Diffraction and Exclusive Production at CDF · Road towards LHC Summary 2 Outline. Non-Diffractive...
Transcript of Diffraction and Exclusive Production at CDF · Road towards LHC Summary 2 Outline. Non-Diffractive...
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Koji TerashiThe Rockefeller University
for the CDF Collaboration
Wine & Cheese Seminar, March 30th, 2007
1
Diffraction and Exclusive Production at CDF
~ Towards Exclusive Higgs at LHC ~
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Motivation Run I Results Run II Results and Prospects Road towards LHC Summary
2
Outline
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Non-Diffractive Diffractive
Color exchange Colorless exchange with vacuum quantum numbers
GOAL : Understand the QCD nature of diffractive exchange
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Diffractive Physics
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Exclusive (QCD)
Gluon exchange with extra soft gluon→neutralize color-flow
GOAL : Test and calibrate theoretical calculations of exclusive production
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Exclusive Production
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η
φp
p-ln ξ
p
ξ
ξ : momentum fraction of p carried by diffractive exchanget : 4-momentum transfer squaredMX : mass of system X
Strategy Characterize formation of rapidity gap(s) in events
with different gap topology Examine partonic structure using high pT probes
X
X
5
GAP
ln MX2
ξ = MX2 / s
ln s
t
Diffractive pp Interactions
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Single Diffraction
Double Diffraction
Double Pomeron Exchange
Single + Double
Diffraction
ηφ
p
p
ηφ
p
p
ηφ
p
p
ηφ
p
p
14 published papers : 13 PRL and 1 PRD
6
σtotal and σelastic (not discussed today)
CDF Diffraction in Run I
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‣ Pomeron trajectory : αIP(t) = 1 + ε + α’t‣ ε ≃ 0.1‣ s’ = MX2 = sξ
[ ]Flux fIP/p(ξ, t)
Single Diffraction Cross Section
d2σSD
dξdtβIPp(t)2 ξ
16π1
=1-2αIP(t) βIPp(0)g(t)( )s0
s’ ε
σIPptotal
σSD = ∫ξmin
0.1
∫∞0
fIP/p(ξ, t)σIPptotaldξ dt ~ sε ∫ξmin
0.1
dξξ−(1+ε)
~ s2ε
p
p
p
ξX
cf. σtotal = βIPp(0)2( )s0
s ε~ sε
7
Diffraction in Regge Theory
ξmin = M02/s
−
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Regge Theory
σSD ~ s2ε (ε ≃ 0.1)⇒ exceeds σtotal at √s ≈ 2 TeV
Measurement‣ σSD ~ s2(0.015±0.008)
⇒ much weaker s-dependence
➡ A factor of ~10 suppressed in normalization
‣ dσ/dξ ~ ξ−(1+ε) dependence➡ Same as Regge theory
8
1000010001001 01
1 0
1 0 0
!s (GeV)
Tota
l Sin
gle
Diffr
actio
n Cr
oss
Sect
ion
(mb)
" < 0.05Albrow et al.Armitage et al.UA4CDFE710
Renormalized
Standard
f luxCool et al.
pp
f lux
"knee" at 22 GeV
CDF: 546 GeV and 1.8 TeVPRD 50, 5535 (1994)
Tota
l Sin
gle
Diff
ract
ion
Cro
ss S
ectio
n (m
b)
√s (GeV)
K. Goulianos, PLB 358,379(1995)
RenormalizationPomeron flux integral (re)normalized to unity ∫
ξmin
0.1
∫∞
0
fIP/p(ξ,t) = 1dξ dt
Soft Single Diffraction
−
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DDPRL 87,141802(2001)
DPEPRL 93,141601(2004)
SDDPRL 91,011802(2003)
Event yield as a function of Δηgap or ξRegge-based MC simulations normalized to data
10
10 2
10 3
10 4
10 5
0 1 2 3 4 5 6 7
!s=1800 GeVDATADD + non-DD MCnon-DD MC
"#0=#max-#min
even
ts
10
10 2
10 3
10 4
10 5
10-6
10-5
10-4
10-3
10-2
10-1
1!p
X
MX2
Num
ber o
f Eve
nts
per "
log!
