Marc Kamionkowski- New Views of Cosmology and the Microworld

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    New Views ofNew Views ofNew Views ofNew Views ofNew Views ofNew Views ofNew Views ofNew Views ofNew Views of

    Cosmology and thCosmology and thCosmology and thCosmology and thCosmology and thCosmology and thCosmology and thCosmology and thCosmology and th

    MicroworldMicroworldMicroworldMicroworldMicroworldMicroworldMicroworldMicroworldMicroworld

    arc am on ows

    (Caltech)

    SLAC Summer InstituAugust 16, 2002

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    Topics in Particle Astrophysics andI. Dark matter and relic particles

    II. Gamma rays and x rays(GLAST, STACE

    III. The CMB and inflationIV. Structure formation, cosmological par

    dark energy. Ultrahigh energy cosmic rays

    I. Gravitational radiationII. Neutrino astrophysics

    III. Early universe and tests of fundamen

    brane worlds and large extra dime

    (see, e.g., Akerib, Carroll, MK, Ritz,of P4 Working Group at Snowm

    hepph/0201178

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    Funda

    Forc

    100 GeV 101516

    GeV

    strong

    EM

    weak

    gravity

    ????

    electroweak

    GUT

    Energy

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    Astrophysics/cosmology and

    advances in fundamental physics;

    Keplers and Newtons laws

    Discovery of helium

    Serendipitous discovery of positrons, muons in

    Big bang nucleosynthesis and number of light

    Cosmological constraints to stable neutrino mSolar and atmospheric neutrinos and neutrino

    Astrophysical verifications of general relativity

    Eddington and bending of light

    expansion of Universe

    pulsar timing and gravitational waves

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    Physics with astrophysical

    neutrino masses and mixi

    solar and atmospheric ne

    SuperK

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    I. The Cosmic Microwav

    Background and Infl

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    Geometry

    Hubbleconstant

    Jungman, MK, Kosows

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    esults!!!Netterfield et al. (BOOMERanG) astroph/0104460 (also fro

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    Current results:

    show that Universe is flat

    determine primordial seeds for large scal

    independently verify big bang nucleosyntconfirm existence of nonbaryonic dark m

    suggest 70% of total energy density is so

    negative pressure dark energy (espe

    combined with dynamical measurem

    matter density of 30%)Physics is simple and peak structure is distincti

    so most results (especially for geomet

    ...show is not over!! What we have seen so far

    iceberg; MAP and Planck will improve precismeasurements by order of magnitude.

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    Th

    ebigbang!!!

    Nuc

    leosynthesis:

    n+p

    H,

    D,

    He,L

    i

    SecoT~M

    q

    uarksn,p

    103 sec

    T~100 MeV

    elec

    troweakEM

    ,weak

    109 sec

    T~100 GeV

    quantumg

    ravity,strings???

    10

    43

    secT~ 1019 GeV

    1036 sec

    T~ 1016 GeV

    GUT

    electrowea

    k,s

    trong??

    10

    22

    secT~ 1012 GeV

    PQsymmetrybreaking??

    SU

    SYbreaking??

    INFLATION

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    CMB tests of inflation:

    Recent CMB shows are on right trackWhat next? Determine energy scale o

    Inflation robustly predicts gravitation

    background with amplitude proportof energy scale of inflation (Abbott&W

    Detection of inflationary gravitational wav

    through CMB polarization can providgun" for inflation at GUT scale.

    (MK, Kosowsky, Stebbins 1997; Seljak,Zald

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    Gr

    avitationalW

    aveAmplitud

    e

    (Energyscale

    ofinflation)

    2

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    Gravitational waves: Another probe of the inflato

    GW amplitude h()

    C

    W

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    Brief aside: CMB detection of Brief aside: CMB detection of

    violation from Planck scale phviolation from Planck scale ph

    (Lue, Wang, MK, 1999)

    Certain cross correlations between temperat

    polarization components can arise only if pa

    FF~

    RR

    Two examples: Rolling scala

    with P,T viol

    to EM

    P,T violating couplingto gravity can produce

    preponderance of right

    versus left handed GWs

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    II. Large scale structure and

    Inflatonpotential

    Ma

    spe

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    Galaxy megasurveys now mapping

    mass distribution over huge volumes (2

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    Forecast

    SDSS

    Power

    Spectrum

    CD

    Mo

    h=0.5

    h=0.2

    (as

    bia

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    Dodelson et al. (SDSS Collaboration) ApJ (2

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    Cosmic Shear

    First detection (by several indgroups) of "cosmic shear", weagravitational lensing due to

    large scale mass inhomogenei

    Probes largescale distributio

    rather than ofgalaxies.

    ...and mapping of dark matter aro

    has become routine.

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    Possible, e.g.

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    Inflation: What Else??

    Inflation distribution of primdensity perturbations is

    Can be checked with CMB mapssurveys, weak lensing, cluster

    abundances, abundances of

    highredshift objects, clusterproperties....

