Setting the scale for dis at large bjorken x
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Setting the Scale for DIS at Large Bjorken x. Simonetta Liuti University of Virginia INT Workshop, “The Jefferson Laboratory Upgrade to 12 GeV” October 7th, 2009 , USA. Outline. Review DGLAP evolution at large Bjorken x

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Setting the scale for dis at large bjorken x

Setting the Scale for DIS at Large Bjorken x

Simonetta Liuti

University of Virginia

INT Workshop,

“The Jefferson Laboratory Upgrade to 12 GeV”

October 7th, 2009, USA


Outline

Outline

Review DGLAP evolution at large Bjorken x

z-dependent scale gives rise to “large Bjorken x evolution”

Interplay of TMCs, Large Bjorken x evolution,HigherTwists (A. Fantoni)

Nuclear corrections at large Bjorken x

Conclusions/Outlook for the 12 GeV program and beyond…


Interest in large x studies

Interest in Large x Studies

  • Precise determination of PDFs(Jlab + CTEQ studies): extend the domain of validity of PDF global analyses (importance of large x gluons, …)

  • QCD predictions at xBj=1 (Ratio F2n/F2p,…)

  • Parton-Hadron Duality in DIS at large xBj monitors the transition in QCD between the “perturbative” region, where factorization applies to the “non-perturbative” region: consequence of factorization theorems in QCD?

    (L. Frankfurt, J. Collins)

  • Possibility of extracting sat low scale (complementary to GDH sum rule analysis by J.P. Chen and A. Deur)


Large x bj at fixed q 2 implies the continuation of the pqcd curve into the resonance region

Large xBj at fixed Q2 impliesthe continuation of the pQCD curve into the resonance region

Main question: how to continue pQCD curve? What defines the pQCD curve?

Suggested approach

(S.L., R. Ent, C.Keppel, I. Niculescu, PRL 2000)

TMC

Fix the order of the analysis, e.g. NLO and extend curve 

corrections arise that are more important than at low xBj and that point at interesting physics (duality)

Large x structure of

PQCD evolution equations

NNLO and higher…

Higher Twists

Nuclear corrections

(for neutron)


Setting the scale for dis at large bjorken x

All effects need to be taken into account simultaneuosly. Some results from Bianchi, Fantoni, S.L. (PRD, 2003) and Fantoni, S.L. (2006)

n=2

Precise pQCD prediction 

Mn  lnQ2 + NLOrders…

n=4

n=6

n=8

In and Mn calculated using CTEQ


Setting the scale for dis at large bjorken x

Unpolarized Jlab+SLAC data

(I. Niculescu)

Polarized HERMES+Jlab+SLAC data

TMC

Large x Res.


Setting the scale for dis at large bjorken x

New polarized data? (O. Rondon et al.)

O.Rondon


Setting the scale for dis at large bjorken x

Large xBj evolution

(S. Brodsky, SLAC lectures (1979), D. Amati et al., NPB(1980), R. Roberts, “Structure of the Proton”)

S  g2/4=S (k2) at each vertex


Setting the scale for dis at large bjorken x

k’

*q  q’ g

q

k

*

l

g

Invariant mass!

In terms of LC variables

k (k+=zP+,,k-=P-- l-, kT)

Next, write amplitude for

*P  (final quark) + g + X 


Setting the scale for dis at large bjorken x

|Amplitude|2 for *P  (final quark) + g + X 

k’+q

q

k’

l

k

P’

P

If z-dependence in kT integration limit is disregarded


Setting the scale for dis at large bjorken x

kT2=Q2=10 GeV2

z-dependent limit

It matters at large x!


Setting the scale for dis at large bjorken x

As a consequence…

This takes care of the large log term in the Wilson coefficient f. (NLO, MS-bar)

{

The scale that allows one to annihilate the effect of the large ln(1-z) terms at large x at NLO is the invariant mass, W2

Equivalent to a resummation of these terms up to NLO


Setting the scale for dis at large bjorken x

Work in progress based on recent analysis by A.Accardi, J.Qiu, JHEP (2008) that extends range of validity of TMCs approach without introducing mismatches between the x andranges (see Alberto’s talk)

Instead of 1

Join large x evoluion with new treatment of TMCs

A.Accardi, S.L., W.Melnitchouk


Setting the scale for dis at large bjorken x

Once PQCD is taken into account, extract HTs

additive form

F2exp=FPQCD(1+C(x)/Q2)


Setting the scale for dis at large bjorken x

Nuclei (S. Malace’s talk)

 Are HTs isospin dependent? Deviations from PQCD effects

Cp-Cn

NMC data

Alekhin, Kulagin and S.L., PRD (2003)


Setting the scale for dis at large bjorken x

In addition …. Sneeds to be continued at very low Q2

J.P. Chen and A. Deur

GDH analysis

S.L. work in progress

Use this “positively” to

extract S at low scale


Setting the scale for dis at large bjorken x

Towards the Jlab 12 GeV program….The very large and accurate Jlab Hall C set of data has shown that parton hadron duality can be studied in detail: Q2,W2 and longitudinal variables dependences have been analyzed thouroughly

Observation of similarity between “high” and “low”

energy cross sections at the core of strong interaction theory

Theoretical background: starts from Finite Energy Sum Rules

(FESR)

Dolen, Horn and Schmid, PR166(1968)

Is there an interpretation within QCD?

Shifman (2005), Bigi and Uraltsev (2004)

Is there a more general implication from factorization theorems of QCD? Interplay of ISI and FSI Frankfurt (this workshop)


All experimental measurements should be compared

All experimental measurements should be compared….


Conclusions and outlook

Conclusions and Outlook

  • Parton-hadron duality is interesting theoretically: low to high energy connection…

  • Quantitative studies of parton-hadron duality are important in “Global Analyses” but… all aspects including TMCs, LxR, and dynamical HTs need to be included\

  • Interesting to compare unpolarized and polarized results

Thank you!


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