38
Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 1 Supersymmetry in Particle Physics and Cosmology

Supersymmetry in Particle Physics and Cosmologydeboer/html/Talks/... · Particle Physics: Unification. Cosmology: Dark Matter. Supersymmetry in Particle Physics and Cosmology. Wim

  • Upload
    others

  • View
    3

  • Download
    0

Embed Size (px)

Citation preview

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 1

    Supersymmetry in Particle Physics and Cosmology

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 2

    Outline:

    Particle Physics: UnificationCosmology: Dark Matter

    Supersymmetry in Particle Physics and Cosmology

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 3

    Unification with precisely measuredcoupling constants at LEP (1991)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 4

    Fit results

    GUT scale ≈1016 GeV(above proton decay limit)

    SUSY scale ≈103 GeV(above proton decay limit)

    Unification excluded in SM

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 5

    mSUGRA: need to solve 28 coupled differential RGEs(From W. de Boer, Review, hep-ph/9402266)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 6

    Mathematics is beautiful

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 7

    On the 1000+ citation list..

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 8

    Global electroweak fits and gauge coupling unification.Wim de Boer, Christian Sander

    PLB 585(2004)276 hep-ph/0307049

    ALR (SLAC)

    LEP

    αs fromhadronic x-sect

    αs fromhadronic/leptonic

    Z0 branching ratio

    A few 2-3 σ deviations happens to be in coupling constants

    Discrepancy in αsgoes away, if one

    requires3.0 neutrino generationsinstead of 2.98 from fit

    Believe αs = 0.122 is correct

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 9

    Center of the Coma Cluster by Hubble space telescope ©Dubinski

    Discovery of DM in 1933Zwicky(1898-1974 )

    Zwicky notes in 1933 that outlying galaxies in Coma cluster moving much faster than expected from visible mass. His conclusion: 90% of mass is “Dark Matter”

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 10

    Confirmation by WMAP observing acoustic waves of early universe

    Early Universe

    Present Universe

    The Cosmic screen

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 11

    Solution:pressure small: δ=aebt , i.e. exponential growth of δ(->gravitational collapse)pressure large: δ=aeibt , i.e. oscillation of δ (acoustic waves)

    Define: δ=Δρ/ρ

    From Newton`s F=ma:δ``+ (pressure-gravity) δ=0

    Why acoustic waves in early universe?

    FG

    PF=ma

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 12

    Three basic problems with DM1.Why it is there?

    2.Why so little, i.e. np≈nχ

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 13

    Expansion rate of universe determines WIMP annihilation cross section

    Thermal equilibrium abundance

    Actual abundance

    T=M/22Com

    ovin

    g nu

    mbe

    r den

    sity

    x=m/TGary Steigmann

    WMAP -> Ωh2=0.113±0.009 ->=2.10-26 cm3/s

    DM increases in Galaxies:≈1 WIMP/coffee cup ≈105 .

    DMA (∝ρ2) restarts again..

    T>>M: f+f->M+M; M+M->f+fTf+f

    T=M/22: M decoupled, stable density(when annihilation rate ≅ expansion-rate, i.e. Γ=nχ(xfr) ≅ H(xfr) !)

    Annihilation into lighter particles, likequarks and leptons -> π0’s -> Gammas!

    Only assumption in this analysis:WIMP = THERMAL RELIC!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 14

    Example of DM annihilation (SUSY)

    Dominant χ + χ ⇒ A ⇒ b bbar quark pairSum of diagrams should yield

    =2.10-26 cm3/s to getcorrect relic density

    Quark fragmentation known!Hence spectra of positrons,

    gammas and antiprotons known!Relative amount of γ,p,e+ known

    as well.

    χ

    χ

    χ

    χ

    χ

    χ

    χ

    χ

    χ

    χ

    f

    f

    f

    f

    f

    f

    Z

    Z

    W

    Wχ± χ

    0

    f~ A Z

    ≈37 gammas

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 15

    Thermal relics can annihilate with cross section as large as =2.10-26 cm3/s -> enormous rate of gamma rays

    from π0 decays (produced in quark fragmentation)(Galaxy=1030 higher rate than any accelerator)(109 bbbar pairs produced in 10-20 s, B-factory needs 5 y)

    Expect large fraction of energetic Galactic gamma rays to come from DMA in this case. Remaining ones from pCR+pGAS-> π0+X , π0->2γ (+some IC+brems)

    This means: Galactic gamma rays have 2 componentswith a shape KNOWN from the 2 BEST studied reactionsin accelerators: background known from fixed target exp.

