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Predictions of Diffractive Cross Sections in Proton-Proton CollisionsPowerPoint Presentation

Predictions of Diffractive Cross Sections in Proton-Proton Collisions

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Predictions of Diffractive Cross Sections in Proton-Proton Collisions

Konstantin Goulianos*

The Rockefeller University

Diffractive Cross Sections in pp Collisions K. Goulianos

CONTENTS Collisions

- Introduction
- Cross Sections
- (Event Generation)
- (Implementation in PYTHIA8)
- Conclusions

For details on the phenomenology of the predictions see:

DIFFRACTION 2010

“Diffractive and total ppcross sections at the LHC and beyond” (KG)

http://link.aip.org/link/doi/10.1063/1.3601406

This talk: an implementation of these cross sections in PYTHIA8.

Diffractive Cross Sections in pp Collisions K. Goulianos

INTRODUCTION Collisions

- The RENORM (renormalization model) soft pp cross sections previously used in MBR (Minimum Bias Rockefeller) simulation are adapted to PYTHIA8.
- MBR was successful at Fermilab in fixed target and collider experiments.

- RENORM predictions are based on a parton-model approach in which diffraction is derived from inclusive PDFs and color factors.
- Diffractive cross sections and final states are both predicted:
- Cross sections vs gap width or vs forward momentum loss of proton(s):
- Absolutenormalization!

- Hadronization of dissociated proton:
- A (non-perturbative) “quark string” is introduced and tuned to reproduce the MBR multiplicity and pT distributions.
- dN/dh, pT, and particle ID: new in this PYTHIA8 implementation
- (the original MBR simulation produced only p± and p0).

- Unique unitarization based on a saturated “glue-ball” exchange.

- Cross sections vs gap width or vs forward momentum loss of proton(s):
- Total Cross section ~ln2s based on a glue-ball-like saturated-exchange.
- Immune to eikonaalization-model dependences.

Diffractive Cross Sections in pp Collisions K. Goulianos

p Collisions

Incident hadrons acquire color

and break upart

POMERON

CONFINEMENT

STUDIES OF DIFFRACTION IN QCD- Non-diffractive
- color-exchange gaps exponentially suppressed

- Diffractive
- Colorless vacuum exchange
- large-gap signature

rapidity gap

Incident hadrons retain their quantum numbers

remaining colorless

p

p

p

p

Goal: probe the QCD nature of the diffractive exchange

Diffractive Cross Sections in pp Collisions K. Goulianos

M CollisionsX

p’

p’

DEFINITIONSSINGLE DIFFRACTION

x,t

xp

p

p

MX

dN/dh

Rap-gap

Dh=-lnx

0

ln Mx2

ln s

ln s

since no radiation no price paid for increasingdiffractive gap size

Diffractive Cross Sections in pp Collisions K. Goulianos

SDD Collisions

DIFFRACTION AT CDFsT=Im fel (t=0)

Elastic scattering

Total cross section

OPTICAL

THEOREM

gap

f

f

h

h

DD

SD

DPE /CD

Single Diffraction or

Single Dissociation

Double Diffraction or Double Dissociation

Double Pom. Exchange or

Central Dissociation

Single + Double

Diffraction (SDD)

exclusive

JJ…ee…mm...gg

p

p

JJ, b, J/y,W

Diffractive Cross Sections in pp Collisions K. Goulianos

p’ Collisions

p

x,t

p

M

540 GeV

1800 GeV

see KG, PLB 358, 379 (1995)

FACTORIZATION BREAKING IN SOFT DIFFRACTIONdiffractive x-section suppressed relative to Regge prediction as √s increases

Regge

Factor of ~8 (~5)

suppression at

√s = 1800 (540) GeV

RENORMALIZATION

CDF

√s=22 GeV

Diffractive Cross Sections in pp Collisions K. Goulianos

DD at CDF Collisions

gap probability

x-section

renormalized

Diffractive Cross Sections in pp Collisions K. Goulianos

SDD at CDF Collisions

- Excellent agreement between data and MBR (MinBiasRockefeller) MC

Diffractive Cross Sections in pp Collisions K. Goulianos

CD (DPE) at CDF Collisions

- Excellent agreement between data and MBR
low and high masses are correctly implemented

