weak Gravitational Lensing Weak Lensing 1 Tom Kitching

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(weak) Gravitational Lensing

(weak) Gravitational Lensing

Weak Lensing 1 Tom Kitching

Weak Lensing 1 Tom Kitching

Introduction • Lecture 1 : Introduction to w� eak lensing • Background to the

Introduction • Lecture 1 : Introduction to w� eak lensing • Background to the subject • Basic equations and derivations • Lecture 2 : Observing weak lensing • How to observe weak lensing • Overview of simulations • Lecture 3 : Statistics of weak lensing • Cosmic shear • Fisher matrices

Part I : Introduction to Lensing • • Weak lensing Why is weak �

Part I : Introduction to Lensing • • Weak lensing Why is weak � lensing useful Brief History of Surveys Current and future cosmological applications

Introduction • What is weak lensing? • strong vs. weak lensing

Introduction • What is weak lensing? • strong vs. weak lensing

What is Gravitational Lensing? • •

What is Gravitational Lensing? • •

Kappa > 1 Strong Lensing Multiple Images z

Kappa > 1 Strong Lensing Multiple Images z

Kappa<< 1 Weak Lensing Local Distortion © NASA z

Kappa<< 1 Weak Lensing Local Distortion © NASA z

What can we observe? z z

What can we observe? z z

What can we observe? z •

What can we observe? z •

z z

z z

Why is weak lensing useful? • Low-z equivalent to high-z CMB

Why is weak lensing useful? • Low-z equivalent to high-z CMB

Weak Lensing Surveys • What we need • Large field, high resolution • Mostly

Weak Lensing Surveys • What we need • Large field, high resolution • Mostly in optical so far (some radio) • Weak Lensing by LSS First Detected in 2000 • • Bacon et al. Kaiser et al. van Waerbeke et al. Wittman et al.

Kaiser Kasier et al. 2000 Kaiser 2000

Kaiser Kasier et al. 2000 Kaiser 2000

Weak Lensing Surveys • Current and on going surveys Euclid DES LSST Ki. DS*

Weak Lensing Surveys • Current and on going surveys Euclid DES LSST Ki. DS* Pan-STARRS 1** CFHTLen. S** 05 10 ** complete or surveying * first light 15 20 25

Dark Energy • Current constraints, • Kitching et al, (2007) COMBO-17 2 sqdeg proof

Dark Energy • Current constraints, • Kitching et al, (2007) COMBO-17 2 sqdeg proof of concept • Sembolini et al. (2006) • Kilbinger et al. (2009) CFHTLS 170 sqdeg Preliminary results • Schrabback et al. (2010) COSMOS, 2 sqdeg

Dark Energy • Expect constraints of 1% from Euclid

Dark Energy • Expect constraints of 1% from Euclid

Dark Matter • Clusters • Halo masses • 3 D DM mapping

Dark Matter • Clusters • Halo masses • 3 D DM mapping

Part II: Weak Lensing Foundations • • Lens Equation From General Relativity Derivation of

Part II: Weak Lensing Foundations • • Lens Equation From General Relativity Derivation of the Distortion Matrix Complex Notation for shear

Geometry • The Born Approximation

Geometry • The Born Approximation

The Lens Equation • Lens equation and define the terms Relates True Position to

The Lens Equation • Lens equation and define the terms Relates True Position to Observed Position

Deflection Angle from GR • Want to know what the deflection angle is

Deflection Angle from GR • Want to know what the deflection angle is

Deflection Angle from GR §

Deflection Angle from GR §

Deflection Angle from GR

Deflection Angle from GR

Deflection Angle from GR • Equation of motion of deflected light §

Deflection Angle from GR • Equation of motion of deflected light §

GR-Newton Factor of 2 Confirmed in 1919 © R. Massey 2010

GR-Newton Factor of 2 Confirmed in 1919 © R. Massey 2010

The Distortion Matrix • Go back to the lens equation • Every point is

The Distortion Matrix • Go back to the lens equation • Every point is mapped to a new point via a shear mapping

The Distortion Matrix • Define a lensing potential • Projected Newtonian potential - Born

The Distortion Matrix • Define a lensing potential • Projected Newtonian potential - Born approximation (linear transform) • Describes how unlensed point maps to lensed point • =0 implies no mass and no lensing

The Distortion Matrix • Define the Distortion Matrix as • Derivatives of the lensing

The Distortion Matrix • Define the Distortion Matrix as • Derivatives of the lensing potential • 11, 22, 21, 12

Shear and Convergence • Closer look at the Distortion matrix • Decompose into a

Shear and Convergence • Closer look at the Distortion matrix • Decompose into a trace and traceless part • Define

Shear and Covergence • What shape of distortion does this imply?

Shear and Covergence • What shape of distortion does this imply?

Disortion is Elliptical • For a general set of source positions X write the

Disortion is Elliptical • For a general set of source positions X write the eigen equation • • AX= X (A- )X=0 Characteristic equation : |A- 1|=0 are the eigenvalues

Disortion is Elliptical • Solving the determinant

Disortion is Elliptical • Solving the determinant

Disortion is Elliptical • The shear is symmetric under rotations of 180 degrees •

Disortion is Elliptical • The shear is symmetric under rotations of 180 degrees • Anew=RAold. RT • Distortion is elliptical • “Ellipticity” defined as note |e|< 1 or with r (see next lecture)

Distortion is elliptical 1 2

Distortion is elliptical 1 2

Complex Notation • Can write shear in complex form • Shear is a spin-weight

Complex Notation • Can write shear in complex form • Shear is a spin-weight 2 field • Symmetric under rotations of 180 deg. • Polarisation also an example of spin-2 • Kappa is is spin-wight 0 field (symmetric under any rotation) • Spin 0 = scalar • Spin 1 = vector

Raising and Lowering • Shear as spin 2, Kappa as spin 0 • is

Raising and Lowering • Shear as spin 2, Kappa as spin 0 • is a scalar (spin-0) field • Define a complex derivative • A raising/lowering opertato • Kappa and shear are now defined as

Recap • Lensing useful for • Dark energy • Dark Matter • Lots of

Recap • Lensing useful for • Dark energy • Dark Matter • Lots of surveys covering 100’s or 1000’s of square degrees coming online now

Recap • Lensing equation • Local mapping • General Relativity relates this to the

Recap • Lensing equation • Local mapping • General Relativity relates this to the gravitational potential • Distortion matrix implies that distortion is elliptical : shear and convergence • Simple formalise that relates the shear and convergence (observable) to the underlying gravitational potential

Next Lecture How do we measure the lensing effect?

Next Lecture How do we measure the lensing effect?