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(1)

Welcome to the workshop

``Strong Gravitational Lensing in the Next Decade’’

Cogne, Aosta, Italy

(2)

Strong Gravitational Lensing:

A Past, A Present, A Future?

Léon Koopmans

(Kapteyn Astronomical Institute)

Note:

This talk will be my own, sometimes biased,

view of the current state of strong lensing. I hope by the end of the workshop that we have a more common/

shared view where where strong lensing is now and where it should be heading in the next decade.

(3)

Some questions to be addressed during this workshop

What has strong lensing accomplished in the last three decades in terms of scientific results?

Where has strong lensing had the most impact?

What is the current status of the field compared to other techniques?

Where will strong lensing have the most impact in the coming decade?

How many strong lenses do we know and do we cover enough of “parameter space’’?

From where will we obtain new strong lenses?

Should the field get more organized (science cases)?

(4)

Some Accomplishments of Strong Lensing over the last 3 Decades

Cosmography: H0, Ωm, ΩΛ

Galaxy Structure & Evolution

Mass Substructure

Central SMBHs

Galaxy ISM

Source Structure

Alternative Gravity Theories?

More?

Some ramblings on different topics...

(5)

Lens Surveys

(Jackson, Wucknitz, McKean, Marshall, Courbin, Dobler)

(6)

For a field to flourish, it requires not only excellent theory (GR) and detailed modeling, but also a lot of data.

Do we have enough lenses?

There are several (traditional) ways to go about finding new strong gravitational lenses

Imaging: Radio/Optical (efficient)

Spectroscopy: Looking for different redshifts

Variability? Looking for correlated variations

Search for lenses or search for sources?

(if Nlens > Nsrc, search for the src, and visa versa!)

Lens Surveys

(7)

Lens Surveys

To find strong lenses, several requirements have to be met:

(1) The telescope has to have sufficient spatial resolution (<1” typically) to resolve multiple images/arcs/rings

(2) The telescope has to have sufficient survey speed/depth (targeting many objects at once or fast one-by-one;

i.e. blind vs targeted, depending on Nsrc/lens) (3) Preferably the telescope has a wide FOV for blind surveys.

(4) Contrast of lens vs source has to be such that it can be recognized as a lens in the first place.

(5) Luck!

(8)

Lens Surveys

Recent/Past Surveys

CFHT-LS

Muscles

Haggles

Cosmos

SLACS

JVAS/CLASS

SLS-AEGIS

OLS

PANELS

SDSS

2dF Lens Survey

HST Snapshot Lens Survey

FKS Lens Survey

NOT Lens Survey

APM Lens Survey

MG Survey

Discover through luck: Q0957+561

SKA

LOFAR

E-MERLIN

E-VLA

Meerkat/ASKAP

LSST

JDEM/EUCLID

PANSTARRS

more?

Future Survey Instrument

(9)

CLASS SLACS

Lens Surveys

CASTLES

(10)

Lens Surveys

Current Status:

(1) Around ~200 lenses are known (e.g. CASTLES+SLACS);

most surveys discover several to several tens of lenses.

(2) Roughly half of the lenses are source selected (QSOs) and half are lens selected.

(3) Most source-selected surveys have heterogeneous lens samples (lens-selected surveys are more uniform).

(4) It has remained hard to split samples in bins and make detailed statements about trends (small # statistics)

(5) Small number statistics has plagued us for a long time

(11)

Lens Surveys

Questions:

(1) Do we have enough lenses to keep us going for the next decade and is follow-up sufficient, or not?

(2) Do we need larger samples that cover a wider range in

redshift, galaxy/src properties, environment, etc? How large?

(3) Which telescopes/surveys will yield sample of lenses >>100 in the coming decade, or even >>104?

(4) Are we prepared or are we preparing for these and should we push harder to get strong lensing “on the agenda” and into science cases for new telescopes/surveys?

(12)

The Hubble Constant

(Coe, Suyu)

(13)

The Hubble Constant

This was traditionally one of the main science goals of strong lensing. Will/should it remain so and why?

The Hubble Constant is inverse proportional to

the scale of the Universe; light travel time is proportional to the same scale. If we can measure light-travel-time

to an object (or differences), we would know H0.

With lenses we measure time difference between lensed

images, which is a function of geometry (where is the src wrt the images and what Shapiro delays do they have?;

typically these terms are roughly equal).

(14)

The Hubble Constant

(15)

Hence two ingredients are required:

(1) A good mass model (where is the source and what is the Shapiro delay) of the lens, the field and the l.o.s

(2) A good time-delay (few % accuracy)

The Hubble Constant

Monitoring campaigns to get time-delays:

(1) Radio: VLA, MERLIN, [WSRT]

(2) Optical/IR: NOT, COSMOGRAIL, Maidanak (3) X-ray: ???

Follow-up of the lens for modeling

(1) Deep imaging: lens & image structure, color info, etc (2) Spectroscopy: redshifts, kinematics, etc.