Diffractive Cross Sections in pp Collisions K. Goulianos

Scale s Collisions0 and triple-pom coupling

Pom. flux: interpret as gap probability

set to unity: determines gPPP and s0

Slide #16

Ddffr. 2012

KG, PLB 358 (1995) 379

Pomeron-proton x-section

- Two free parameters: s0 and gPPP
- Obtain product gPPP•s0e / 2 from sSD
- Renormalized Pomeron flux determines s0
- Get unique solution for gPPP

gPPP=0.69 mb-1/2=1.1 GeV -1

So=3.7±1.5 GeV2

Diffractive Cross Sections in pp Collisions K. Goulianos

Reduce the uncertainty in s Collisions0

Diffractive Cross Sections in pp Collisions K. Goulianos

Cross Sections Collisions

el

tot

CD

SD

SD

DD

- SD single diffraction (single dissociation)
- DD double dissociation (double diffraction)
- CD central dissociation (double pomeron exchange)

Diffractive Cross Sections in pp Collisions K. Goulianos

Total, elastic, and inelastic x-sections Collisions

GeV2

Diffractive Cross Sections in pp Collisions K. Goulianos

Total, elastic, and inelastic x-sections versus √s Collisions

Diffractive Cross Sections in pp Collisions K. Goulianos

TOTEM vs PYTHIA8-MBR Collisions

Diffractive Cross Sections in pp Collisions K. Goulianos

ALICE tot-inel vs PYTHIA8-MBR Collisions

Diffractive Cross Sections in pp Collisions K. Goulianos

Difractive x-sections Collisions

a1=0.9, a2=0.1, b1=4.6 GeV-2, b2=0.6 GeV-2, s′=s e-Dy, k=0.17, kb2(0)=s0, s0=1 GeV2, s0=2.82 mb or 7.25 GeV-2

Diffractive Cross Sections in pp Collisions K. Goulianos

Difractive x-sections of Collisions√s

- Supress x-sections at small gaps by a factor S using the error function with DyS=2 for SD and DD, and Dy=Dy1+Dy2 =2 for CD (DPE).

Diffractive Cross Sections in pp Collisions K. Goulianos

ALICE SD and DD vs PYTHIA8-MBR Collisions

Diffractive Cross Sections in pp Collisions K. Goulianos

SD and DD at 7 TeV MBR vs PYTHIA8-4C Collisions

- The differences between the PYTHIA8(4C) and MBR predictions are mainly due to the (1/M2)1+e behavior, with e=1.104 in MBR vs 1,08 in PYTHIA8(4C).

Diffractive Cross Sections in pp Collisions K. Goulianos

CD (DPE) x-sections at 7 TeV versus (a) CollisionsDy=Dy1+Dy2 and (b) Dy1

- Both figures are MBR predictions with a Dy=2 cut-off in the error function.
- The normalization is absolute with no model uncertainty other than that due to the determination of the parameters in the formulas as determined from data

Diffractive Cross Sections in pp Collisions K. Goulianos

SUMMARY Collisions introduction

- The ENORM (renormalization model) soft pp cross sections previously used in MBR (Minimum Bias Rockefeller) simulation are adapted to PYTHIA8.
- MBR was successful at Fermilab in fixed target and collider experiments.

- RENORM predictions are based on a parton-model approach, in which diffraction is derived from inclusive PDFs and color factors.
- Diffractive cross sections and final states are both predicted:
- Cross sections vs gap width or vs forward-momentum loss of proton(s):
- Absolutenormalization!

- Hadronization of dissociated proton:
- A (non-perturbative) “quark string” is introduced and tuned to reproduce the MBR multiplicity and pT distributions.
- dN/dh, pT, and particle ID: new in this PYTHIA8 implementation
- (the original MBR simulation produced only p± and p0).

- Unique unitarization based on a saturated “glue-ball” exchange.

- Cross sections vs gap width or vs forward-momentum loss of proton(s):
- Total Cross section ~ln2s based on a glue-ball-like saturated-exchange.
- Immune to eikonaalization-model dependences.

Thank you for your attention

Diffractive Cross Sections in pp Collisions K. Goulianos

References in arXiv:1205.1446v2 [hep-ph] Collisions

multiplicities

Diffractive Cross Sections in pp Collisions K. Goulianos

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