summary(3) -- dynamics in the universe --

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Summary(3) -- Dynamics in the universe -- T. Ohashi (Tokyo Metropo litan U) 1. Instrumentation for dynam ics 2. Cluster hard X-rays 3. X-ray cavities 4. Dark matter dynamics 5. Large-scale features

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Summary(3) -- Dynamics in the universe --. T. Ohashi (Tokyo Metropolitan U) Instrumentation for dynamics Cluster hard X-rays X-ray cavities Dark matter dynamics Large-scale features. Strong gravity(BH, Darkmatter) Collision, Explosion, Jets, Magnetic fields etc. X-rays. g -rays. - PowerPoint PPT Presentation

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Page 1: Summary(3) -- Dynamics in the universe --

Summary(3)-- Dynamics in the universe --

T. Ohashi (Tokyo Metropolitan U) 1. Instrumentation for dynamics 2. Cluster hard X-rays3. X-ray cavities4. Dark matter dynamics 5. Large-scale features

Page 2: Summary(3) -- Dynamics in the universe --

Science with NeXT

Strong gravity(BH, Darkmatter)Collision, Explosion, Jets, Magnetic fields etc

Gas motion, Shocks

Particle acceleration

Spectroscopy Microcalorimeter

Hard X-ray image Supermirror + imaging detector

-ray spectrum Compton telescope

Gas heating

High-energy universe

X-rays

-rays

Doppler spectroscopy Microcalorimeter

Cosmic rays

Global view of dynamical processes in the universe

Page 3: Summary(3) -- Dynamics in the universe --

Emission lines and Doppler spectroscopy

12 eV

Energy resolution of SXS E~7 eV (or better) Fe-K line complex resolved into resonance, intercombinatio

n, forbidden lines Gas motion with v ~ 100 km s-1 resolved

Page 4: Summary(3) -- Dynamics in the universe --

2-order increase in hard-X sensitivity

Suzaku

NeXT

10 keV 100 keV

Page 5: Summary(3) -- Dynamics in the universe --

LHard ~ 1043 erg s-1 is reported from about 10 clusters

Merger systems tend to show hard X-ray emission

The detection is still controversial.Coma cluster(Fusco-Femiano et al 04 ⇔ Rossetti and Molendi 04)

Cluster hard X-rays

Nevalainen et al. 04

Hard X-rays from 14 clusters

Thermal

Page 6: Summary(3) -- Dynamics in the universe --

Cluster radio halos and relics

A3667: Radio relic

1045 1046Lx

(h=0.5)

Ensslin and Roettgering 02

1042

1041

LRadio

(erg/s)

Feretti astro-ph/0406090

=3 GHz

Page 7: Summary(3) -- Dynamics in the universe --

Expected hard X-ray luminosity

Observed data → LRadio~1041-42 erg s-1

if B = 3 G, then uB ~ uph ~ 0.3 eV cm-3

→ sensitivity of LHard ~ 1041-42 erg s-1 is necessary to explore inverse Compton emission

This is about 100 times higher sensitivity, achievable with the supermirror instrument

If protons carry 100 times more energy than electrons ( magnetic energy density), then non-thermal energy is a large fraction in clusters (equivalent to 1043-44 erg s-

1)

ph

B

IC

syn

u

u

L

L

L

L

X-Hard

RadioMicrowave background

Page 8: Summary(3) -- Dynamics in the universe --

X-ray CavitiesHCG62 (Chandra):Morita et al. 06

“Ghost cavity”

MS0735.6+7421 (z=0.22)McNamara et al. 05

Hot gas displaced by radio lobesGhost cavities are X-ray cavities without radio lobes nor radio galaxy

deviation

Page 9: Summary(3) -- Dynamics in the universe --

Non-thermal pressure

HCG62k/f

k = Ratio of proton/electron energy density

f = filling factor (~1)

Required energy density

>> u(magnetic field + electrons)

Large variation of k All protons or extremely

hot gas? Dunn et al. 05

Pressure to match gas pressure

Page 10: Summary(3) -- Dynamics in the universe --

Dark matter blobs

Gas Dark Matter

(z=0)

Cluster simulation: Eke et al. 98

Galaxy group simulation:Klypin et al. 99

Simulation under CDM scenario

Dark matter blobs are produced

In local group, only ~1/10 are detected as satellite galaxies

Blob velocity (groups): v = 100-1000 km s-1

Page 11: Summary(3) -- Dynamics in the universe --

Motion of dark matter blobs

1E0657-56: Markevitch et al. 04

Weak lens mass (DM travels forward)

Evrard 1990 (line = velocity)

DM particles/blobs continue to move even after gas is relaxed

Dark matter blobs may carry significant fraction of energy

Gas

Darkmatt

er

Page 12: Summary(3) -- Dynamics in the universe --

DM blobs may contribute to acceleration

Particle collision with DM blobs can cause Statistical Fermi acceleration

It is possible to accelerate particles within life of clusters

y1024

1 9coll

2

acc

tVc

t

(V = 2000 km s-1, tcoll = 100 kpc/c = 1013 s)

Dark Matterblob

Particle

V

Intracluster space

Page 13: Summary(3) -- Dynamics in the universe --

Pointing vs survey

Narrow field, high sensitivity: NeXT, Con-X, Xeus

Wide field, survey: eROSITA, MAXI, DIOS Only a few % of the whole sky covered with

CCD resolution Truly large scale structures: cosmic web, G

alactic hot gas, cluster survey etc

Page 14: Summary(3) -- Dynamics in the universe --

Spectroscopy with microcalorimeters

NeXT SXS

Large 12x12 pix, f.l. = 6m

32 pix, f.l. = 9m

Page 15: Summary(3) -- Dynamics in the universe --

Warm-hot intergalactic medium

Yoshikawa et al. 03

5 degree = 75 Mpc

Expectation from DIOS

Page 16: Summary(3) -- Dynamics in the universe --

Dynamics of galactic hot gas

Dynamics of hot galactic ISM: Galactic fountain

OVII

Snowden et al. 95, ApJ 454, 643

Inoue et al. 79, ApJ 227, L85

ROSAT map

GSPC spectrum

Page 17: Summary(3) -- Dynamics in the universe --

Suzaku to NeXT decadeLow background and wide-band sensitivity

Detection of non-thermal emission from bright objects

First image of non-thermal emission with >100 times higher sensitivity

Gas dynamics through X-ray spectroscopy, with low background soft -ray detectors

Science of on-thermal universe will be much advanced

Suzaku

NeXT

+ Wide field mission for complementary science