= 0
.1
DataDPE MCSD MCDPE+SD MC
#s$ = 1800 GeV0.035 % !- p % 0.095| t- p | % 1.0 GeV2
( GeV 2 )1 10 10 2 10 3 10 4 10 5 106
10 2
10 3
10 4
10 5
0 1 2 3 4 5 6 7!"0
exp="max-"minev
ents
#s=1800 GeVDATASDD + SD MCSD MC
η
φ
η
φ
η
φ
fixed
fixed
Data agree with Regge predictions in ξ-dependence 9
Soft Diffraction
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DD DPE SDDFraction (or cross section) of gap events as a function of √s
1
10
10 2
10 102
103
!s (GeV)
"DD
(mb)
for #
$ >
3.0
ReggeRenormalized gap
CDFUA5 (adjusted)
10-1
1
103
sub-energy !s--, (GeV)
gap
fract
ion "#
> 3
.0 CDF: one-gap/no-gapCDF: two-gap/one-gapRegge predictionRenorm-gap prediction
2-gap
1-gap
2100
0.1
0.2
0.3
0.4
0.5
103
!s" (GeV)
Frac
tion
of E
vent
s wi
th #
p < 0
.02
CDF Data (Preliminary)Regge + FactorizationGap Probability Renorm.Pomeron Flux Renom.
Single gap rates are suppressed by O(10) Double gap rates are less suppressed
relative to Regge predictions
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Soft Diffraction
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Proposed by Ingelman and Schlein in 1985 PLB 152, 256(1985)
Discovery of diffractive di-jets by UA8 PLB 211,239(1988), 297,417(1992)
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Probing partonic structure of the diffractive exchangeSD DD DPE
‣ W boson‣ Di-jet ‣ b-quark‣ J/ψ meson
‣ jet-gap-jet (not shown today)
‣ Di-jet
ηφ
p
p
ηφ
p
p
ηφ
p
p
Hard Diffraction
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p
e
p
e
IPzIPx
p
p
p
!jetjet
"
Tevatron : σ(pp→pX) ≈ FjjD ⊗ Fjj ⊗ σ(ab→jj)
Universal parton densitiesin diffractive exchange?
Proved by J. Collins PRD 57,3051(1998)
HERA ep TEVATRON pp
HERA : σ(ep→eXp) = FjjD ⊗ σ(ab→jj)
Factorization Test
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?
‣ hard scatteringmatrix element
‣ process dependent
QCD Factorization
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WPRL 78,2698(1997)
Di-jetPRL 79,2636(1997)
b-quarksPRL 84,232(2000)
J/ψPRL 87,241802(2001)
13
Probing quark and gluon contents in diffractive exchange
p
p
pIP
W
p
p
pIP
JetJet
p
p
pIP
bb
p
p
pIP
!J/
q
g g
q/g
Hard Single Diffraction in CDF
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W Di-jet b-quark J/ψ
R[ ] (%) 1.15±0.55 0.75±0.10 0.62±0.25 1.45±0.25diffincl
Diffractive production rates are all similar at ~1% relative to inclusive rates
Factorization approximately holds within Tevatron (at fixed √s)
√s=1.8 TeV
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Diffractive to Inclusive Ratio
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GLUON FRACTION IN POMERON
0
0.2
0.4
0.6
0.8
1
1.2
0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
D (M
EASU
RED
/ PRE
DICT
ED)
ZEUS
CDF-DIJET
CDF-WCDF-b
Gluon Fraction in Pomeron
R(m
easu
red/
pred
icte
d)
R = 0.19 ± 0.04SD production rates are severely suppressed relative to HERA
Factorization breakdown between Tevatron and HERA
R = 1 : factorization valid
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PRL 84, 232(2000)
Factorization Breaking
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p
p
p
!jetjet
"
σ(pp→pX) ≈ Fjj ⊗ FjjD ⊗ σ(ab→jj)
Determine FjjD in LO QCD using
FjjD (xBj, Q2) Fjj (xBj, Q2)σjj(Diff)
