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Title: Search for ExtraDimensions at pp and ep Colliders


1
Search for Extra-Dimensionsat pp and ep
Colliders
_
  • Eric Kajfasz, CPPM/D0
  • kajfasz_at_cppm.in2p3.gov
  • for the CDF, D0, H1 and Zeus collaborations

2
Extra Dimensions Outline
  • Extra Dimension Models and Signatures studied at
    CDF D0 Run II, H1 and ZEUS
  • Preliminary results on virtual graviton/gauge
    boson exchange and direct graviton emission
  • Summary and Conclusions
  • Why ED?
  • come naturally with string theory
  • provide mechanism to explain why MEW ltlt MPL
  • ...

3
Extra Dimensions Models Explored
  • focus on n extra dims in models where SM fermions
    live on a D3-brane
  • Large Extra Dimensions (LED) Arkani-Hamed,Dimopoul
    os,Dvali Phys Lett B429 (98)
  • MPL 1019GeV
  • n gt 2 compact and flat - MS
    string/fundamental scale M2PL Rn MSn2 gt MS
    can be lowered to TeV scale
  • gravitons propagate in the bulk gt Kaluza-Klein
    tower G(k)
  • cant resolve successive modes (0.01eVn2
    1MeVn3 100MeVn6)
  • gt expect
  • virtual exchange of graviton KK modes
  • real graviton emission
  • TeV-1 Extra Dimension (TeV-1) Dienes,Dudas,Gherghe
    tta Nucl Phys B537 (99)
  • MC compactification scale ( TeV)
  • gauge fields can propagate in the bulk gt KK
    towers of gauge bosons
  • modes with nearly equal energy spacing TeV
  • lower GUT scale by changing running of the
    couplings
  • gt expect
  • resonances at high energies (LHC ...)
  • virtual exchange (Hera, Tevatron)

4
Extra Dimensions Models Explored ...
  • Warped Extra Dimension (RS) Randull,Sundrum Phys
    Rev Lett 83 (99)
  • ED of size R, highly curved, compactified on
    S1/Z2 orbifold y Rf.
  • Zero mode graviton G(0) localized at the
    Planck-brane (y 0)
  • SM fields localized on TeV-brane (y Rp)
  • metric ds2 e-2kRf hmndxmdxn R2df2
    k curvature scalefor kR 11-12, Lp
    MPLe-kRp TeV
  • consistency gt 0.01 lt k/MPL lt 0.1
  • Gravitons propagate in the bulk gt KK tower G(n)
    of modes of mass mn xnke-kRp (xn 1st Bessel
    func. zeros i.e. 3.83, 7.02, 10.17, ...)gt well
    separated modes
  • Lp m1MPL/(kx1) gt model characterized by m1 and
    k/MPL
  • gt Look for first graviton resonance

5
Extra Dimensions Topologies Explored
Exchange Virtual Gravitons (LED,TeV-1,RS)
Tevatron
Hera
G
jet(s) MET g MET
Emission of Real Gravitons (LED)
q
g(jet),g
Tevatron
6
Large Extra DimensionsVirtual Graviton Exchange
dilepton channel (Tevatron)
SM
SM
diphoton channel (Tevatron)
DIS channel (Hera)
SM
7
Large Extra DimensionsVirtual Graviton Exchange
s sSM hGsint hG2sKK
  • Effect of ED parameterized by a single
    variable
  • different formalisms have different definitions
    of MS
  • Hewett (Hewett, Phys Rev Lett 82, 4765 (99) )F
    2l/p with l 1
  • GRW (Giudice, Rattazzi, Wells, hep-ph/9811291)F
    1
  • HLZ (Han, Lykken, Zhang, hep-ph/9811350)F
    log(MS2/s) for n 2F 2/(n-2)
    for n gt 2

hG F/ MS4
8
Large Extra Dimensions Virtual Graviton Exchange
ee
  • 2 isolated es, ETgt 25 GeV
  • es coming from luminous region
  • MET significance cut
  • eCC 92.4 0.4 eCP 79.2 0.5
  • for Mee gt 350 GeV Nexp 4.6, Nobs 8
  • Mee distrib. used in binned likelihood gt Limits
    on hGl/MS4

CCCP
95 CL limits on MS (TeV)
Mee
C(entral) hlt1 P(lug) 1lthlt3
9
Large Extra Dimensions Virtual Graviton Exchange
diEM
  • diEM combine ee and gg
  • 2 EM objects, ET gt 25 GeVwith track isolation
  • overall ID efficiency 85 1
  • for MdiEM gt 350 GeVNexp 9.7 (1.6 QCD), Nobs
    8
  • Systematics 12

200pb-1
CC-CC CC-EC
signal for hG 0.6
D-Y direct gg QCD
QCD
CC-CC CC-EC
CC hlt1.1 EC 1.5lthlt2.4
10
Large Extra Dimensions Virtual Graviton Exchange
diEM
  • Data agree with SM predictions gt
  • MdiEM vscosq distrib. usedin 2D Binned
    Likelihood
  • gtSet limits on hG alone orin combination with
    Run I results
  • gt give 95 CL limits on MS (TeV)
  • Most stringent constraints on LED for n gt 2 to
    date among all experiments.

