Presentation is loading. Please wait.

Presentation is loading. Please wait.

Hideki Maki Department of Physics, Rikkyo University

Similar presentations


Presentation on theme: "Hideki Maki Department of Physics, Rikkyo University"— Presentation transcript:

1 Hideki Maki Department of Physics, Rikkyo University
Dissipation of Magnetic Flux in Primordial Clouds Hideki Maki Department of Physics, Rikkyo University Collaborator: Hajime Susa (Rikkyo University) * This work was partly supported by the “Rikkyo University Special Found for Research”. September Mini Niigata

2 Importance of the First Star’s Mass
Of course, its own is one of the interesting things. Influence on the reionization of the universe Massive stars → strong UV → earlier reionization Heavy elements pollution Massive stars → production of heavy elements WMAP QSO absorption lines The mass of first stars affects the formation of objects after the first star forming. September Mini Niigata

3 Mini workshop @ Niigata
Mass of First Stars Star formation Fragments of high dense gas that are the parent of star are formed. Mass accretes to the core that is formed at the center of the fragment. envelope CDM density perturebation mass accretion stellar core fragments mass of a star depends on the fragment’s mass and mass accretion rate. Therefore, September Mini Niigata filament

4 Mini workshop @ Niigata
Mass Accretion Rate accretion disk stellar core mass accretion Envelope with angular momentum Formation of accretion disk Accretion rate depends on the rate of angular momentum transport. Mass of the first star depends on the mechanism of angular momentum transport. One of the possible mechanism is the turbulence by magnetorotational instability. (e.g. Sano, Inutsuka & Miyama 1998: Sano & Inutsuka 2001) But, we are neglecting the magnetic fields on the studies for first star, since one consider that magnetic flux in the early universe is very weak. Magnetic flux must be considered in primordial cloud too?! September Mini Niigata

5 Thermal Evolution of Primordial Cloud
Collapse of primordial gas cloud No heavy elements and grains Collapse at high temperature Much differential thermal history than present-day (Omukai 2000) Is dissipation history of the magnetic flux different ? September Mini Niigata

6 Mini workshop @ Niigata
Purpose In order to assess the seed magnetic flux in the accretion disk of first stars, we investigate the appearance of dissipation of the magnetic flux in the course of collapse of the primordial cloud. We will study the influence of seed magnetic flux for the transport of angular momentum in primordial clouds. We will derive the mass of first stars. September Mini Niigata

7 Mini workshop @ Niigata
Method : Contraction Free-fall core collapse One-zone approximation Equation of state with poritoropic index γ=1.1 (K : constant coefficient.) September Mini Niigata

8 Method : Chemical Network
Non-equilibrium of 24 species 114 chemical networks collision ionization, collision dissociation recombination, electron attachment 3 body reaction, etc. no photo-ionization, no photo-dissociation Rate equations September Mini Niigata

9 Dissipation of Magnetic Flux
Dissipation process Ohmic loss Magnetic energy loss as thermal energy, by charged particles colliding with neutral particles. Ambipolar diffusion Charged particles twine around the magnetic lines by Lorenz force. On the other hand, since neutrals are not influenced by the Lorenz force, neutral particles fall into the stellar core with the relative velocity for charged particles. So, magnetic flux seems to diffuse out the cloud at the point of neutrals. n n n p e e p e e p n p n n B B B p e p e p n n e n n September Mini Niigata

10 Mini workshop @ Niigata
Diffusion Velocity In this work, the relative velocity of dissipation for collapse gases is defined using the argument in Nakano & Umebayashi We investigate the degree of dissipation by looking a ratio of diffusion velocity for free-fall velocity. Ohmic loss Ambipolar diffusion : electrical conductivity : viscous damping time notation ν : charged particles notation n : neutral particles : reduced mass : momentum-transfer rate coefficient R : radius of cloud, c : speed of light q : charge, n : number density : free-fall velocity M : mass of cloud September Mini Niigata

11 Results at Present-Day
Evolution of ionized fraction at present-day diffusion velocity at present-day main charged particles : e, ions frozen dissipation main charged particles : charged grains (Nakano & Umebayashi 1986) September Mini Niigata

12 Initial Conditions of Primordial Cloud
Density : Temperature : Mass : Jeans mass : Chemical abundance :   values at 1+z =1 (Galli & Palla 1998) September Mini Niigata

13 Mini workshop @ Niigata
Initial Magnetic Flux rotation of protogalaxy Still too much uncertainty. generation of vorticity generation of seed magnetic flux (Biermann battery effect) We regard the initial magnetic flux as parameter. We take B = G. dynamo by rotation of galaxy within galaxy formation time (Pudritz & Silk 1989) September Mini Niigata

14 Results : Evolution Ionized Fraction
Decreases by recombination September Mini Niigata

15 Results : Diffusion Velocity
Dissipation : Viscous dumping time Frozen  :Cyclotron frequency Resign of ambipolar diffusion Resign of ohmic loss Br2=const. September Mini Niigata

16 Inefficient Ohmic Loss
diffusion velocity at present-day diffusion velocity at primordial Ohmic loss efficient main charged particles : grains (Nakano & Umebayashi 1986) September Mini Niigata

17 Mini workshop @ Niigata
Conclusions Magnetic fields are frozen, as far as the condition B<10-5(nH/1 cm-3) G is satisfied. If B=10-20 G at nH=1 cm-3, magnetic flux might be amplified to B~10-6 G at nH=1018 cm-3. future We next study the influence of seed magnetic flux for the transport of angular momentum in primordial clouds. September Mini Niigata


Download ppt "Hideki Maki Department of Physics, Rikkyo University"

Similar presentations


Ads by Google