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An argument that the dark matter is axions

An argument that the dark matter is axions. Pierre Sikivie Center for Particle Astrophysics Fermilab, March 17, 2014 Collaborators: Ozgur Erken, Heywood Tam, Qiaoli Yang Nilanjan Banik. Cold dark matter axions thermalize and form a

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An argument that the dark matter is axions

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  1. An argument that the dark matter is axions Pierre Sikivie Center for Particle Astrophysics Fermilab, March 17, 2014 Collaborators: Ozgur Erken, Heywood Tam, Qiaoli Yang Nilanjan Banik

  2. Cold dark matter axions thermalize and form a • Bose-Einstein condensate. Outline • The axion BEC rethermalizes sufficiently fast that • axions about to fall onto a galactic halo almost all • go to the lowest energy state for given total • angular momentum. 3. As a result the axions produce - caustic rings of dark matter - in the galactic plane - with radii

  3. There is observational evidence for the existence • of caustic rings of dark matter • - in the galactic plane • - with radii • - with overall size consistent with tidal torque • theory • The evidence for caustic rings is not explained • if the dark matter is entirely in some other form. • Ordinary cold dark matter (WIMPs, sterile • neutrinos, non-rethermalizing BEC, …) • forms tent-like inner caustics.

  4. The remaining axion window laboratory searches cosmology stellar evolution

  5. There are two cosmic axion populations: hot and cold. When the axion mass turns on, at QCD time,

  6. Axion production by vacuum realignment V V a a initial misalignment angle J. Preskill, F. Wilczek + M.Wise; L. Abbott + P.S.; M. Dine + W. Fischler 1983

  7. Cold axion properties if decoupled number density velocity dispersion phase space density

  8. Bose-Einstein Condensation if identical bosonic particles are highly condensed in phase space and their total number is conserved and they thermalize then most of them go to the lowest energy available state

  9. why do they do that? by yielding their energy to the non-condensed particles, the total entropy is increased. BEC preBEC

  10. the axions thermalize and form a BEC after a time the axion fluid obeys classical field equations, behaves like CDM the axion fluid does not obey classical field equations, does not behave like CDM

  11. the axion BEC rethermalizes the axion fluid obeys classical field equations, behaves like CDM the axion fluid does not obey classical field equations, does not behave like CDM

  12. from M.R. Andrews, C.G. Townsend, H.-J. Miesner, D.S. Durfee, D.M. Kurn and W. Ketterle, Science 275 (1997) 637.

  13. Axion field dynamics O. Erken et al., PRD 85 (2012) 063520 From self-interactions Fromgravitationalself-interactions

  14. In the “particle kinetic” regime implies When

  15. 4 1 2 3

  16. D. Semikoz & I. Tkachev, PRD 55 (1997) 489D.

  17. After , axions thermalize in the “condensed” regime implies for and for self-gravity

  18. Toy model thermalizing in the condensed regime: with i.e.

  19. 50 quanta among 5 states 316 251 system states Start with Number of particles Total energy Thermal averages

  20. Integrate Calculate Do the approach the on the predicted time scale?

  21. PS + Q. Yang, PRL 103 (2009) 111301 Thermalization occurs due to gravitational interactions at time

  22. Gravitational interactions thermalize the axions and cause them to form a BEC when the photon temperature After that

  23. Tidal torque theory neighboring protogalaxy Stromberg 1934; Hoyle 1947; Peebles 1969, 1971

  24. Tidal torque theorywith ordinary CDM neighboring protogalaxy the velocity field remains irrotational

  25. Axions rethermalize before falling onto galactic halos and go to their lowest energy state consistent with the total angular momentum they acquired from tidal torquing provided i.e. Axion fraction of dark matter is more than of order 3%.

  26. Tidal torque theorywith axion BEC in their lowest energy available state, the axions fall in with net overall rotation

  27. Caustics of light at the bottom of a swimming pool on a sunny breezy day water surface pool bottom light intensity position

  28. DM forms caustics in the non-linear regime . . x x DM particles in phase space x x x x

  29. (from Binney and Tremaine’sbook)

  30. Galactic halos have inner caustics as well as outer caustics. If the initial velocity field is dominated by net overall rotation, the inner caustic is a ‘tricusp ring’. If the initial velocity field is irrotational, the inner caustic has a ‘tent-like’ structure. (Arvind Natarajan and PS, 2005).

  31. simulations by Arvind Natarajan in case of net overall rotation

  32. The caustic ring cross-section D -4 an elliptic umbilic catastrophe

  33. in case of irrotational flow

  34. On the basis of the self-similar infall model(Filmore and Goldreich, Bertschinger) with angular momentum (Tkachev, Wang + PS), the caustic rings were predicted to be in the galactic plane with radii was expected for the Milky Way halo from the effect of angular momentum on the inner rotation curve.

  35. Effect of a caustic ring of dark matter upon the galactic rotation curve

  36. Composite rotation curve(W. Kinney and PS, astro-ph/9906049) • combining data on 32 well measured extended external rotation curves • scaled to our own galaxy

  37. Inner Galactic rotation curve Inner Galactic rotation curve from Massachusetts-Stony Brook North Galactic Pane CO Survey (Clemens, 1985)

  38. Outer Galactic rotation curve R.P. Olling and M.R. Merrifield, MNRAS 311 (2000) 361

  39. Monoceros Ring of stars H. Newberg et al. 2002; B. Yanny et al., 2003; R.A. Ibata et al., 2003; H.J. Rocha-Pinto et al, 2003; J.D. Crane et al., 2003; N.F. Martin et al., 2005 in the Galactic plane at galactocentric distance appears circular, actually seen for scale height of order 1 kpc velocity dispersion of order 20 km/s may be caused by the n = 2 caustic ring of dark matter (A. Natarajan and P.S. ’07)

  40. from L. Chemin, C. Carignan & T. Foster, arXiv: 0909.3846 Rotation curve of Andromeda Galaxy

  41. 15.4 29.2 kpc 10.3 10 arcmin = 2.2 kpc

  42. L. Duffy & PS PRD78 (2008) 063508 The caustic ring halo model assumes net overall rotation axial symmetry self-similarity

  43. The specific angular momentum distribution on the turnaround sphere Is it plausible in the context of tidal torque theory?

  44. Tidal torque theorywith ordinary CDM neighboring protogalaxy the velocity field remains irrotational

  45. in case of irrotational flow

  46. Tidal torque theorywith axion BEC net overall rotation is obtained because, in the lowest energy state, all axions fall with the same angular momentum

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