σjj(Non-Diff)R(xBj) of=
DataProton PDF
×
16
FjjD = FjjD (ξ, t, xBj, Q2)Diffractive Structure Function
β = xBj/ξ : Momentum fraction of diffractive exchange carried by the scattering parton
Diffractive Di-jet Production
Diffractive Structure Function
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FjjD at the Tevatron is suppressed relative to expectations from dPDFs measured by H1 at HERA
Similar suppression as in soft SD relative to Regge expectations
Breakdown of QCD Factorization confirmed
17
CDF PRL 84,5043(2000)
P. Newman : Hera-LHC workshop, March 2007(Also, see M. Ruspa’s talk in Small-x workshop)
H1(2006)
H1(1997)
Diffractive Structure Function
0.1 1
0.1
1
10
100
CDF dataET
Jet1,2 > 7 GeV0.035 < ! < 0.095| t | < 1.0 GeV2
H1 fit-2H1 fit-3
( Q2= 75 GeV2 )
"
F#D JJ
(")
H1 2006 DPDF Fit AH1 2006 DPDF Fit B
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0.1 1
0.1
1
10
100
!
FD jj(!)
from DPE/SD , 0.01 " # " 0.03
from SD/ND , 0.035 " # " 0.095
SD
SD
ND
DPE
FjjD from DPE/SD is larger than FjjD from SD/ND
gap no gap
Factorization breakdown within the Tevatron18
1.8 TeV
PRL 85, 4215(2000)
Diffractive Structure Functions from DPE and SD Data
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0.1 1
0.1
1
10
100
!
FD jj(!)
CDF data, based on DPE/SD
Expectation from H1 2002 "rD QCD Fit (prel.)
FjjD measured from DPE is approx-imately equal to expectations from dPDFs measured at HERA
2nd gap less suppressed if a gapis already present in the events
QCD factorization between HERA and Tevatron restored?
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Restoring QCD Factorization?
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SD ‣ ξ, t, and Q2 dependence of FjjD
‣ Process dependence of FD(W, Z) →M. Convery’s talk
DPE ‣ ξp dependence on FjjD measured on p-side
DD ‣ Δηgap dependence for fixed large Δηjj →C. Mesropian’s talk
Exclusive ‣ di-jet, di-photon, χc
‣ e+e−, μ+μ− →L. Zhang’s talk
GOAL Further characterize diffractive structure function anddiffractive exchange Measure exclusive production and calibrate theoreticalcalculations
Results presented in this talk20
Run II Diffractive Program
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CDF II
QUADsDIPOLEs
2m
57m to CDF
p p
DIPOLEsQUADs
TRACKING SYSTEM CCAL PCAL MPCAL CLC BSC RPS
Tracking Detectors : |η| < 2.0 Calorimeters : |η| < 5.2 Beam Shower Counters (BSC) : 5.4 < |η| < 7.4 Roman Pot Spectrometers (RPS) : 0.02 < ξ < 0.1
0 < |t|< 2 GeV2
CDF II Detector
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MiniPlug Calorimeters
PMTs25
1/4
"1512 WLS fibers
PMTs
22 1/2"
36 PLATES
BEAM
5 1/
2"
STAINLESS STEEL SUPPORTALUMINUM1/4" THICK PLATE (3/16" PB + 2x0.5mm AL)KURARAY Y11 MULTI!CLAD 1.0mm DIA. WLS FIBER BICRON 517L LIQUID SCINTILLATOR
Electromagnetic calorimeter withhadron detection capability
➡ Good position resolution retained e+ : σposition/E = 9.2mm/√E σenergy/E = 18%/√E+0.6%
➡ Used to measure particle energy and multiplicity in 3.6<|η|<5.2
32X0, 1.3λI
Read out byWLS fibers
Built by Rockefeller Group
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Among problems we had to overcome, the most challenging one is multiple pp interactions (pile-up) that spoil diffractive signatures
pCAL! pCAL!