    DMA known from e+e- annihilation (LEP)

    Conclusion sofar

    Data driven and model independent analysis possible byfitting signal and background shape in each sky direction ->

    DM distribution in whole sky independentof model for profile or model for background

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 16

    Usual astrophysicist’s search strategies

    Particle physicist: get rid of modeldependence by DATA DRIVEN calibration

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 17

    Sundisc

    Basic principle for indirect dark matter searches

    R

    Sun

    bulge disc

    From rotation curve:

    Forces: mv2/r=GmM/r2or M/r=const.for v=cons.

    andρ∝(M/r)/r2ρ∝1/r2

    for flat rotation curve

    Expect highest DM densityIN CENTRE OF GALAXY

    IF FLUX AND SHAPE MEASURED INONE DIRECTION, THEN FLUX AND

    SHAPE FIXED IN ALL SKY DIRECTIONS!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!!

    R1

    THIS IS AN INCREDIBLE CONSTRAINT, LIKE SAYING I VERIFYTHE EXCESS AND WIMP MASS WITH 180 INDEPENDENT MEAS.

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 18

    Background + signal describe EGRET data!

    Blue: background uncertainty

    Background + DMA signal describe EGRET data!

    Blue: WIMP mass uncertainty

    50 GeV

    70

    Brems .

    ICWIM

    PS

    π 0

    IC

    π0 WIM

    PS

    Brems .

    IC

    Fitted known shapes of background and DMA (from accelerator experiments) with free normalizations. W. de Boer et al., A&A (2005)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 19

    180 skydirections:80 in longitude ⇒ 45 bins

    4 bins in latitude 4x45=180 bins -> >1400 data pts

    Every direction has different gas and DM density, so fluxes change

    in every direction

    Chi2/d.o.f. summed over all directions EQUALS ONE, i.e. DM

    constraints w.r.t. shape and intensity fullfilled!!!!

    2-parameter fits in 180 different sky directions

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 20

    Halo density on scale of 300 kpc(from normalization factors in 180 sky directions)

    Sideview Topview

    Cored isothermal profile with scale 4 kpcTotal mass: O(1012) solar masses

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 21

    Halo density on scale of 30 kpc

    Sideview Topview

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 22

    The Milky Way and its 13 satellite galaxies

    Canis Major

    Tidal force ∝ ∆FG ∝ 1/r3

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 23

    N-body simulation from Canis-Major dwarf galaxy

    prograde retrograde

    Obs

    erve

    d st

    ars

    R=13 kpc,φ=-200,ε=0.8

    Canis Major (b=-150)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 24

    EGRET Excess predicts shape of rotation curve!

    Outer Ring

    Inner Ring

    bulge

    disk

    Rotation Curve

    Normalize to solar velocity of 220 km/s

    R0=8.3kpc

    R0=7.0v

    R/R0

    Innerrotationcurve

    Outer RC

    Black hole at centre: R0=8.0±0.4 kpc

    Sofue &Honma

    Note 1: Absolute value of rotation curve depends on distances.

    But chance of slope can ONLYbe explained by ringlike structure.

    Note 2: fact that shape of DM halocan describe shape of RC implies

    that EGRET excess has exactly rightintensity to deliver grav. potential!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 25

    Gas flaring in the Milky Way

    no ring

    with ring

    P M W Kalberla, L Dedes, J Kerp and U Haud, A&A 469(2007) 511,arxiv.org/0704.3925

    Gas flaring needs EGRET ring with mass of 2.1010M☉!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 26

    The dark connection between Canis Major, Monoceros Stream, gas flaring, the rotation curve and the EGRET excess

    EGRET excess ->• WIMP mass• WIMP halo

    (= standard halo + DM rings)WdB, C.Sander, V.Zhukov, D.Kazakov,

    A.Gladyshev,A&A, 444 (2005) 51

    Confirmation:

    • Rotation curve• Canis Major/Monoceros stream• Gas flaring

    Objections

    • EGRET data wrongly calibrated?• Antiproton flux too high?• Extragal. gamma rays inconsist.?