(16)

Oguri et al. 2007

(17)

Current Status:

(1) Around 20 systems with time-delays are now known (2) The Hubble Constant still lies between ~60-80 km/s/

Mpc sometimes even lower, when assuming SIE models (3) Too little effort is often going into mass modeling once a time-delay is measured.

(4) All galaxies with time-delays are QSO/AGN and often the lens-galaxy is hard to study, limiting detailed mass modeling. Visa versa, lenses that are easy to study

often have non-varying sources.

The Hubble Constant

(18)

The Hubble Constant

Questions:

(1) Why are lens H0 values still “all over the place”?

Is this due to wrong time-delays, wrong mass models, or wrong physics?

(2) Should we concentrate on more lens system or invest more time in systems where both a good time-delay and a good mass model can be determined?

(3) Is H0 from lensing still interesting and competitive, or is that the wrong question and agreement tests our fundamental understanding of cosmology?

(19)

Cosmography

(20)

Cosmography

Also this in the 1990s was a hot topic in strong lensing, before SNae/CMB/LSS measurements took over. It seems that very little has happened in this field the last 5 years.

How does it work: If one assumes no (or known)

evolution in the comoving number density of lenses and their properties, then the physical number of lenses

(hence the accumulative lensing cross-section) is a function of the volume/length between us and a source at redshift z.

This volume is a function of cosmology and hence the number of lensed objects at a given z depends

on cosmography (e.g. increases with increasing Λ).

(21)

Cosmography

To do lensing statistics properly, once requires a very

well-understood lens survey that is “statistically complete”.

Not many such surveys exists and JVAS/CLASS is probably still the largest survey for these purposes. It has 22 lenses.

Most other surveys are looking to maximize the number of lenses w/o regards to being complete in some sense or

being able to quantify selection effects (e.g. dust, variability, lens/src contrast, survey-brightness limits, flux-ratios, etc).

(22)

Chae et al. 2002

Cosmography

Why is it difficult?

The difference between a (Ωm=1, ΩΛ=0) cosmology and a (Ωm=0.3,

ΩΛ=0.7) cosmology is a factor of two smaller volume to z=1. With

22 lenses a Poisson error of ~4.5 is expected, making the difference

between 22 or 11 lenses only significant at the 2.5-σ level for

an assumed flat Universe even if no systematics are

included (evolution/biases, etc).

(23)

Questions:

(1) Whereas in the 1990s lensing statistics was still competitive, is this still the case?

(2) Could it become competitive again the in the next decade with 100s of new lenses being discovered?

(3) Should we turn around the question and fix the cosmography and use lensing statistics to study

galaxy evolution (i.e. marginalize of cosmography or over galaxy evolution)?

(4) Will lensing statistics ever become competitive again?

(5) Can cosmography be done differently with lenses?

Cosmography

(24)

Galaxy Structure & Evolution

(Auger, Chantry, Halkola, Czoske, Barnabe, vdVen, Grillo, Faure, Nipoti, Meneghetti, Lombardi [clusters])

(25)

Galaxy Structure & Evolution

Strong lensing allows for a precise measurement of galaxies masses and set constraints on their density profiles over a wide range in redshift and moderate

range in galaxy masses.

This provides a powerful method to study galaxy structure & evolution over 8 Gyr in look-back time.

Lensing studies can also be combined with other techniques (e.g. dynamics/X-rays, etc) to improve

precision and accuracy.

(26)

Galaxy Structure & Evolution

Applications vary wildly:

(a) Total density profiles (b) DM density profiles (c) Shape of haloes

(d) Fundamental Plane Studies (e) Calibrating stellar IMF

(f) etc.

(27)

Galaxy Structure & Evolution

Koopmans et al. 2006, 2009

It is not well understood why baryonic & DM add to a combined ~1/r2 density

profile, despite different

physics and starting conditions.

!γLD! " = 2.085+0.0250.018 (68% CL)

Isothermal, but with intrinsic spread of <10%

(28)

Galaxy Structure & Evolution

Kochanek

Joint constraints can be set on stellar mass-

fraction and DM density slope.

(29)

Galaxy Structure & Evolution

Bolton et al; Koopmans et al.

A Mass Fundamental Plane has been found, which sheds

light on the tilt in the FP and the structure of ETGs

(30)

ISM

(Ellisadottir)

(31)

ISM/Scattering/Microlensing

Compact (possibly extended) sources allow on the study the content of the lensing galaxy (e.g. stars, gas, dust, ionized gas, etc). However, this requires disentangling the lensed source structure from what is

happening to it in the lens.

Also scattering/dust/gas, etc can affect the surface brightness of the lensed image and change it

(microlensing does not).

(32)

ISM/Scattering/Microlensing

Some of the main questions addressed in these studies:

(1) A considerable amount of work has been done on

(differential) spectroscopy to look at the gas/dust content in lens galaxies -> provides a detailed look at the ISM

of high-z galaxies hard to get in other ways (e.g. emission).