Even
ts
10-1
1
10
102
103
104
105
106 CDF Run II Preliminary
BGSD
10-3 10 -2 10-1 1 10
RPS + Jet5 > 5 GeV) - rescaledT
seedJet5 (E
pRPS!
0 0.02 0.04 0.06 0.08 0.1 0.12
pCA
L!
0
0.2
0.4
0.6
0.8
1
1.2
0
2
4
6
8
10
12CDF Run II Preliminary
Σtowers ETe-η
√sξCAL =
ξCAL
pile-up events
signal region
Used to reject pile-up eventsby selecting ξCAL < 0.1
Linst~2×1031cm-2s-1 (not “high” lum!)
23
ξCA
L
ξRPS
Run II Challenge
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Bjx
) / N
D!
"Ra
tio (
SD
/
10-3
10-2
10-1
1
10 / ndf 2
# 23.26 / 12
Prob 0.0256
Const 0.000965± 0.01031
slope 0.04419± -1.027
/ ndf 2# 23.26 / 12
Prob 0.0256
Const 0.000965± 0.01031
slope 0.04419± -1.027
10-3 10-2 10-1
6% (slope)± 20% (norm), ±systematic uncertainty:
<0.09pCAL!0.03<
|<2.5)jet$ CDF Run II preliminary (||<4.2)jet$ CDF Run I (|
Run I result is confirmed(difference at high xBj caused from different jet acceptance)
FjjD (xBj, Q2)
Fjj (xBj, Q2)RSDND (xBj) ≈
24
xBjorken-dependence of FjjD
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Bjx
) / N
D!
"Ra
tio (
SD
/
10-3
10-2
10-1
1
10 / ndf 2# 23.26 / 12
Prob 0.0256
Const 0.0009656± 0.01031
slope 0.04422± 1.027
/ ndf 2# 23.26 / 12
Prob 0.0256
Const 0.0009656± 0.01031
slope 0.04422± 1.027
10-3 10-2 10-1
6% (slope)± 20% (norm), ±overall syst. uncertainty: )/2jet2
T+Ejet1T>=(E*
T, <E2>*T <E$ 2Q
<0.09pCAL!0.03<
CDF Run II Preliminary2 100 GeV%
2Q2 400 GeV%
2Q2 1,600 GeV%
2Q2 3,000 GeV%
2Q2 6,000 GeV%
2Q2 10,000 GeV%
2Q
No appreciable Q2 dependence relative to Fjj in 100 < Q2 < 10000 GeV2
Pomeron evolves similarly to proton
FjjD (xBj, Q2)
Fjj (xBj, Q2)RSDND (xBj) ≈
25
~10 GeV〈ET*〉
~100 GeV
NormalizationN
~10-4N
Q2-dependence of FjjD
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2 |t| (GeV/c)0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
2 |t| (GeV/c)0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
/dt [
arbi
trary
uni
ts]
!d
10
102
103
104
RPS inclusive
)2~225GeV2RPS+Jet5 (Q
)2~900GeV2RPS+Jet20 (Q
)2~4,500GeV2RPS+Jet50 (Q
)/2jet2T+Ejet1
T>=(E*T, <E2>*
T <E" 2Q<0.08p
RPS#0.05<
CDF Run II Preliminarystatistical uncertainties only
)2 (GeV2Q10-2 10-1 1 10 10 2 103 104
) at |
t|=0
(arb
itrar
y un
its)
2b(
Q
0
0.2
0.4
0.6
0.8
1
1.2
1.4
1.6
1.8
2CDF Run II Preliminary
<0.08pRPS!0.05<
RPS inclusivenorm. to unity and
2=1 GeV2set at Q
Fit t-distributions to a double exponential function :
F = 0.9eb1t + 0.1eb2t
Slope at t=0 is independent of Q2 in the range 0<Q2<4500 GeV2
Work in progress for➡ absolute t-slope values➡ larger |t| range up to ~4 GeV2
26
arbitrary normalization
t-dependence of FjjD
→M. Gallinaro’s talk
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Motivated by unique potential to measure particle state produced in exclusive reaction pp→pXp
‣ JPC = 0++ state due to Jz = 0 rule‣ clean signal (no underlying event)
Primary aim is Higgs boson (and new physics)
27
p
p
p
p
gg
gHX
Exclusive Production
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p
p
p
p
gg
gH
Tagging forward nucleons
➡ Higgs quantum numbers➡ mass resolution < 2~3 GeV using missing mass method: MH = (pin+pin−pout−pout)1/2
SM Higgs boson (MH=120 GeV):σ(pp→pHp) < 0.1 fb at Tevatron, = 1~10 fb at LHC
Calibrate theoretical calculations using exclusive processes with higher cross sections
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Standard Model Higgs Boson
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Exclusive Di-jet/Di-photon Exclusive Di-lepton
p
p
p
p!
