• No se han encontrado resultados

Elizabeth Cooke

N/A
N/A
Protected

Academic year: 2022

Share "Elizabeth Cooke"

Copied!
50
0
0

Texto completo

(1)

Elizabeth Cooke

Collaborators: Nina Hatch, Stuart Muldrew, Emma Rigby, Jaron Kurk, Dan Stern, Dominika Wylezalek + CARLA collaboration

ING La Palma March 2014

(2)

Intro to clusters

High z protoclusters

MRC2104-242

CARLA survey

Red sequences

(3)

Useful tools

Probes of history of galaxy and structure formation

Cosmology

Galaxy evolution-labs of 1000s of galaxies

Representative sample of the Universe

Galaxies in clusters differ from field:

Redder (e.g. Bamford et al., 2009)

Predominantly early types (e.g. Dressler et al., 1980)

Older ellipticals (e.g. Rettura et al., 2010)

(4)

Larger (e.g. Papovich et al., 2012)

More massive (e.g. Steidel et al., 2005)

Redder (e.g. Hayashi et al., 2012)

More metal rich (e.g. Kulas et al., 2013)

High z (proto)clusters can help constrain what physical processes are going on

(5)

Usual methods (X-ray, red sequence...) don’t work

Radio-loud AGN (RLAGN) tend to reside in

overdense environments (Venemans et al. 2007)

Act as beacons for protoclusters

(6)

No difference in sSFR between (proto)cluster and field

Used K band flux to estimate masses

AV ∝ M

Do these results change with more robust

measures of mass/AV?

From Koyama et al., 2013a

(7)

z = 2.49

2.5′ x 2.5′

Study properties of any galaxies with respect to environment at this redshift

MRC2104 COSMOS UDS GOODS-S

A = 7.09 sq arcmin A =170.4 sq arcmin (total)

(8)

NB survey

VLT: ISAAC NB λcen = 2.29μm

VLT HAWK-I: K, J, H

Gemini GMOS: g′, z′

IRAC: 3.6μm, 4.5μm

MIPS: 24μm

Herschel: 250μm

(9)

Look for excess NB flux compared to Ks image

(10)
(11)
(12)
(13)

Ks-NB colour vs NB magnitude

Σ > 2

Selection in SFR

(14)

Remove low-z contaminants

BzK

(B-z) – (z-K) > -0.2

(Daddi et al., 2004)

IRAC

[3.6]-[4.5] > -0.1

(Papovich et al., 2008)

(15)

FAST

(Kriek et al., 2009, ApJ)

SEDs robust

measure of mass

Line emission not accounted for

Constrained

redshift to centre of NB filter

Elizabeth Cooke

(16)
(17)

Green : Hα emitters Blue : AGN

Red : red galaxies

(18)

Spatial density of 8 x control field density

Overdensity of same order as other

protoclusters (e.g. Hayashi et al., 2012; Hatch et al., 2011b;

Kurk et al., 2004)

MRC2104 COSMOS UDS GOODS-S

17 sources 34 sources (total)

A = 7.09 sq arcmin A =170.4 sq arcmin (total)

(19)

Radio galaxy and “companions” not included

(20)

Radio galaxy and “companions” not included

Mass SFR AV sSFR

Suspected AGN in blue

(21)

Masses from SED fits

KS = 2.2x10-5

Consistent with previous

surveys

Steidel et al., 2005

Hatch et al., 2011b

Koyama et al., 2013

(22)

AV from UV slope

E(B-V) = 0.25(B-z + 0.1)AB (Daddi et al., 2004)

KS = 3.2x10-6

(23)

SFR/sSFR from Hα fluxes

KS >0.05 for M > 1010Mʘ

(24)

Hα SFR

Corrected for extinction

Same sSFR- no starbursts

MRC2104 galaxies more

massive/star forming

(25)

Stacked MIPS 24μm images

Calculate SFR in 2 ways:

ULIRGs (Reike et al., 2009)

Main sequence

(Rujopakarn et al., 2013)

MRC2104-242 COSMOS

UDS GOODS-S

(26)

IR+Hα SFR

More hidden SF in

protocluster

Possible starbursts (2σ)

(27)

SFR-mass relation of protocluster and control field galaxies are consistent

Observed mass distributions very different

Overdensity function of mass

(28)

At M>1010Mʘ protocluster is 25x

control field density

Lack of low mass

objects seen in

protocluster

(29)

Mass functions

Observational effects

Dust

Quenching

Mass segregation

(30)

Mass functions

Observational effects

◦ Dust

◦ Quenching

Mass segregation

(31)

Mass functions

Observational effects

Dust

Quenching

Mass segregation

(32)

Mass functions

Observational effects

◦ Dust

◦ Quenching

Mass segregation

Circle = 10 Mpc diameter, comoving

(33)

8x density of control field – protocluster

Protocluster galaxies are more massive and have more hidden star formation

Mass effect

Average SFR-mass relations are the same in both environments

Large difference in the mass distributions

Expect 21-22 galaxies in the protocluster at M < 1010Mʘ

Higher level of dust extinction in low mass galaxies in the protocluster?

Protocluster forming more high mass galaxies

monolithic collapse ?

undergoing more mergers in the early stages of their growth?

Tentative evidence of a larger fraction of starburst galaxies in the protocluster than in the control field

Further data required to confirm 250μm detections

Need a larger selection of protoclusters

(34)

Clusters Around Radio-Loud AGN

Spitzer: ~400 hours

419 RLAGN

(35)

Spitzer IRAC selection

[3.6] – [4.5] > -0.1

(36)

Density- RLAGN in overdense environments

92% denser than SpUDS peak

55% >2σ

37% >3σ

(Wylezalek et al. 2013)

(37)

i′ band

looking for evolved galaxies that have quenched SF and moved onto the red sequence

(From Eisenhardt et al., 2008)

(38)

WHT: ACAM

2 hours per target

~30 targets in total

(39)
(40)

Circle = 1 arcmin

(41)
(42)
(43)
(44)

Control field = UDS (1 sq.deg)

(45)

Statistically subtract contaminants

(46)

Statistically subtract contaminants

Grey = UDS control field Black =

target field – control field

(47)

Low z <i-[3.6]>

(Eisenhardt et al. 2008)

(48)

<i-[3.6]> can distinguish between different formation redshifts

(49)

First look: difficult to see any trend

(50)

Average RS galaxy colour can indicate zf for cluster

Large sample of clusters required due to hugely varying cluster to cluster properties

Work in progress, next steps:

Improve contamination subtraction

Measure strength/scatter of any red sequences

Referencias

Documento similar

The circularized stellar mass density profiles for the galaxies in our sample, comparing them with similar mass SDSS ETGs and the massive compact galaxies in Szomoru et al..

Many of the cluster members are detected, including some embedded, very low-mass objects, several protostars (some of them extended), and substantial emission from the

Comparison of the observed and expected number of events in control and signal regions for the dimuon and dielectron mass distributions... the technical and administrative staff at

Since the dilepton mass distribution and lifetime- related variables are only weakly correlated in simulated background candidates, the shape of the mass distribution is

The mass distributions observed in data together with the background estimate, its system- atic uncertainty and examples of expected signal are shown in figures 2–4 for the

In the MSSM, radiative corrections to the Higgs mass are required due to the smallness of the tree-level Higgs quartic coupling (not large enough to be consistent with LEP Higgs

Therefore to characterize and study possi- ble evolution effects of the structural and dynamical properties of ELOs, we describe their three dimensional distributions of mass

Our previous results on the Higgs mass corrections show that the corrections to the lightest Higgs mass ∆m h are negative in many of the studied cases and can be very large for