200pb-1
11
Large Extra Dimensions Virtual Graviton Exchange
mm
  • 2 ms with PT gt 15 GeV
  • isolated, hlt2.0
  • cosmic veto
  • Mmm gt 50 GeV
  • for Mmm gt 300 GeVNexp 6.4 and Nobs 5
  • Systematics 13

D0 RunII Preliminary
Mmmvscosq distr. used in 2D Binned
Likelihood gt Set limits on hG gt 95 CL limits
on MS (TeV)
250pb-1
12
Large Extra DimensionsHERA Virtual Graviton
Exchange
G(k) Virtual exchange in t-channel interferes
with Deep Inelastic Scattering (DIS) Small
contribution O(1) from eg -gt eg G(k)
exchange affects the Q2 distribution at high Q2
Compare ds/dQ2 to what is expected from SM
Q2 (k-k)2 -q2
,KK
13
Large Extra Dimensions Virtual Graviton Exchange
DIS
c2 fit of ds/dQ2 no deviation from SM gt Set
limits on hG gt 95 CL limits on MS (TeV)
Hewett formalism
14
Large Extra Dimensions Virtual Graviton
Exchange
DIS
ds/dQ2 used in binned likelihood gt Set limits on
hG gt 95 CL limits on MS (TeV)
  • Hewett formalism
  • l - 1 MS gt 0.79 TeV
  • 1 MS gt 0.78 TeV

15
Large Extra DimensionsDirect Graviton Emission
jet(s)MET
  • Graviton produced along with a jet disappears in
    the bulk, undetected gt mono-jet like topology
    with high MET
  • Nexp 100.2 6.3 (stat) 7.5 (theo)
    50 - 30 (JES)
  • Nobs 63 ( 5 efficiency)
  • Final Selection
  • MET gt 150 GeV
  • PT(jet1) gt 150 GeV, h lt 1
  • PT(jet2) lt 50 GeV
  • Df(MET,jet1) gt 30o

limits on MS 660-680 GeV
85pb-1
QCD
MC SM bkg mostly Z-gtnnjet(s)
updated analysis with 200pb-1 and new JES in
process ...
n 6 and MS 0.7 TeV
16
TeV-1 Extra DimensionVirtual Exchange of Z/g KK
states
D0 ee
200pb-1
  • (gt 1 EM w/ track match)
  • same procedure as for LED analysis but with
    virtual Z/g KK states effects parameterized
    by hC p2/3MC2
  • Nexp 12.1 (4.3 QCD), Nobs 9
  • gt Limit set as done for LED hC lt 2.63 TeV-2 gt
    MC gt 1.12 TeV _at_ 95 CL

signal for hC 5 TeV-2
QCD
D-Y QCD
H1 DIS
KK states modify the Z/g propagators 1/Q2 -gt
1/Q2 hC 1/(Q2MZ2) -gt 1/(Q2MZ2) hC Fit to
ep and e-p data gt MC gt
1.0 TeV _at_ 95 CL
LEP
from combined precision EW measurements
MC gt 6.6 TeV
17
RS Extra Dimension
  • Graviton KK states well separated gt resonant
    graviton search
  • CDF analyses
  • ee and mm binned likelihood method
  • gg counting limits using 3s mass window around
    resonance
  • D0 analysis
  • diEM using 3s mass window method

18
RS Extra Dimension
ee, mm, gg
  • mm
  • 2 isolated ms w/ PTgt20GeV
  • hm1 lt1, hm2lt1.5
  • cosmic veto

??
ee
??
  • gg
  • 2 isolated gs w/ ETgt15GeV
  • CC
  • ee
  • 2 isolated es w/ ETgt25GeV
  • CC or CP

data agree with expected SM bkg ...
19
RS Extra Dimension
ee, mm, gg
  • cross-section limits computed from binned
    likelihood (ee,mm) and 3-s mass window (gg)
  • compare to R-S cross-section for different
    values of the k/MPL parameter.

??
ee
??
gt exclusion contour plot ...
20
RS Extra Dimension
ee, mm, gg
Lower limits on MG (GeV) for k/MPL 0.1
  • Further improvement can be achieved by
  • using mass window method for dilepton channels
  • combining channels

21
RS Extra Dimension
diEM
same diEM data set as for LED search
200pb-1
CC-CC CC-EC
signal RS Graviton MG 300 GeV
D-Y direct gg QCD
QCD
785 GeV
data agree with expected SM background gt set
limits with mass window method
22
Summary
23
Conclusions
  • Tevatron, CDFD0 working well
  • CDFD0 have by now each 450pb-1 on tape
  • Tevatron and HERA are great tools to start
    looking for EDs
  • Very competitive results and even most stringent
    limits are starting to come out
  • There is still room for improvement, so stay
    tuned.
  • However, for the final word on some models, we
    may very well need to wait for LHC ...
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