(2) Some effects of scattering have been found in radio lenses (eg CLASS 0128) that indicates a dense ionized medium (e.g. HII regions, SF, etc).

(33)

Biggs et al.

Surface brightness is not conserved

Motta et al.

ISM/Scattering/Microlensing

Extinction survey at high z

(34)

ISM/Scattering/Microlensing

Questions:

(1) One man’s signal is another man’s noise: Should we worry in lensing studies about microlensing, dust,

scattering etc (e.g. for substructure/time-delay studies).

(2) What have we learned from these studies about the ISM/*IMF of distant galaxies?

(3) Are these studies competitive/complementary/better to/than other studies? Could they provide evolutionary studies of the galaxy ISM/IMF?

(35)

Substructure

(Keeton, Chen, Vegetti, Fassnacht)

(36)

Substructure

Smooth mass models predict a distinct relation between the magification/fluxes of merging cusp/fold images: i.e.

the cusp relation (sum of magnification is zero).

This relation is violated in many instances.

!N

i=1

µi = 0

Mass substructure is generic prediction of the LCDM cosmography and lensing is a unique method to find it.

(37)

Substructure

B2045+265 is a classical example of the cusp violation

Fassnacht et al. McKean et al.

(38)

B2016-112: violation is due to a visible dwarf satellite;

could this hold for many/most anomalous lenses?

Substructure

(39)

Substructure

Dalal & Kochanek

Current predictions are fDM<1% inside Reinst

Limits have been set but some of the data has been questioned, so the jury is still out.

(40)

Questions:

(1) What is current level of substructure and is this interesting for lensing studies?

(2) Is lensing competitive or even unique for substructure studies in the future?

(3) What techniques are there (e.g. flux-ratio/direction

imaging) and what are their complementarities/strength?

(4) How many lenses do we need to pin down the fraction of DM and is mass function?

(5) Could there be too much high-mass substructure?

Substructure

(41)

Central SMBHs

(42)

Central SMBHs

The absence of central (3rd/5th) images in lens galaxies implies that the central density of the lens must be very high.

µ = 1

(1 κ)2 γ2 1 κ2core

µ = 1

(1 κ)2 γ2 1

γSMBH2

Due to density core

Due to central SMBH

If a SMBH exists, the image formed near the center of the galaxy will have properties determined by the

SMBH mass (plus external shear).

(43)

Central SMBHs

Current status/Requirements:

(1) Only one detected central image (Winn et al.) (2) Deep high-resolution and high contrast images (3) Most likely only reachable with VLBI radio

experiments.

(4) Currently still factor ~10 away from required sensitivity.

(5) Asymmetric lens geometries are requires (high flux-ratio), which are even rarer.

(44)

Central SMBHs

Extra images can form (two on one side!) or central image can be

destroyed.

These images or absence can be signs of SMBHs and be used

to quantify their mass in a geometric manner.

Mao et al.; Rusin et al.

(45)

Central SMBHs

Questions:

(1) Is measuring the mass of SMBHs interesting and competitive if ever doable?

(2) Can it provide a model-independent mass measurement?

(3) Can it probe SMBH-mass evolution?

(4) How many lenses are needed to find a single case?

(5) Could one probe gravity in the strong regime?

(46)

Lensed Sources & Their Structure

(Volino, Bradac)

(47)

Source Structure

The high macro/microlensing magnification allows one to study the source structure in great detail.

Caution: Magnification bias works for unresolved sources, but not for resolved source, where the real limit is

not the flux-limit but the surface brightness limit.

Hence lensing provides really only a way to super-resolve a source, but not to gain much in integration time (only because of multiple imaging)!

(48)

Source Structure

Magnification of 200-300 !

Study the counter jet of an AGN at z>3.

More et al.

(49)

Source Structure

Optical image is not anomalous X-ray image is anomalous

Explained by microlensing; requires QSO optical source size >> x-ray size

(50)

Source Structure

Questions:

(1) Can the increasing number of light-curves with

microlensing provide interesting limits on the stellar content (M/L) in lenses?

(2) Are microlensing results being recognized in the AGN community are being interesting?

(3) Will lensing being leading or complementary in studying source structure because of the small numbers of lenses and the serendipity of the source structure?

(51)

Some new surveys & instruments coming online that could provide more lenses?

(1) optical: LSST/Panstarss/...

(2) radio: e-MERLIN/e-VLA/LOFAR/Meerkat/Askap/SKA (3) space: JDEM/Euclid/...

Possible fields of large impact?

(1) Galaxy Structure & Evolution (2) Mass substructure

(3) Central SMBHs?

(4) ... Pick your favorite ...

A Future? Yes!

But we have to keep working

(52)

Some questions to be addressed during this workshop

What has strong lensing accomplished in the last three decades in terms of scientific results?

Where has strong lensing had the most impact?

What is the current status of the field compared to other techniques?

Where will strong lensing have the most impact in the coming decade?

How many strong lenses do we know and do we cover enough of “parameter space’’?

From where will we obtain new strong lenses?

Should the field get more organized (science cases)?

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