Andrew Brandt – September 19 2003 Small-x 2003 – 1 Forward Physics with Forward Physics with ATLAS ATLAS • Luminosity measurement for ATLAS • Forward Physics with ATLAS D.Bocian, M.Boonekamp, A.Brandt, E.Brash, B.Caron, K.De, I.Efthymiopoulos, A.Faus-Golfe, P.Grafstrom, W.Guryn, M.Haguenauer, A.Hamilton, V.Hedberg, B.Jeanneret, J.Lamsa, C.Leroy, M.Lokajicek, G.Lolos, J-P.Martin, J.McDonald, Z.Papandreou, J.Pinfold, M.Rijssenbeek, E.Rosenberg, V.Simak, J.Soukup, H.Takai, V.Telnov, S.Tapprogge, W.Turner, S.Valkar, J.Velasco, A.Verdier, S.White, Y.Yao Thanks to: Michael Rijssenbeek for his slides! .
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Andrew Brandt – September 19 2003Small-x 2003 – 1 Forward Physics with ATLAS Luminosity measurement for ATLAS Forward Physics with ATLAS D.Bocian, M.Boonekamp,
Andrew Brandt – September Small-x 2003 – 3 The ATLAS Detector Calorimetry: TAS R Barrel FCAL LUCID Tracking EndCap RP ZDC/TAN Diffraction/Proton Tagging Region y 109 -chambers Tracking: ATLAS has insufficient forward coverage for Total Rate measurement
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Andrew Brandt – September 19 2003 Small-x 2003 – 1
Forward Physics with Forward Physics with ATLASATLAS
• Luminosity measurement for ATLAS• Forward Physics with ATLAS
– Precision comparison with other expt’s• Luminosity from:
– LHC Machine parameters (~5-10%)– Rates of well-calculable processes
• Dedicated Luminosity monitor: LUCID
Relative precision on the measurement of HBR for various channels, as function of mH, at Ldt = 300 fb–1. The dominant uncertainty is from Luminosity: 10% (open symbols), 5% (solid symbols).
(ATL-TDR-15, May 1999)
Andrew Brandt – September 19 2003 Small-x 2003 – 3
The ATLAS DetectorThe ATLAS Detector
GeV
10%( , ) 0.3%/
E eE E
GeV
60mrad/E
GeV
4 ns/t E
GeV
50%( ) 3%/
E
E E
GeV
50%( jet) 2%/
E
E E
Calorimetry:
TAS
R
50 1 2 43 6 7 8
Barrel
FCAL LUCIDTracking
EndCapRP
ZDC/TAN
Diffraction/Proton Tagging Region
y109
-chambers
GeV(Inner Det) (0.03 / 1.2)%TT
pp
Tracking:
GeV(IDet+ ) (0.009 / 1.4)%TT
pp
ATLAS has insufficient forward coverage for Total Rate measurement
Andrew Brandt – September 19 2003 Small-x 2003 – 4
Andrew Brandt – September 19 2003 Small-x 2003 – 5
BaselineBaseline• Luminosity with CNI optics and Coulomb Normalization
– Roman Pots at 220-240 m– Scintillating strip detectors– Integrate into L1 Trigger
• LUCID for relative L monitoringDedicated detector:
• bundle of projective Cerenkov cones: 5 layers of 40 tubes each• low mass (6 kg), rad hard, quartz fiber readout
proof of principle: CLC at CDF!
• Cross checks with:– W/Z rates– Double photon exchange production of muon pairs– Elastic slope of dN/dt|t=0 plus machine L– others…
Andrew Brandt – September 19 2003 Small-x 2003 – 6
ExtensionsExtensions• Diffractive cross sections
– need RP pairs at intermediate locations: 90, 150 m– possibly forward calorimetry (TAS region)
• Large-|t| studies (t in dip region and beyond) – need RP pairs at intermediate locations: 90, 150 m and
smaller?
• DPE Higgs production…– need additional RP pairs at cryogenic locations: 330 m, 420 m– forward calorimetry (TAS region) might be attractive…
Andrew Brandt – September 19 2003 Small-x 2003 – 7
Coulomb Normalization of Coulomb Normalization of LLPossible with very high
β* (≥ 2500 m) optics (3500m now dead):
*=3500 m optics: A. Faus-Golfe, M. Haguenauer, J. Velasco, "Luminosity determination using Coulomb scattering at the LHC",
presented at EPAC2002, June 2002
• Normalization of the scattering amplitude at t 0 to the exactly calculable Coulomb amplitude:
determines Luminosity L directly (and measure σtot, ρ0, b, …)
L/L ~ 2% (UA4 experience) • Need closest possible
approach to the beam• Very-small-angle detectors in
Roman Pots UA4
??
