sussex 22.8.2007 the wimp of a minimal walking technicolor theory j. virkajärvi jyväskylä...
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Sussex 22.8.2007
The WIMP of a minimal walking Technicolor Theory
J. VirkajärviJyväskylä University, Finland
with K.Kainulainen and
K.Tuominen
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Outline• Technicolor and the WIMP
• Dynamical Dark Energy and the WIMP density
• Model results
• Conclusion & outlook
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Basic idea of Technicolor (TC)
Technifermion condensate = a composite Higgs
(+ (pseudo) Goldstone bosons)
• New gauge interaction TC which only technifermions feel
• Left and right handed fermions (massless) have SU(2) chiral symmetry
• Spontaneus symmetry breaking dynamicallyElectroweak symmetry breakingRight mass ratio for EW gauge bosons
Early UniverseHigh TemperatureT > TeV
Universe expands,T drops
GeVTEW 175
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• Model: Two techniquarks(flavors) in two index symmetric (= adjoint) presentation of an SU(2) TC gauge group.
• Witten anomaly cured by introducing a new Heavy lepton family
Minimal Walking TC (WTC)
2121 ,, , ccR
ccR DU
L
cc
cc
D
U
},{
},{
21
21
LN
Heavy Neutrino = the WIMP
• Near conformal (=walking) FCNC’s suppressed.
• Compatible with EW precision measurements
(Sannino & Tuominen, hep-ph/0405209)
(Pure Majorana case)
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Heavy neutrino mass term• Dirac mass term for charged lepton
• For neutrino three cases:
1. Pure Dirac mass term ( )
2. Pure Majorana mass term (M)
3. Mixed Dirac-Majorana mass term:
..0
2 chm
mML C
R
L
D
DR
CLmass
Thermally averaged annihilation cross section:
MAJORANAPURENMIXED vv 4)( sin
1
decays to = the WIMP 2N 1N
Diagonalize two Majorana particles: and (mass eigenstates) for which and21 mm
1N 2N
Dm
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EW precision measurements
Neutrino
Charged lepton
• Model consistent with data (hep-ex/0509008) .• Oblique parameters S and T (Peskin & Takeuchi, PRD 46 (1992)).
Pure Majorana
12 2 mm Similar results in Pure Dirac and mixed cases
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• Quintessence:
• Dark energy dominates the energy density at early times
Dynamical Dark Energy
• Dark Energy
• Dark Matter
• Baryonic Matter
20.0~N
76.0~
04.0~B
)(2
1QVQQLQ
0)(33
QH
QVQHQ
63 i.e. aaQ Q 4 arad SM only radiation
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”0” means T = 1MeV
• Relic density from Lee Weinberg equation
• Biggest effects to final abundance of the heavy neutrinos comes from the cross section and Hubble parameter
)()()( 2
eq2
2
xfxfH
xmv
x
xf N
Exponentialdrop
Freeze out
Relic density and dynamical dark energy
)()()( 2
eq2
2
xfxfH
xmv
x
xf N
Number density
3*
23/1
)(45
2 , ,
)()( TTgs
m
sx
s
xnxf
N
SUSY and Our mixed D-M mass case
Our Model
6
0
4
00,3
8
a
ar
a
ah
GH rad
N
”0” means T = 1 MeV
6 aQ4 aradSM
0,
0,
rad
Qr
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Model results
contours const.~N
)0(1009.1 6 famNN
Both cases compatible with nucleosynthesis since r small (for masses shown).
Pure Dirac Pure Majorana
Majoranafor 2
1
Diracfor 1
a
a
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Model resultsMixed Dirac-majorana case:
410rDotted:
Dashed: 710r
Solid: Standard expansion
0r
contours const.~N
2
32
4 41sin308,0
Zm
mN
Yellow areaExcluded by LEP:
Similar results by Kouvaris:(hep-ph/0703266)for neutral bound state betweentechniquark and technigluon
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Constraints to results• Direct search limits
Bound depends on the ratio between local and cosmic WIMP densities
0/ nnk G
• Limit from rotation curves + halo models: lower bound for local density 3
06.0cm
GeVG
(Jungman, Kamionkowski, Griest, Phys. Rept. 267)
Pure DiracPure Majorana,(mixed D-M)Upper limits for ),( kmNN
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Conclusion and outlook• If a Quintessence-like Dark Energy dominates the early
universe evolution– 4th generation dirac neutrino (from MWTC) with m < 800 GeV is excluded– Majorana neutrino with m > 100 GeV candidate for dark matter: not excluded by direct searches
• In standard expansion case from mixed Majorana-Dirac mass term– Mainly right handed Majorana neutrino with m > 23 GeV candidate
for dark matter: not excluded by LEP or direct searches.
• Further studies:– Other CDM in extensions of MWTC– Replacing Quintessence with more advanced DE models