Title: Onset of Scaling in Exclusive Processes
1Onset of Scaling in Exclusive Processes
Marco Mirazita Istituto Nazionale di Fisica
Nucleare Laboratori Nazionali di Frascati
First Workshop on Quark-Hadron Duality and the
Transition to pQCD Laboratori Nazionali di
Frascati, June 6-8 2005
2Outline
- Asymptotics in exclusive processes counting
rule and helicity conservation - Experimental test of asymptotic predictions in
em reactions - -cross section and polarization data in g d ? p
n - -Form Factors and tensor polarization in e d ? e
d - Comments and outlooks
3Scaling laws for exclusive processes
4Polarization in exclusive reactions
5The counting rule
- There are a large number of measured exclusive
reactions in which the empirical power law
fall-off predicted by dimensional counting pQCD
appear to be accurate over a large range of
momentum transfer - pp?pp p-p?p-p Kp?Kp
- A critical question is the momentum transfer
required such that leading-twist pQCD
contributions dominate. - An efficient way for reaching the hard regime is
the deuteron photodisintegration reaction gd ? pn
6Hard regime in gd ? pn
Already with E1 GeV tN exceeds the nucleon mass
in more realistic pQCD (light-front) calculations
the relevant scale is transverse momentum pT
7g d ? p n at SLAC
New extensive studies at SLAC and JLab
8g d ? p n experimental data
9Check of CCR adopted procedure
10An example
qCM 65o
11Determination of pT threshold
- for central angles
- PTth 1.00 ? 1.27 GeV/c
- ltPTthgt 1.13 GeV/c
- for forward and backward angles
- PTth 0.6 ? 0.7 GeV/c
- PTth uncert. ?100 MeV/c
SCALING THRESHOLD pT 1.1 GeV/c
12Check of CCR
Fit of ds/dt data for the central angles and
PT1.1 GeV/c with A s-11
For all but two of the fits c2? 1.34
- Better c2 at 55o and 75o if different data
- sets are renormalized to each other
- No data at PT1.1 GeV/c at forward and
- backward angles
- Clear s-11 behaviour for last 3 points at 35o
13HHC in gd ?pn
Py 0 (?
t-1) HHC PREDICTIONS Cx 0 (? t-1)
Cz 0 (? t-2)
at 90o
HHC PREDICTION S 1 (? t-2) at 90o
14g d ? p n polarization data
Data at 90o (CM) only
15Elastic ed scattering
16Deuteron FFs
17Scaling of deuteron FFs
18Polarization in ed ? ed
Deuteron tensor polarization tij depend on the
scattering angle
Data at 70 (LAB)
19Comments and Outlook - 1
- CCR is based on dimensional arguments only,
provided that - - energy is high enough
- - partons are free
- Details of QCD strong interactions dont play
any role
- CCR reproduces the general behaviour of the
cross section for several exclusive hadronic
reactions (pp?pp, p-p?p-p, Kp?Kp, )
- Detailed analysis of experimental data shows
that gd?pn cross section agrees with CCR for
central CM angles and pT gt 1.1 GeV
- Deuteron em Form Factors are consistent with CCR
predictions
- More realistic QCD calculations could give non
negligible corrections to the expected scaling.
For example - - oscillations in fixed angle cross sections
- - proton em Form Factors scaling
20Proton Form Factors
Asymptotic scaling Dirac F1 ? Q-4
Pauli F2 ? Q-6 Q2 F2/F1 const
pQCD quark orbital angular momentum (Ralston,
CIPANP 2000, Quebec City) Q F2/F1 const in
agreement with data
21Comments and Outlook - 2
- HHC is less successful in describing
polarization data, even in hadron-hadron reactions
- Polarization observables are more sensitive to
QCD details, corrections could be large
- Experimental data on em reactions seem to
indicate violation of HHC, but the situation is
not sufficiently clear
- More polarization data are needed
- - deuteron photodisintegration at other angles
than 90o - - tensor polarization in ed elastic scattering at
higher Q2
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23Hadronic reactions with deuteron
Uzikov, hep-ph/0503185
dd?3He n dd?3H p
pd?pd
24Polarization in pd elastic scattering
Azhgirey et al., PL 391B,22
25From Hadrons to Partons
The challenge is to look for some experimentally
accessible phenomena naturally predicted by pQCD
Scaling in some physics observables is one of the
simplest signatures of pQCD
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