!
+l-l)µl=(e,
p
p
p
p
gg
g
!j, !j,
Potential to improve LHCluminosity measurements
Validate analysis method
QED-mediated processCross section well known (< 1%)
Exclusive Production at CDF
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Analysis requires - protons do not dissociate- only e+e− produced (ET>5GeV, |η|<2) and nothing else
Good control sample for pp→pγγp search
30
p
p
p
p!
!
+e-e
Detailed analysis performed to set thresholds for each detectorEffective Luminosity : 46±3 pb-1 (out of 532 pb-1)
Exclusive e+e− Production
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Et = 15.62 GeV
!
-4-3
-2-1
01
23
4
"
0100
200300
TE
0
10
20
16 candidate events observed
31
ET1 = 15.2 GeVET2 = 14.6 GeV
of leading electronTE0 5 10 15 20 25 30
of s
econ
d el
ectro
nTE
0
5
10
15
20
25
30 CDF Run II PreliminaryData (no BG subtracted)LPAIR MC
(rad)! "2.8 2.85 2.9 2.95 3 3.05 3.1 3.15
)! "
1/N
dN/d
(
00.10.20.30.40.50.60.70.8
CDF Run II PreliminaryData (no BG subtracted)LPAIR MC
CDF Run II
Exclusive e+e− Production
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Number of Additional Clusters0 10 20 30 40 50
Num
ber o
f Eve
nts
02468
101214161820 Candidate Sample
LPAIR SimulationBackground Fit
a)
σMEAS. = 1.6 +0.5-0.3(stat) ± 0.3(syst) pb
agrees with LPAIR Monte Carlo (QED) prediction σLPAIR = 1.71 ± 0.01 pb
PRL 98, 112001 (2007)
16 candidate eventsBackground: 1.9±0.3 events 5.5σ observation
Good agreement serves to validate analysis method
CDF Run II
Exclusive e+e− Production
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Gluon exchange process factor 3~4 uncertainty in σ
33
Can be used to calibrate exclusive Higgs cross section
Analysis requires - same event selections as pp→peep (except etrack veto)- only γγ produced (ET>5GeV, |η|<1) and nothing else
p
p
p
p
gg
g!!
