Title: Diffractive and Total pp Cross Sections at LHC
1Diffractive and Totalpp Cross Sections at LHC
Konstantin Goulianos The Rockefeller University
13th International Conference on Elastic
Diffractive Scattering (13th "Blois Workshop")
CERN, 29th June - 3rd July 2009
2Contents
- References
- Strategy
- Unitarity and renormalization
- Cross sections _at_ LHC
- Global fit to pp, pp, Kp x-sections
- The ratio of a'/e
- Discussion
3References
http//physics.rockefeller.edu/dino/my.html CDF
PRD 50, 5518 (1994) sel _at_ 1800 546 GeV CDF
PRD 50, 5535 (1994) sD _at_ 1800 546 GeV CDF
PRD 50, 5550 (1994) sT _at_ 1800 546 GeV KG-PR
Physics Reports 101, No.3 (1983) 169-219
Diffractive interactions of hadrons at
high energies KG-95 PLB 358, 379 (1995)
Erratum PLB 363, 268 (1995)
Renormalization of hadronic diffraction CMG-96
PLB 389, 176 (1996) Global fit
to pp, p and Kp cross sections KG-09
arXiv0812.4464v2 hep-ph 26 March 2009
Pomeron intercept and slope the QCD
connection
4Strategy
- Froissart bound
(s in GeV2) - For m2 mp2 ? p/m2 104 mb large!
- If m2 so (mass)2 of a large SUPERglueBALL,
the bound can be reached at a much lower s-value,
sF, -
? - Determine sF and s0 from sTSD
- Show that vsF lt 1.8 TeV
- Show that at vs 1.8 TeV Reggeon contributions
are negligible - Get cross section at the LHC as
5 Standard Regge Theory
(KG-95)
- Parameters
- s0, s0' and g(t)
- set s0 s0 (universal IP)
- g(t) ? g(0) gPPP see KG-PR
- determine s0 and gPPP how?
6Unitarity and Renormalization
Pomeron flux
Pomeron-proton x-section
- Two free parameters s0 and gPPP
- Obtain product gPPPs0e / 2 from sSD
- Renormalized Pomeron flux determines s0
- Get unique solution for gPPP
7Single Diffraction
KG-95
Pomeron flux
- Renormalization
-
- Flux integral depends on s and s0
- knee vs-position determines s-value
- where flux becomes unity ? get so
- get error in so from error in vs-knee
- dso/so -2 ds/s -4 (dvs)/vs
8The value of so - a birds-eye view
KG-95
- vs (GeV)
- Cool KG FNAL 14 20
- Albrow ISR 23.3 26.9
- Armitage ISR 23.3 27.4
- ? error in knee position 1 GeV
knee _at_ 22 1 GeV ? s0 1 0.2 GeV
?riple-Pomeron coupling
KG-95
9The value of so- limited edition
shape of renormalized sSD
shape of Regge s2e
CDF
- use CDF points to fix the level of renormalized
curve - use E396 points to fix the level of the Regge
curve - both curves are somewhat high in this plot
- ?adjusting height leads to the same knee
position
E396
10The SUPERBALL cross-section
- Froissart bound
- Valid above knee at vs 22 GeV and therefore
at vs 1.8 TeV - Use superball mass
- ? m2 s0 (10.2) GeV2
- At vs 1.8 TeV Reggeon contributions are
negligible (see global fit) -
? compatible with CGM-96 global fit result of 114
5 mb (see next slides)
11Global fit to pp, p, Kp x-sections
Global fit to pp, p, Kp x-sections
CMG-96 ?
Use standard Regge theory
negligible
12sT at LHC from global fit
- s _at_ LHC vs14 TeV 122 5 mb Born, 114 5 mb
eikonal - ? error estimated from the error in e
given in CMG-96
Compare with SUPERBALL s(14 TeV) 113 6 mb
caveat so1 GeV2 was used in global fit!
13Extra the ratio of a'/e
KG-09
The key!
?
14SUMMARY
- Froissart bound
- Valid above the knee at vs 22 GeV in sTSD
vs. vs - and therefore valid at vs 1.8 TeV of the CDF
measurement - Use superball mass s0 (saturated dressed proton
mass) in the Froissart- Martin formula, where
s0 is determined from setting the integral of the
Pomeron flux to unity at vs 22 GeV - ? m2 s0 (10.2) GeV2
- At vs 1.8 TeV Reggeon contributions are
negligible (see global fit) -
- compatible with CGM-96 global fit result of
114 5 mb
15thank you
thank you
16DISCUSSION
ANY QUESTIONS?