pierre sikivie- dark matter caustics

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  • 8/3/2019 Pierre Sikivie- Dark Matter Caustics

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    Dark MatterCaustics

    Pierre Sikivie(U of Florida)

    Miami 2007

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    Elucidating the structure ofgalactic halos is important for

    - understanding galactic

    dynamics

    - predicting signals for dark

    matter searches

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    WIMP detectors

    CDMS Xenon

    Also: DAMA, Edelweiss, CRESST, ZEPLIN,

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    WIMP nucleus elastic scattering

    ionization, scintillation, phonons

    v

    v)(vkm/s)220(

    2)(

    )(vmin

    fdET

    rE

    r

    =

    )()(0 rr

    ETqFdE

    dR

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    Axions

    solve the Strong CP Problem of the

    Standard Model

    are a cold dark matter candidate when

    mass

    require only a gentle modification of

    the Standard Model

    are detectable by the cavity technique

    5

    10 eVam

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    Axion Dark Matter eXperiment

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    2 21

    2)ah m c = (1 +

    1

    aQ

    1

    LQ

    dP

    d

    2/am hc

    0Bur

    a

    X

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    ADMX

    has reached sufficient sensitivity to detect galactichalo axions in favorable cases (KSVZ coupling)

    is being upgraded with SQUIDs (50 mK

    noise temperature vs. 2 K with HEMTs)

    when cooled to 50 mK, will have sensitivity

    to detect dark matter axions at even a fraction of

    the halo density. The remaining challenge will

    be to extend the searchable mass range.

    if a signal is found, will be able to measure the local

    CDM velocity distribution in detail

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    Galactic halos live in phase space

    ordinary fluid

    dark matter (collisionless) fluid

    );( trdr

    );(v trrr

    );v,( trfrr

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    Galactic halo models

    Isothermal sphere late infalling particles

    do not thermalize

    N-body simulations present resolution

    is inadequate

    Caustic ring model

    complaintmodel

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    x

    x.

    Dark matter particles are red and,on this page, they are free.

    Caustics in cold dark matter

    x

    xx

    dd

    .x

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    Phase space distribution of CDM

    in a homogeneous universe

    z

    z

    .

    ztHz )(=& v

    -1710v =-12

    10v =

    for axions

    for WIMPs

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    The cold dark matter particles lie on

    a 3-dimensional sheet in6-dimensional phase space

    the physical

    density is theprojection ofthe phase

    space sheetonto positionspace ( , t) = t) ( , t)r r rv v( +

    ur r r ur r

    z

    z.

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    The cold dark matter particles lie on

    a 3-dimensional sheet in6-dimensional phase space

    the physical

    density is theprojection ofthe phase

    space sheetonto positionspace ( , t) = t) ( , t)r r rv v( +

    ur r r ur r

    z

    z.

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    Phase space structure ofspherically symmetric halos

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    Implications:1. At every point in physical space, the

    distribution of velocities is discrete, eachvelocity corresponding to a particular flow

    at that location .

    2. At some locations in physical space, where

    the number of flows changes, there is acaustic, i.e. the density of dark matter is veryhigh there.

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    - the number of flows at our location in the Milky Way halo

    is of order 100

    - small subhalos from hierarchical structure formation

    produce an effective velocity dispersion

    but do not destroy the sheet structure in phase space

    - the known inhomogeneities in the distribution of matter are

    insufficient to diffuse the flows by gravitational scattering

    - present N-body simulations do not have enough particles to

    resolve all the flows and caustics(see however: Melott and Shandarin; Stiff and Widrow; Shirokov and Bertschinger;

    Vogelsberger, White, Helmi and Springel)

    effv 30 km/s

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    Hierarchical clustering introduces effective

    velocity dispersion

    effv

    effv 30 km/s

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    - the number of flows at our location in the Milky Way halo

    is of order 100

    - small subhalos from hierarchical structure formation

    produce an effective velocity dispersion

    but do not destroy the sheet structure in phase space

    - the known inhomogeneities in the distribution of matter are

    insufficient to diffuse the flows by gravitational scattering

    - present N-body simulations do not have enough particles to

    resolve all the flows and caustics(see however: Melott and Shandarin; Stiff and Widrow; Shirokov and Bertschinger;

    Vogelsberger, White, Helmi and Springel)

    effv 30 km/s

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    (from Binney and Tremaines book)

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    Phase space structure ofspherically symmetric halos

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    Galactic halos have inner caustics aswell as outer caustics.

    If the initial velocity field is dominated by netoverall rotation, the inner caustic is a tricusp ring.

    If the initial velocity field is irrotational, the innercaustic has a tent-like structure.

    (Arvind Natarajan and PS, astro-ph/0510743).

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    simulations by Arvind Natarajan

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    The caustic ring cross-section

    an elliptic umbilic catastrophe

    D-4

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    Galactic halos have inner caustics aswell as outer caustics.

    If the initial velocity field is dominated by netoverall rotation, the inner caustic is a tricusp ring.

    If the initial velocity field is irrotational, the innercaustic has a tent-like structure.

    (Arvind Natarajan and PS, astro-ph/0510743).

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    Effect of a caustic ring of dark matter upon

    the galactic rotation curve

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    On the basis of the self-similar infall model

    (Filmore and Goldreich, Bertschinger) with angularmomentum (Tkachev, Wang + PS), the causticrings were predicted to be

    in the galactic plane

    with radii

    was expected for the Milky Wayhalo from the effect of angular momentum

    on the inner rotation curve.

    ( )1,2,3...n =

    rot max40kpc v j

    220km/s 0.26n

    na =

    26.0jmax

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    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

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    Inner Galactic rotation curve

    Inner Galactic rotation curve

    from Massachusetts-Stony Brook North Galactic Pane CO Survey (Clemens, 1985)

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    from W.B. Burton and W.W. Shane, 1970

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    Outer Galactic rotation curve

    R.P. Olling and M.R. Merrifield, MNRAS 311 (2000) 361

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    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 planeat galactocentric distanceappears circular, actually seen forscale height of order 1 kpc

    velocity dispersion of order 20 km/s

    Natarajan and P.S. (arXiv: 0705.0001) identify twoprocesses through which the Monoceros Ring of starsmay have formed as a result of the presence of thesecond caustic ring of dark matter in the Galaxy

    20 kpcr 0 0100 270l