Exclusive Di-photon Production
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3 candidate events observedExclusive Di-photon Production
34
ET1 = 6.8 GeVET2 = 5.9 GeV
CDF Run II Preliminary (rad)!"2.8 2.85 2.9 2.95 3 3.05 3.1 3.15 3.2
)! "
1/N
dN/d
(
0
0.1
0.2
0.3
0.4
0.5
0.6
0.7 CDF Run II PreliminaryData (no BG subtracted)ExHume MC
)2Invariant Mass (GeV/c0 10 20 30 40 50 60
!!1/
N dN
/dM
00.20.40.60.8
11.21.41.6
CDF Run II PreliminaryData (no BG subtracted)ExHume MC
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3 candidate events including exclusive π0π0 or ηη (π0,η→γγ)Background : 0.09±0.04 events 3.7σ evidence for combined exclusive (γγ, π0π0, ηη) signal EM shower analysis indicates 2 of 3 events are likely γγ
σ(pp→pγγp) < 410 fb (95% C.L.)Khoze, Martin, Ryskin : σγγ~40 fb (factor 3 uncertainty)
Assuming 2 events are exclusive γγ,σ(pp→pγγp) = 90 +120-30(stat) ± 16(syst) fb
35
Exclusive Di-photon Production
→M. Albrow’s talk
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Exclusive Di-jet Production
Select inclusive DPE di-jets : p+p → p+X(∋2jets)+gapReconstruct di-jet mass fraction : Rjj = Mjj/MX
Look for data excess over DPE di-jet background as Rjj→1
Strategy
36
Rjj→1 0 η→+
pp
Jet Jet
0 η→+
pp
Jet Jetdetected
not detected
X
➡ Signal (Rjj=1) smeared due to shower/hadronization effects, NLO gg→ggg, qqg contributions, etc.
➡ DPE di-jet background shape from POMWIG MC simulation (⇒ Uncertainty from Pomeron PDF)
gap
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37
X / Mjj = MjjR0 0.2 0.4 0.6 0.8 1
dN /
N
10-4
10-3
10-2
10-1 DPE data (stat. only)
Background
POMWIG + BackgroundH1!POMWIG : CDF
POMWIG : CDFPOMWIG : H1-fit2POMWIG : ZEUS-LPS
CDF Run II Preliminary
Excess observed over MC simulations with varied PDFs
!
-4-3
-2-1
01
23
4
"
0100
200300
TE
0
5
10
Et = 16.94 GeV
ET1 = 33 GeVET2 = 31 GeV
Rjj = 0.96CDF Run II Preliminary
Di-jet Mass Fraction
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Binned likelihood fits (MC normalizations as free parameters)
Signal MC ExHuMECPC 175,232(2006)
Exclusive DPE (DPEMC)CPC 167,217(2005)
CDF H1CDFH1-fit2ZEUS-LPS
22.1±1.8 %21.7±1.8 %24.7±2.0 %24.3±2.0 %
23.0±1.9 %22.6±1.9 %26.0±2.1 %25.4±2.1 %
X / Mjj = MjjR0 0.2 0.4 0.6 0.8 1
Even
ts
0
100
200
300
400
500CDF Run II Preliminary
DPE data (stat. only)H1!POMWIG: CDF
ExHuMEBest Fit to Data
| < 5.9gap"3.6 < | > 10 GeVjet2
TE < 5 GeVjet3
TE < -0.5jet1(2)"
1.8 %± = 22.1 exclF(stat. only)
X / Mjj = MjjR0 0.2 0.4 0.6 0.8 1
Even
ts
0
100
200
300
400
500CDF Run II Preliminary
DPE data (stat. only)H1!POMWIG: CDF
Exclusive DPE (DPEMC)Best Fit to Data
| < 5.9gap"3.6 < | > 10 GeVjet2
TE < 5 GeVjet3
TE < -0.5jet1(2)"
1.9 %± = 23.0 exclF(stat. only)
stat. error only
databkgdsignalfit
38
⊕
MC Fit to Rjj Shape
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39
X/Mjj = MjjR0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
F0.5
1
1.5
CDF Run II Preliminary
Systematic Uncertainty1F
= POMWIG + BackgroundinclMCH1-fit2)!(CDF
<0.4jj at Rinclnormalized to Data
: stat. error only2F
"<0.4)jj(Rbc/inclF# / bc/incl F$ 1Fincl / Dataincl MC$ 2F
LO exclusive gg→qq suppressed due to Jz = 0 rule Look for the suppression in heavy flavor jet fraction vs Rjj
X/Mjj = MjjR0 0.1 0.2 0.3 0.4 0.5 0.6 0.7 0.8 0.9 1
!<0
.4)
jj(R
bc/in
clF"
/ bc
/incl
F 0.5
1
1.5
CDF Run II Preliminary
DPE data (SVT)Systematic Uncertainty
(RAW) > 10 GeVjetTE
| < 1.5jet#|
X / Mjj = MjjR0 0.2 0.4 0.6 0.8 1
dN /
N
10-4
10-3
10-2
10-1
DPE data (stat. only)H1!POMWIG : CDF
BackgroundPOMWIG + Background
H1!CDFCDF Run II Preliminary
inclMC
incldata
HFdata
incldata
The two results are consistent with each other
Exclusive Di-jet Signal
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(GeV)minTJet E
10 15 20 25 30 35
>0.8
) (pb
)jj
(R e
xcl
jj!
