Title: Search for ExtraDimensions at pp and ep Colliders
1Search for Extra-Dimensionsat pp and ep
Colliders
_
- Eric Kajfasz, CPPM/D0
- kajfasz_at_cppm.in2p3.gov
- for the CDF, D0, H1 and Zeus collaborations
2Extra 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
- ...
3Extra 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)
4Extra 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
5Extra 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
6Large Extra DimensionsVirtual Graviton Exchange
dilepton channel (Tevatron)
SM
SM
diphoton channel (Tevatron)
DIS channel (Hera)
SM
7Large 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
8Large 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
9Large 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
10Large 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
11Large 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
12Large 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
13Large 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
14Large 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
15Large 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
16TeV-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
17RS 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
18RS 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 ...
19RS 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 ...
20RS 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
21RS 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
22Summary
23Conclusions
- 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 ...