Warped extra dimensions

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Warped extra dimensions NExT Meeting, Queen Mary, November 2011 Stephan Huber, University of Sussex

description

Warped extra dimensions. Stephan Huber, University of Sussex. NExT Meeting, Queen Mary, November 2011. Hierarchies from Warping. [Randall, Sundrum 1999]. 4D und 5D cosmological constants curve the extra dimension metric: Anti-de-Sitter (AdS) space ( AdS curvature k~M 5 ~M P ). - PowerPoint PPT Presentation

Transcript of Warped extra dimensions

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Warped extra dimensions

NExT Meeting, Queen Mary, November 2011

Stephan Huber, University of Sussex

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Hierarchies from Warping

• 4D und 5D cosmological constants curve the extra dimension

• metric: Anti-de-Sitter (AdS) space (AdS curvature k~M5~MP)

[Randall, Sundrum 1999]

warp factor all scales red shifted:

R~11k-1 : Meff(πR) ~ TeV hierarchy problem

localized gravity

πR

UV-brane V>0

IR-brane V<0

Λ<0

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KK Gravitons

• wave functions: sin, cos Bessel functions

• KK states are localized (IR-brane):

mass splitting ~ TeV

couplings ~ 1/TeV

(instead of 1/MP!)

spin-2 resonances at

colliders

m1 > ~ TeV, depending on k/MPl

no astrophysical constraints like in ADD

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IR-braneGraviton wave functions

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[Davoudiasl, Hewett, Rizzo hep-ph/0006041]

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Problems

• the SM is an effective theory with cut-off Λ• all mass scales get rescaled!

Λ ~ TeV

generic four-fermion operators

suppressed only by 1/TeV Q

Q

Q

L

proton decay (QQQL: >1015 GeV)flavor violation (DSDS: >106 GeV)neutrino masses (HHLL: >1014 GeV)…symmetries??

?

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Way out: SM in the bulk

• cut-off is y-dependent:

• electroweak scale Higgs: IR-brane

• gauge bosons, fermions: bulk

Higgsgauge bosons

fermions

IR-braneUV-brane

allows cut-off Λ >> TeV !

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IR-braneMain properties of gauge bosons:

-->

(0)

(2)

(1)almost universality:

FV suppressed

enhanced KK couplings:

large EW corrections

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Electroweak constraints

• W and Z mix with their KK excitations → SM mass relations modified at tree-level

MW somewhat enhanced (contribution to the ρ parameter)

MKK > 10 TeV (compared to an LHC reach of 5 TeV?)

• bounds can be relaxed to a few TeV by introducing a) brane kinetic terms [Carena, Ponton, Tait, Wagner] b) left-right symmetric gauge group [Agashe, Delgado, May,

Sundrum] c) bulk Higgs (soft wall?) [Cabrer, Gersdorff, Quiros] d) more than 5 dimensions [Archer, SH]

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More than 5 dimensions

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[Archer, SH]

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Fermion mass hierarchy

● zero modes: shape depends on 5D Dirac mass c

tau

electron

top

UV-Brane IR-brane

c>½ UV-brane

c<½ IR-brane

zero modes

● Yukawas λ(5) to the Higgs

● 5D geography: overlap

light (heavy) fermions UV (IR)-brane

hierarchical fermion masses with λ(5) ~ 1

Higgs

[Gherghetta, Pomarol; S.H., Shafi]

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Flavor violation

• KK gauge bosons couple

non-universally, so that

g=diag(ge,gμ,gτ)

• in the mass basis flavor non-diagonal couplings• but: couplings almost universal for c>1/2 where the light fermions are localized ‘‘warped GIM mechanism“

g (1)/g(0)

c

1. KK gauge boson

Z(1)

e

ee

µ

-->

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IR-braneMain properties of gauge bosons:

-->

(0)

(2)

(1)almost universality:

FV suppressed

enhanced KK couplings:

large EW corrections

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• strongest constraints from CP violation in the

Kaon system εK: mKK > ~30 TeV note: bounds are much weaker than for flat extra

dimensions, where mKK > 1000 TeV! [Delgado, Pomarol, Quiros 1999]

• lepton flavor violation: BR(µ→eee) ~ 10-13

(exp. bound: < 1x10-12)

BR(µ→eγ) ~ 10-16 (exp. bound: < 1.1x10-11) muon electron conversion BR(µN→eN) ~ 10-15

exp. bound: < 1x10-13 (but plans to reach ~10-17) → observable??

Flavor violation: examples

[Bauer, Casagrande, Haisch, Neubert 2009]

[Huber 2003]

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[Batell, Gherghetta, Sword ‘08]

(mKK~2 TeV, Falkowski, Perez-Victoria ‘08)

Mass scales:

AdS curvature k

KK scale µ

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Constraints from CP violation the kaon sector: much relaxed!

[Archer, SH, Jaeger 2011]

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Conclusions

Models with warped geometry provide a rich phenomenology:

new resonances (KK gravitons etc.) at colliders

fermion mass geography

main constraints: electroweak (RS: > ~10 TeV few TeV)

flavor (RS: > ~30 TeV few TeV)

results depend sensitively on variants of the model: more than 5D?

soft wall?

Warped models may be dual to strongly coupled 4D models

Cosmology: no immediate dark matter candidate

holographic phase transition

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KK Gravitons

• wave functions: sin, cos Bessel functions

• KK states are localized (IR-brane):

mass splitting ~ TeV

couplings ~ 1/TeV

(instead of 1/MP!)

spin-2 resonances at

colliders

m1 > 0.2-1.5 TeV, depending on k/MPl

no astrophysical constraints like in ADD

-->

-->

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IR-braneGraviton wave functions

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The Klebanov-Strassler solution10-dimensional metric:

“internal 5+1 dimensional metric:

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[Davoudiasl, Hewett, Rizzo hep-ph/0006041]

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Electroweak constraints

(you can also consider S und T parameter)

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Back to the Klebanov-Strassler solution

huge constraints!