LHC
ISR
2
el tot2
el20
0
20
2 ( )4
4
C N
ti
ft
bE
f
t
d d G e i edtdt tt
N
L L L
RHIC
Caveat: Phase and shape of FN(s,t) ! V.Kandrát, M.Lokajíček, PL B 544 (2002) 132.
Andrew Brandt – September 19 2003 Small-x 2003 – 8
Elastic Scattering in CNI Regime Elastic Scattering in CNI Regime • Need: t min tCNI = 8EM/tot 710–4 GeV2
• For εN ≃1106 , kσ=15, t min= pBmp kσ
2εN/* = 610–4 GeV2 * ≳ 2500 m
• Detector: beam size (rms) d = √(βdεN/) , kσ d ≳ 1.5 mm d ≳ 80 m
• Roman Pot detectors between Q5-Q6 or Q6-Q7 (z 220-240 m)– Leff 500 m, =x /Leff, x ∈ {~1.5 mm, 25 mm}
tmin = (pmin)2 4×10–4 GeV2 tmax (pmax)2 0.12 GeV2
– Precision needed: t/t ≃ 1‰ x O(10 m) need “self-calibrating” detectors
L/L 2%• Positions at z >300 m possible, but difficult
240 m 220 m
dN/dt shapeis crucial!
Andrew Brandt – September 19 2003 Small-x 2003 – 9
June Workshop on Roman Pot June Workshop on Roman Pot DetectorsDetectors
• Parallel effort on RP detectors…• Aim: focus on a (single?)
appropriate technology for TOTEM/CMS and ATLAS
http://efthymio.home.cern.ch/efthymio/LHC-LUMI/Workshop03/or via the Luminosity and Forward Physics WG webpage
Andrew Brandt – September 19 2003 Small-x 2003 – 10
Requirements for Roman Pot Requirements for Roman Pot DetectorsDetectors• “Dead space” d0 at detector’s edge near the beam the beam:
d0 ≲ 100 m (full/flat efficiency away from edge)• Detector resolution: d = 30 m (10 m for pleading measurement)• Same d = 30 m (10 m) relative position accuracy between
• Radiation hardness: 100 Gy/yr (105-6 Gy/yr at full L)• Operate with the induced EM pulse from circulating bunches
(shielding, …)
• Rate capability: O(Mhz) (40 MHz); time resolution t = O(ns) • Readout and trigger compatible with ATLAS TDAQ• Other:
– Simplicity, Cost– extent of R&D needed, time scale, manpower, …– issues of LHC safety and controls
Andrew Brandt – September 19 2003 Small-x 2003 – 11
Forward Physics Interest…Forward Physics Interest…Possible extension of ATLAS baseline physics:• (Soft) Diffractive cross sections are large:
el 26 mb, SD DD 13 mb (i.e. close to Pumplin bound!)
– need only modest L
• Elastic and Total cross section measurements: tot, elastic, Re(fN)/Im(fN), del/dt |N
•dip/structure in d/dt at |t|≈0.5 GeV2? •Regge Pomeron & Odderon à la D&L• transition to pQCD at |t| ≈ 8 GeV2
– Roman Pots at 220-240 m
Andrew Brandt – September 19 2003 Small-x 2003 – 12
Single and Double DiffractionSingle and Double Diffraction•Soft Pomeron Exchange:
production of a forward colorless system…
•P exchange Study of QCD
•Requires: – Accurate pleading measurement ( E <<0.10, small |t|) – Forward & Central measurement– large range for rapidity gap detection…
•Needs additional forward coverage for case of ATLAS…NO plans so far…
IP
p (ξ, t)
M2 = ξ sIP
Andrew Brandt – September 19 2003 Small-x 2003 – 13
Central (hard) DiffractionCentral (hard) Diffraction• Double Pomeron Exchange: production
of a central colorless bosonic system…Requires: – Accurate pleading measurement ( E <<0.10) – Central measurement, e.g. M = gg, H, …– Rapidity gap detection… Δη = lnξ
• Simulations by S. Tapprogge et al., (Helsinki Group, preprint HIP-2003/EXP)
• Predictions for ex(in)clusive production:– “Calibrated” with TeVatron data– Predictions for LHC vary – Many talks/discussions on DPE at this conference:
DPE is THE main argument (towards the Hi-PT community) for doing Forward Physics at LHC!
IP
IP
p (ξ1)
p (ξ2)
M2 = ξ1ξ2s
Andrew Brandt – September 19 2003 Small-x 2003 – 14
Acceptance for Central Acceptance for Central ProductionProduction
• Combined acceptance of: All detectors- - - - 420 m + 215 m____ 215 m alone- - 420 m alone