    Physics = correlationsRichard Feynman

    Gamma spectra for BG + DMAParticle Physics

    Cosmology

    Astroparticle-physics

    23%DM, Annihilation x-section

    Tidal streams

    CosmicsGamma rays

    AstronomyRotation curveDwarf galaxies

    Gas flaring

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 27

    With convection Without convection

    Comparison of propagation modelsincluding convection

    Summary: preferred propagation perp. to disk reduces contribution of charged particles from DMA by large factor

    and can be consistent with B/C and 10Be/9Be

    (Bergstrom, Edsjo, Gustafssonand Salati, JCAP, astro-ph/0602632)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 28

    NATURE 452, 17. April 2008, “Blown away by cosmic rays”, D.Breitschwerdt

    NGC 253

    Fit to ROSAT data,Everett et al.

    arXiv:0710.3712v1

    Cosmic Rays (CR) form a plasma. If blowing in a given direction,it will take other particles with it, thus exerting pressure.

    This CR pressure drives all halo particles to intergalactic space,thus reducing strongly the flux of charged particles from DMA.

    Convection observed between 100 and 3000 km/s, thus dominating over diffusion in the disk region

    http://arxiv.org/abs/0710.3712v1

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 29

    a“Observation of an anomalous positron abundance

    in the cosmic radiation“, PAMELA, arXiv:0810.4995

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 30

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 31

    Lots of speculation about increase in positron ratio

    But simple isotropic propagationsmodels WRONG?Or do propagation uncertainties cancel in ratio? NO!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 32

    AMS-01 p/e ratio increases

    AMS-01 Data from Shuttle Flight in 1998Positrons from π+ production by protons

    Electrons from Supernovae. Increasing p/e ratio -> increasing,e+/e- ratio? YES, EASY!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 33

    Propagationmodel compatible with EGRET, ROSAT, INTEGRAL, WMAP, AMS

    Energy [GeV]

    -310 -210 -110 1 10 210 310

    ep

    /e+

    ep

    -410

    -310

    -210

    -110

    1

    averaged data

    total

    DM

    Data from Chung et al,arXiv:0710.2428v1

    PositronFractione+/(e++e-)

    WdB,arXiv:0810.1472Anisotropic propagationmodel

    compatible mit EGRET, ROSAT,INTEGRAL, AMS, WMAP ->easily increase in e+/e- ratio

    Expect only tiny DM contribution, because of convection andlarge background fromlight pion production

    DMA signal NOT in positrons, but.

    in Pamelas antiprotons!!!

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 34

    What aboutSupersymmetry?

    Assume mSUGRA5 parameters: m0, m1/2, tanb, A, sign μ

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 35

    Expected SUSY mass spectra in mSUGRA

    mSUGRA: common masses m0 and m1/2 for spin 0 and spin ½ particles

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 36

    Gauge unification perfect with SUSY spectrum from EGRET

    SUSY spectrum from EGRET/LEP->perfect gauge coupling unification!

    Upd

    ate

    from

    Amaldi, dB

    ,Fü

    rste

    nau,

    PLB

    260

    199

    1

    SM SUSY

    Also b->sγ and g-2 agree within 2σ with SUSY spectrum from EGRET

    NO FREEPARAMETERS

    WdB, C. Sander,PLB585(2004). e-Print: hep-ph/0307049

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 37

    Dark matter, what is it?

    EGRET excess shows an intriguing hint, that DMis an annihilating thermal relic from the early universe!

    Its properties are perfectly consistent with SUPERSYMMETRY, in which case

    LHC experiments will tell! Expect: squarks & sleptons heavy (>1 TeV)

    gauginos light (50-500GeV)

  • Wim de Boer, Karlsruhe Memorial Conference in Honor of Julius Wess, Munich, 6-7.11.2008 38

    Discovery of the new world of

    SUSY

    Back to 60’s

    New discoveries every year

    Superparticles

    Slide Number 1Slide Number 2Slide Number 3Slide Number 4Slide Number 5Slide Number 6Slide Number 7Slide Number 8Slide Number 9Slide Number 10Slide Number 11Slide Number 12Expansion rate of universe determines �WIMP annihilation cross sectionExample of DM annihilation (SUSY)Slide Number 15Slide Number 16Slide Number 17Slide Number 18Slide Number 19Slide Number 20Slide Number 21Slide Number 22Slide Number 23Slide Number 24Slide Number 25Slide Number 26Slide Number 27Slide Number 28aSlide Number 30Slide Number 31Slide Number 32Slide Number 33Slide Number 34Slide Number 35Slide Number 36Slide Number 37Slide Number 38