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Gravitational Flexion: Galaxy

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David Bacon (Edinburgh) - GG Lensing/Theory. Richard Massey ... Priya Natarajan (Yale) - Initial work. Students. Kara Blaine (Drexel) Michael French (Drexel) ... – PowerPoint PPT presentation

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Title: Gravitational Flexion: Galaxy


1
Gravitational Flexion Galaxy Lensing to Second
Order
David Goldberg Drexel University
Gravitational Lensing, Dark Energy and Dark
Matter January 7, 2005
2
  • Acknowledgements
  • David Bacon (Edinburgh) - GG Lensing/Theory
  • Richard Massey (Cal. Tech) - Shapelets
  • John Peacock (Edinburgh) -Clusters
  • Priya Natarajan (Yale) - Initial work
  • Students
  • Kara Blaine (Drexel)
  • Michael French (Drexel)
  • Thanks also to Tereasa Brainerd for helpful
  • comments on the method and initial drafts.

3
Outline
  • What is Flexion?
  • Results from Galaxy-Galaxy Lensing.
  • The topic at hand - Dark Matter/Energy
  • Make a better map of Clusters
  • Tomography
  • Constraints in time-delays?
  • Cosmic Flexion?

4
We all know gravitational lensing distorts
images of background sources...
A simulated lens- source system. An isothermal
sphere, with a lens separated by 5 in the
absence of lensing.
5
In reality, this is not simply an elliptical
distortion
NOT an ellipse!
The Arciness of an image is also important
-- Flexion!
6
  • Why is Flexion useful?
  • A local measurement of the
  • underlying density field
  • Intrinsic arciness has a smaller
  • variance than intrinsic shear
  • - higher S/N!
  • Can be used in a lossless way
  • to supplement shear!

7
How does it work?
8
We define the Flexion as a pair of
vectors giving us information not
otherwise accessible!
9
But, as written, Flexion is VERY hard to invert,
so we use Shapelets (2d Hermite Polynomials)
From Refregier (2003)
10
FlexionShapelets make a great pair. Flexion and
shear can transfer power between nearby
(complementary) coefficients
11
This expands out to a rather nasty (but easily
code-able) set of operators
Let's invert our simulation from earlier...
12
Analytic Solution for an isothermal sphere.
13
We can look at the same effect in shapelet space.
14
Goldberg Bacon (2004) measure the Flexion (
shear) from the Deep Lens Survey (Wittman
2001). As with Shear, Flexion has a preferred
direction.
15
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16
You might point out But the Meeting asked about
Dark Matter Energy! True enough...
17
Clusters 1) As a local measure, Flexion can be
used to find/measure substructure in clusters.
Not to be interpreted As a real measurement!
18
2) Measurement of Cluster ellipticity (similar
to aperture moment analysis in shear). 3)
Complement to shear estimates of
aperture masses.
19
4) Tomography Galaxies at different redshifts
will be lensed by a different amount (Consider,
e.g. Jain Taylor 2004). The difference scales
as the angular diameter distance. We need a very
good knowledge of substructure! But - we could
measure w.
20
Consider two arclets near one another
The R factor is a straightforward function of
cosmology!
A
B
We could use this to compute the equation of
state of Dark Energy!
21
3) Using Flexion with Time-Delay Measurements
of Independent Measurements/Image Delays 1xN
-2 Deflections 2xN-1 Distortions 3xN-1 F
lexion 4xN-1
22
Cosmic Flexion would be able to measure
perturbations on highly nonlinear scales!
23
Conclusions and References
  • Flexion is a powerful means of extracting new
    info from
  • galaxy-galaxy lensing
  • It is measurable, and can have high S/N.
  • Flexion may also be applied to weak lensing in
    clusters,
  • cosmic scales, etc.
  • Strong Flexion effects may be useful in
    time-delay
  • measurements and Tomography
  • Bacon, Goldberg, et al. (2005), in preparation
    -- look for it soon!
  • Goldberg Bacon (2005), ApJ 619.
    astro-ph/0406376
  • Goldberg Natarajan (2004), ApJ 564, 65.
    astro-ph/0107187
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