+ All Categories
Home > Documents > Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy...

Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy...

Date post: 19-Dec-2015
Category:
View: 214 times
Download: 1 times
Share this document with a friend
Popular Tags:
16
Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans & Alexie Leauthaud The COSMOS Lensing Team: Jean-Paul Kneib, Justin Albert, David Bacon, Joel Berge, Richard Ellis, Cécile Faure, Anton Koekemoer, Yannick Mellier, Satoshi Miyazaki, John Peacock, Alexandre Refregier, Nick Scoville, Elisabetta Semboloni, Lidia Tasca, James Taylor, Ludovic Van Waerbeke The ACS Parallel team: Jon Gardner & Nicholas Collins
Transcript
Page 1: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Cosmic Shear with HSTJason Rhodes, JPL

Galaxies and Structures Through Cosmic TimesVenice Italy

March 27, 2006

with Richard Massey, Catherine Heymans & Alexie Leauthaud

The COSMOS Lensing Team: Jean-Paul Kneib, Justin Albert, David Bacon, Joel Berge, Richard Ellis, Cécile Faure, Anton Koekemoer, Yannick Mellier,

Satoshi Miyazaki, John Peacock, Alexandre Refregier, Nick Scoville, Elisabetta Semboloni, Lidia Tasca, James Taylor, Ludovic Van Waerbeke

The ACS Parallel team: Jon Gardner & Nicholas Collins

Page 2: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

If there is any intervening large-scale structure, light follows the distorted path (exaggerated). Background images are magnified and sheared by ~2%, mapping a circle into an ellipse. Lensing is most effective for mass structures half way between the source and the observer.

zobserver=0

zgalaxy≈1

zlens≈0.3–0.5

Weak lensing effect cannot be measured from any individual galaxy.

Must be measured statistically over many galaxies

Weak Gravitational Lensing

Page 3: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

How Gravitational Lensing WorksHow Gravitational Lensing Works

Two component ellipticity

Positive Negative

e1

e2

•Statistical measurement on many galaxies•Lensing induced ellipticities 1-2%•Telescope Point Spread Function (PSF) is the primary systematic concern –it changes e!

•Assume galaxy shears are intrinsically uncorrelated•Need to measure shear quite accurately

Page 4: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Patterns in a shear field

Clusters are patterns in a shear field:

Page 5: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

HST Surveys With ACS

GEMS UDF

GOODS

COSMOS

ACS Parallel Survey

Page 6: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

COSMOS For WL•2 square degrees•Single orbit F814(I) ACS images•~80 resolved galaxies per square arcmin•versus ~30 from the ground•Redshifts for lenses galaxies•Unique combination of area, depth and resolution•Opens door for unprecedented dark matter maps and statistics at small angular scales

Page 7: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

The PSF Problems

•PSF time variability•CTE degradation

See Rhodes et al 2006, astro-ph/0512170

Page 8: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

TinyTim- The PSF Solution

Page 9: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Parametric CTE Correction

Page 10: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Shear-shear correlation functions

Page 11: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

E-B mode split

Page 12: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Redshift tomography

Page 13: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Redshift tomography

0.4<z<0.8

0.8<z<1.1

1.1<z<1.5

z>1.5

Page 14: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Cosmological parameter constraints

Courtesy Joel Bergé

8

Ωm

ww

-3.0 -2.5 -2.0 -1.5 -1.0 -0.5 0.0

Page 15: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Combined Errors

Page 16: Cosmic Shear with HST Jason Rhodes, JPL Galaxies and Structures Through Cosmic Times Venice Italy March 27, 2006 with Richard Massey, Catherine Heymans.

Complementary Error bars


Recommended