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Cosmological MHD Hui Li Collaborators: S. Li, M. Nakamura, S. Diehl, B. Oshea, P. Kronberg, S. Colgate (LANL) H. Xu, M. Norman (UCSD), R. Cen (Princeton) Observational overview of large scale magnetic fields Several examples of numerical modeling of cosmological MHD
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Cosmological MHD

Jan 06, 2016

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Cosmological MHD. Hui Li Collaborators: S. Li, M. Nakamura, S. Diehl, B. Oshea, P. Kronberg, S. Colgate (LANL) H. Xu, M. Norman (UCSD), R. Cen (Princeton). Observational overview of large scale magnetic fields Several examples of numerical modeling of cosmological MHD. - PowerPoint PPT Presentation
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Page 1: Cosmological MHD

Cosmological MHDHui Li

Collaborators:

S. Li, M. Nakamura, S. Diehl, B. Oshea,

P. Kronberg, S. Colgate (LANL)

H. Xu, M. Norman (UCSD), R. Cen (Princeton)

Observational overview of large scale magnetic fields Several examples of numerical modeling of cosmological MHD

Page 2: Cosmological MHD

Part I:

Observations

Page 3: Cosmological MHD

Hydra A

Galaxy Clusters

MS0735.6+7421

Page 4: Cosmological MHD

Cluster RadioHalo

A754Kassim et al. ‘01

Page 5: Cosmological MHD

Bachigi et al. 2006, Science

Cluster Accretion Shocks (?)

Page 6: Cosmological MHD

Beyond Clusters…. (???)

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Kronberg et al. 2007, ApJ

Page 7: Cosmological MHD

Part II:

Origin of Extra-Galactic Magnetic Fields

Page 8: Cosmological MHD

Numerical simulations- cold dark matter cosmology = 0.73, DM = 0.27, gas = 0.043, h=0.7, n = 1, 8 = 0.8 without/with gas cooling- computational box: (100h-1 Mpc)3

10243 cells for gas and gravity, 5123 DM particles, x = 97.7 h-1kpc

Ryu et al. 2005

= 1 – 104 <> and higher

Baryon DensityVorticity Generation

Page 9: Cosmological MHD

Cosmic Energy Flow

Gravity

Stars, galaxies, galaxy clusters,

large scale shocks, etc.

IGM

“Feedback”MechanicalChemicalThermal

Non-ThermalMagnetic

collapse

Black Holes

RadiationKinetic WindsMagnetic fields

108 Msun 1062 ergs

Page 10: Cosmological MHD

Part III:

Astrophysical Jet Modeling and Interaction with ICM

Page 11: Cosmological MHD

“flux core: & Iz”(“helix/jet”)

toroidal Bfrom Iz(“lobes”)

confinement(B2

/8 ~ pgas)

Jz @ t = 10global current flow

(Li et al. 2006, Nakamura, Li, Li 2006, 2007)

Page 12: Cosmological MHD

Hydra A

Diehl, Li, et al. 2007

Page 13: Cosmological MHD

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

QuickTime™ and aTIFF (Uncompressed) decompressor

are needed to see this picture.

Zavala & Taylor 20053C273

Differential FRM

Is there current in jets?

Page 14: Cosmological MHD

Part IV:

Magnetic Fields Injected from SMBHs

Page 15: Cosmological MHD

Growing “cherries” on cosmic trees …

Mpc/(1+z)Johnson et al. in preparation

z=2

Page 16: Cosmological MHD

Mpc/(1+z)

B=0.1 G

Li et al. 2007

Page 17: Cosmological MHD

Part V:

Cosmological MHD Simulation of Cluster

formation with Magnetic Fields

Page 18: Cosmological MHD

AMR MHD Cluster Formation Simulations

Same simulation with radiactive cooling, star formation and star formation feedback, uniform initial magnetic fields of 1e-9 G in y direction.

Projected logarithmic baryon density, refined to level 2,4,6 and 8. Each plot has a resolution of 512x512 zones. Best spatial resolution is 7.8125kpc/h

256Mpc/

h4M

pc/h

ΛCMD model, Ω=1, ΩΛ=0.7, Ωb =0.04, h=0.7,and box size = 256 Mpc. Root grid is 1283,refined by 2 to level 8, simulation is from z=30 to z=0.

Page 19: Cosmological MHD

Magnetic Energy Density Evolution

256Mpc/

h

4Mpc/h

Page 20: Cosmological MHD

SZ Effect: y-parameter

256Mpc/

h

4Mpc/h

Page 21: Cosmological MHD

AMR MHD Cluster Formation SimulationsImagines of cluster center(1Mpc/h)

Gas density SZ_y

Magnetic energy density Rotation measurement

Page 22: Cosmological MHD

AMR MHD Cluster Formation SimulationsΛCMD model, Ω=1, ΩΛ=0.7, Ωb =0.04, h=0.7,and box size = 256 Mpc/h. Root grid is 1283,refined by 2 to level 8, simulation is from z=30 to z=0. No initial magnetic fields

Imagines of projected baryon density of inner 4 Mpc/h at z=0, left is from MHD solver and right is from ppm solver

Page 23: Cosmological MHD

AMR MHD Cluster Formation SimulationsΛCMD model, Ω=1, ΩΛ=0.7, Ωb =0.04, h=0.7,and box size = 256 Mpc/h. Root grid is 1283,refined by 2 to level 8, simulation is from z=30 to z=0. No initial magnetic fields

Y parameter of SZ Effect of slice of inner 4 Mpc/h at z=0, left is from MHD solver and right is from ppm solver

Page 24: Cosmological MHD

AMR MHD Cluster Formation SimulationsΛCMD model, Ω=1, ΩΛ=0.7, Ωb =0.04, h=0.7,and box size = 256 Mpc/h. Root grid is 1283,refined by 2 to level 8, simulation is from z=30 to z=0. No initial magnetic fields

X-ray luminosity of of inner 4 Mpc/h at z=0, left is from MHD solver and right is from ppm solver

Page 25: Cosmological MHD

Some Key Problems1. Diffused Radio Emission: Distribution and strength of

cosmic magnetic fields, seeding from first stars, dwarf galaxies, AGN feedbacks, or (turbulent) dynamo.

2. Differential FRM of jet pc-kpc scale: is there current?3. Clusters as magnetic field laboratories: Structure

formation, AGNs, heating, mixing, etc.4. Physical state of IGM: impact on galaxy formation? 5. UHECR transport?6. Does magnetic energy flow destroy the statistics of Lyman-alpha forests?