Bridging galaxy cluster to galaxy simulations

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Bridging galaxy cluster to galaxy simulations Biffi, Rasia (OATS), Petkova (C2PAP), Ragagnin (LRZ), Arth, Bocquet, Remus, Saro, Steinborn, Teklu (USM) Klaus Dolag, Universitäts Sternwarte München www.magneticum.org

Transcript of Bridging galaxy cluster to galaxy simulations

Page 1: Bridging galaxy cluster to galaxy simulations

Bridging galaxy cluster togalaxy simulations

Biffi, Rasia (OATS), Petkova (C2PAP), Ragagnin (LRZ), Arth, Bocquet, Remus, Saro, Steinborn, Teklu (USM)

Klaus Dolag, Universitäts Sternwarte München

www.magneticum.org

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z=0

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Setup:

2x45363

= 186.659.085.312 particle

200 bytes (DM), 456 bytes (GAS)

6 x 512 x 2 x 28 = 172032 tasks

1 MPI task per socket, 28 OpenMP per MPI

68.5 TB for single checkpointing

reaching 150 Gbyte/sec

Various Improvements

Full OpenMP

KD, G. Bazin (USM), M. Petkova (C2PAP)

GreenTree

A. Ragagnin (LRZ)

OpenMP nonblocking density

V. Karakasis (IPCC)

Various memory optimizations

KD, M. Petkova (C2PAP)

Peak 170 Gbyte/sec

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Single bad node

global timestepdying nodes

checkpointing

Power Consumption

12 h

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The Simulations ... Physics:cooling+sfr+windsSpringel & Hernquist 2002/2003

Metals coolingWiersma et al. 2009

SNIa,SNII,AGBTornatore et al. 2003/2006

BH+AGN feedbackSpringel & Di Matteo 2006

Fabjan et al. 2010

Hirschmann et al. 2014 (std)

Steinborn et al. 2015 (new)

Thermal conduction1/20th SpitzerDolag et al. 2004

Numerics:

New Kernels: WC6Dehnen et al. 2012

Low visc. schememr/hr (time dep. alpha)Dolag et al. 2005

uhr (high order grad.)Beck et al. 2015

No finetuning of parameters

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Verification I: large scales (SZ)8.8 x 8.8 degree lightcone up to z=5

Reconstructed (y) from public PLANCK data:

5.4x10-8 < (y) < 2.2x10-6 (Khatri & Sumyaev 2015)

Predicted (y) from map: 1.2x10-6

KD, Sunyaev & Komatsu 2015

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Reproduces Observations (e.g. no

tension with SZ observations !)

Simulation

Tinker 2008

Bocquet 2016

KD, Sunyaev & Komatsu 2015

Verification II: SZ power spectrum

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What Box0 does for Clusters

Bocquet et al. 2016

Accurate halo mass

function including

baryonic processes

for cosmological

applications .

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Verification III: pressure profiles

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(Hot) gas mass of halos

B

A

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Intra Cluster Light

A3888

(Krick et al., 2008)

Virgo

(Mohos et al., 2009)

Box2/hr

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Intra Cluster Light

A3888

(Krick et al., 2008)

Virgo

(Mohos et al., 2009)

Box2/hr

KD, Murante & Borgani 2010

A2199

(Bender et al., 2015)

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Intra Cluster Light

A3888

(Krick et al., 2008)

Virgo

(Mohos et al., 2009)

Box2/hr

A2199

(Bender et al., 2015)

𝜌𝐸𝑖𝑛 𝑟 = ρ0 exp −𝑟

𝑟𝐸𝑖𝑛

α𝐸𝑖𝑛

Fiting Einasto profile

to the stellar component

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Outer halos of Galaxies

Mvir=1e15

Mvir=1e12

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Remus et al.,in prep

Martinez-Delgado et al., 2010

Andromenda

(Irwin,McConnachi, Martin)

Outer halos of Galaxies

Mvir=1e15

Mvir=1e12

MW, Xue et al., 2015

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Remus et al., to be submitted

Martinez-Delgado et al., 2010

Andromenda

(Irwin,McConnachi, Martin)