-110
1
10
210
310
31 ×KMR
Hadronizationuncertainty
CDF Run II PreliminaryData corrected to hadron level
ExHuME
Exclusive DPE (DPEMC)
minT > Ejet1, 2
TE| < 2.5jet1, 2"|
< 5.9gap"3.6 < < 0.08p#0.03 < stat. syst. uncertainty$stat.
40
Khoze, Martin, Ryskin at LO parton-level (factor 3 uncertainty)
hep-ph/0507040
Exclusive DPE (DPEMC)
ExHuME
Measured σjjexcl prefers ExHuME and KMR calculations
Exclusive Di-jet Cross Section
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Exclusive Di-jet Mass Reach
CDF pp→pjjp reaches Higgs mass range!!pp→pHp at LHC
41
)2 (GeV/cjjM20 40 60 80 100 120 140 160
2G
eV/c
pb
jjdM
excl
jj!d
-310
-210
-110
1
10
210 ExHuME (Hadron Level)DefaultDerived from CDF Run II
)minT (Eexcl
jj!Preliminary
| < 2.5jet1, 2"| < 5.9gap"3.6 <
< 0.08p#0.03 <
Systematic Uncertainty
Unfold measured σjjexcl to dσjjexcl/dMjj using ExHuME
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Lum = 1033-34 cm2 (Low β*)
MX2 = ξ1 ξ2 s
TOTEM+CMSSimilarly in ATLAS
FP420
P. BusseyW. Plano
⇒ FP420 project
ATLAS
CMS
42
Acceptance ξ MX (GeV)
220m+220m 0.02-0.2 200-2000
420m+420m 0.002-0.02 30-200
pp→pHp Acceptance at LHC
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MH (GeV) 120 140 160
H→WW(*)→lνjj (fb)proton tagger acceptance
0.25 0.63 0.83
#Events at 30 fb-1
ATLAS lepton trigger 1.1 3.6 5.8
B .Cox et al., Eur. Phys. J. C45, 401 (2006)
43
Exclusive Higgs→WW(*) at LHC
p
p
p
p
gg
gH
H→WW(*) for MH=135-200 GeV MH resolution ~ 2 GeV (any W decay)
by tagging forward protons
“Very small backgrounds” (continuum within ΔMH)
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Feasibility study and R&D for the proton detector at 420m from the IP in normal high luminosity running
‣ R&D fully funded‣ Aim is to install detectors in Fall 2008
44
www.fp420.com
FP420 Project
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Fixed Beampipe
BPM
BPM
Detector Space
Cryogenic Lines
45
Mechanics at 420m
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Test beam at CERN in Sep 2007
46
Fast Timing DetectorsReject pile-up backgrounds by measuring Zvertex using time-of-flight information
UTA, Albert, FNAL, Louvain
Silicon Detectors
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47
Both soft and hard diffraction results appear to point to a picture of diffractive exchange;
Universality of rapidity gap formation Composite ‘proton-like’ structure Factorization breakdown and restoration
Run II studies will help understand the QCD aspects
Exploring physics with exclusive production
Perturbative QCD appears to work well CDF results encouraging for future prospects at LHC Ongoing efforts to install proton taggers at LHC
→ FP420 project
(soft ↔ hard)
Summary