    (e.g., Verde et al., 2

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    Ra

    fo

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    III. Sup

    an acce

    Univers

    Dark E

    1998

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    Courtesy P. Garnavich (Highz Supernova Se(results also from Supernova Cosmology Pr

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    Quintessence:

    V()

    Spintessence:

    (Boyle, MK,Caldwell 2001)

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    Qu(sp)intessence! Other connections:

    "Vacuum" is CPT and Lorentz violatinand may contain global charge

    May drive baryogenesis and/or hide aCould rotate polarization of distant ra

    if scalar field coupled to EMCan reproduce and generalize (e.g., to

    quartic terms in potential) fuzzy cold

    matter

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    III. Particle Dark Matter S

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    Earth

    (r

    density

    r

    r0=8 kpc

    Veloc

    distrib

    With

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    Particle dark matter cand

    Weakly Interacting Massive

    Particles (WIMPS).

    e.g.,neutralinos

    Axions

    ma~104

    v

    cmh

    sec/103

    327

    2

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    WIMPsWIMPsThe relic density of a massive particle is about:

    vh

    1327

    2 scm103

    v OfWeak Interaction strength

    the particle has to be coupled to SM particleThere is chance for detection:

    Detection

    direct

    indirect

    Ne

    from

    ano

    cosm

    WIMP candidate motivated by SUSY:

    Lightest Neutralino, LSP in MSSM

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    Particle dark matter

    searches (axions

    and SUSY particles)

    See

    dmtools.berkeley.edu

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    Spin depende

    WIMPproto

    Spin dependent

    WIMPneutron coupling

    Ullio,

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    Searches for SUSY dark m

    Direct detection inlow background detectors

    Indirect de

    via energefrom LSP a

    in Sun/Ea

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    Detection of SUSY dark

    Indirect detection via observation

    gamma rays from LSP annihilatio

    E.g., in GLAST, VER

    Whipple, CELESTE,

    Or via observation of exotic cospositrons or antiprotons (e.g., iPBAR, AMS....)

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    Axionsearch (Livermore) (courtes

    Scanned already Next year

    Ac

    wi

    (~

    ow ca

    these h

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    Self interacting dark ma

    Cluster

    galactichalo

    Moore et a

    also Klypin

    ph/99012

    Kaufmann

    Guiderdon300 kpc

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    Probably dont need self interactRequires very unusual particles

    scattering cross sections 13 ordmagnitude bigger than annihila

    Not really clear that self interac

    improves agreement with obsMay be due to other exotic proc

    Broken scale invariance in primpower spectrum (MK, Liddle 2

    Absence of small scale structuremost likely due to prosaic astro

    mechanism

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    MK,Liddle (2000)

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    IV. Tests of strongfield gravity:

    Gravitational waves from stellar or

    supermassive black holes (e.g., wit

    X ray timing and spectroscopy from

    disks around supermassive black h

    (RXTE, Chandra, XMM, ConX,GL

    other interesting tests with grav ra

    can test whether gravitational wav

    at speed of light (extra dimensionsmight not!!)

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    Possible detection of effects

    black hole spin on surro

    spacetime!!!

    P. Nandra

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    Gravitational Radi

    Orbiting and merging massive

    objects emit gravitationalradiation

    Two biggest experiments aimigravity waves:

    LISA(spacebasLIGO(groundbased, under construction)

    firstlock at Hanford

    Oct 2000

    4km

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    Possible detection of cosmic

    above GZK cutoff!!!(p + p + ) 30 pc for E

    p 1020 eV,

    but no obvious sourceswithin ~30 Mpc also no

    dramatic cutoff inspectrum near 1020 eV.

    HiRes also seeing events

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    Ultrahighenergy cosmic rays:

    Existence of cosmic rays aboveGreisenZatsepinKuzmin limit su

    propagation of exotic particle and/

    of topological defects or ultrama

    particles. Interactions in atmospheinclude interesting QCD.

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    UHE Cosmic Ray TecNitrogen Fluorescence

    Air Shower

    ~0Ground ArrayAGASA

    ~3Fluor.OWL

    8Fluor.Telescope

    Array

    7

    ( x2

    Ground Array

    + Fluor.

    Auger

    ~1Fluor.HiRes

    Ef

    [10TechniqueExperiment

    OW

    L

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    More:

    Astrophysical probes of large extra dimLorentz/CPT violation...

    Astrophysical tests of general relativity (

    Shapiro time delay, radio deflection

    ranging...Theoretical ultrahigh energy physics: the

    Universe as a laboratory for string t

    PQ symmetry breaking, GUTs, SUSY

    extra dimensions....

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    Conclusions/Summar

    Astrophysics and cosmology are often difficult

    BUT, can in some cases provide real opportuni

    to probe new physics not accessible with accel

    Its a good time for cosmology and particle astrplenty of exciting discoveries and breakthroug

    rich frontier; healthy interplay between theory

    prospects for rapid order of magnitude experim

    in many areas.

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