Outer halos of Galaxies

Mvir=1e15

Mvir=1e12

MW, Xue et al., 2015

Fitting power law

to outer part

MW γ=-6

(Deason et al. 2013)

Andromeda γ=-3

(Ibata et al. 2013)

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Stellar mass function

B

A

Box3/hr

AGN (std)

AGN (new)

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LRG clustering

Steinborn 2016a, in prep128 Mpc/h (hr, new)

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AGN clustering

Steinborn 2016a, in prep128 Mpc/h (hr, new)

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AGN triggering

Steinborn 2016b, in prep

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Morphology of galaxies

Teklu et al. 2015

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Dynamics of galaxies

Simulations

Observations

Teklu et al. 2015

Simulations

Observations

Spheroidals Disks

Stellar mass Stellar mass

Ste

lla

r A

ng

ula

r M

om

en

tu

m

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Dynamics of galaxies

Remus et al. 2015

Ste

lla

r A

ng

ula

r M

om

en

tu

m

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Linking things across all scalesSN 1006

Raynolds et al. 2011

Oxigen ejecta

CALIFA

Sanchez et al. 2014

R200

Perseus

Simionescu et al. 2012Tracing stellar debris with metals

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Chemical enrichment:

std new

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Metal composition in the ICM ?

De Plaa et al. 2007

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Level 0: Metals (Fe) in clusters

Festd

new

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Level 1: composition in clusters

Ni/Fe

O/Fe (SNII)

Ca/Fe (SNIa) Ar/Fe

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Level 2: CC and non CC clustersCC non CC

sims vs obs sims vs obs

entropy

Fe abundance

Rasia et al. 2015

11/29 18/29

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Level 3+4: Metals in galaxies

Mass-metalicity relation for

stars in galaxies (Box4/uhr)

E. Mevius (MA)

Radial profile for

gas in galaxies

M* M*

r/Reff

[Fe

/H

][Fe

/H

]

Mass-metalicity relation for

gas in galaxies (Box4/uhr)

12

+lo

g(O

/H

)

r/Reff

12

+lo

g(O

/H

)

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M51

Fetcher & Beck 2006

Stephans Quintet

Soider et al. 2011

SNR or PWN

Raynolds et al. 2011

Linking more things across scales

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A very simple modelA sub-resolution seeding model basedon supernovae:

Beck et al. 2013

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Exploring a galactic halo forming

Beck et al. 2013

Results do not strongly depend on detailed

parameter choices of the SN seeding model !

SN seeding

RM

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Exploring a galactic halo forming

Beck et al. 2013

Evolution of intrinsic RM of the SN seeding model vs Observations !

Percentiles of sight-

lines through halo,

no disc included !

In

trin

sic

R

otatio

n M

ea

su

re

[ra

d/m

2]

redshift

Williams (2015)

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Applying to a cosmological volume

density magnetic field

Box3/hr (128 Mpc/h) of the Magneticum Pathfinder set.

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Rotation Measure in Clusters (III)R

otatio

n M

ea

su

re

x-Ray brightness

Observations

Simulations

Adding cool-core systems

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There are various physical processes (outer halo, metals , magnetic fields and

more) which are linked accross various scales allowing to investigate the validity

range of our physical descriptions (direct or indirect).

Conclusions:

Be happy (clusters) !

AGN

Conduction

With AGN vs no AGN

Rasia et al. 2015

First time reproducing CC and

non CC Clusters in simulations:

• Complicated interplay between

AGN and heat transport

• Magnetic fields will play crucial

role (modifying heat transport)

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There are various physical processes (outer halo, metals , magnetic fields and

more) which are linked accross various scales allowing to investigate the validy

range of our physical descriptions (direct or indirect).

Conclusions:

Be happy (galaxies) ?

Schlachtberger (MT,2014)

Zoom-in

Simulations of 4

isolated ETGs:

one forms by

major merger of

two LTGs

one forms by

major merger of

two ETGs

one is already an

ETG at high

redshift and

grows through

smooth accretion

One forms

through multiple

minor merger

events

Box4/uhr z=2

Teklu. in prep

Physics in the scaller ?