-V)
• The mean R V is not expected to be strongly biased - although individual systems can
be
Ambitious Goals
• Can we locate tracers of the bump?
– Metallicity?
– UV radiation field - CI lines?
– Dust to gas ratio?
– PAH emission lines?
• Need extensive
followup for selected systems
(ÁE et al. 2009) (Draine 2003)
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