dark matter at the ilc · dark matter at the ilc herbi dreiner bethe center for theoretical physics...
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Dark Matter at the ILC
Herbi Dreiner
Bethe Center for Theoretical Physics & Physikalisches Institut der Universität Bonn,! Germany
LHC-14, IFT, Madrid, Sept. 23rd, 2014
Work done in Collaboration with: Conley, Wienemann
Huck, Krämer, Schmeier, Tattersall
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Outline
1) Measuring a very light neutralino LSP mass at the ILC
2) Effective DM-operator analysis at the ILC
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I) Measuring a very light neutralino LSP mass at the ILC
If they exist, all SUSY Particles must be very heavy.
Text book knowledge:
LHC:
Every SUSY Particle?
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No, not EVERY SUSY particle!
The lightest Neutralino can still be massless!
= 0 very much allowedHeinemeyer, Kittel, Langenfeld, Weiglein, D: EPJC
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& ee J. List et al
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Question: LSP Mass
• Assume we discover SUSY at the LHC?
• Can we determine the LSP mass at the LHC?
• Yes, if it is heavy, larger than about 50 GeV
• How about a (very) light neutralino?
• Must go to ILC
• Note: if we measure: < 25 GeV
have excluded CMSSM neutralino DM!
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• Background: just introduced via efficiency
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H.U. Martyn
• Energy distribution: box
• Edges smeared out by experimental effects
• This example:
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• Yellow band: 30% uncertainty related to our simplified MC
Conley, Wienemann, HD
• Beam polarization: (e-,e+)=(+80%,-60%)
• Currently not possible to measure mass below 10 GeV!
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2) Effective DM-operator analysis at the ILCDaniel Schmeier, Jamie Tattersall, HD
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2) Effective DM-operator analysis at the ILCDaniel Schmeier, Jamie Tattersall, HD
• Relate to underlying UV theory
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Effective Approach
• DM interacts pairwise with SM fermions by single mediating particle
• For very heavy mediators obtain effective coupling Ge↵ =g�g M2
⌦
• Eff. field theory: can go beyond previous non-relativistic approach
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Some Assumptions
• DM is colorless, SU(2) singlet with no hypercharge
• DM particles interact with SM only via heavy mediator
• Obtain eff. theory by integrating out mediator, but do not consider UV complete theory
• Two scenarios:
1. All SM particles couple with same strength
2. Coupling proportional to mass: “Yukawa coupling”
• No resonances or co-annihilation in relic density comp.
• DM & mediator: Scalar, Dirac-Ferm. Maj.-Ferm. Vector
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Outline
The models —>
• Define models
• Choose benchmarks (too many models!)
• Consider ILC constraints:
• Xenon direct detection, ie need relic density
e+e� ! ��+ � Mono photons
• Pamela indirect detection (SI, SD)
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Benchmark Models
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ILC Study
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Backgrounds
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ILC Results
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Comparison Results: Spin Independent
• ILC good for light DM
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Comparison Results: Universal vs Yukawa
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Comparison Results: Spin Indep. vs Spin Dep.
• Spin dependent case, collider is strongest
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Fermions vs Leptons only
• DM coupling to nucleons loop-suppressed
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Contact Interactions @ LHC
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Summary
• Measuring light neutralino mass at ILC
• Eff. Operator DM Analysis at ILC
• Very light neutralino is allowed
e+e� ! e+e� ! e+e��01�
01• Measure mass via:
• Very accurate at high
• Impossible below about 5-10 GeV
�01 mass
• Eff. models describe int. with just 2 parameters:
• Polraisation can help reduce (some) background
• ILC can look for pair produced WIMPs via mono photons
• LHC limits can be improved by orders of magnitude
M� and Ge↵
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Backups
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