Quark-Hadron Duality Cynthia Keppel Hampton University / Jefferson Lab.
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Transcript of Quark-Hadron Duality Cynthia Keppel Hampton University / Jefferson Lab.
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Quark-Hadron Duality
Cynthia Keppel
Hampton University / Jefferson Lab
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“It is fair to say that (short of the full solution of QCD) understanding and controlling the accuracy of quark-hadron duality is one of the most important and challenging problems for QCD practitioners today.”
M. Shifman, Handbook of QCD, Volume 3, 1451 (2001)
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At high energies: interactions between quarks and gluons
become weak(“asymptotic freedom”) efficient description of phenomena afforded in terms of quarks
At low energies: effects of confinement make strongly-coupled QCD highly non-perturbative collective degrees of freedom (mesons and baryons) more
efficient Duality between quark and hadron descriptions
reflects relationship between confinement and asymptotic freedom
intimately related to nature and transition from non-perturbative to perturbative QCD
Duality defines the transition from soft to hard QCD.
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Example: e+e- hadrons /
lim (e+e- X) = NC eq2
E (e+e- +-) q
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Duality in the F2 Structure Function
First observed ~1970 by Bloom and Gilman at SLAC
Bjorken Limit: Q2,
Empirically, DIS region is where logarithmic scaling is observed: Q2 > 5 GeV2, W2 > 4 GeV2
Duality: Averaged over W, logarithmic scaling observed to work also for Q2 > 0.5 GeV2, W2 < 4 GeV2, resonance regime
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What about the other structure functions FL, F1? What about the other structure functions FL, F1? World's L/T Separated Resonance Data (until 2002):World's L/T Separated Resonance Data (until 2002):
Not able to study the Q2 dependence of individual resonance regions!
No resonant behaviour can be observed!
(All data for Q2 < 9 (GeV/c)2)
JLab E94-110: a global survey of longitudinal strength in the resonance region…...
R = L/T
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What about the other structure functions FL, F1? What about the other structure functions FL, F1?
Now able to study the Q2 dependence of individual resonance regions!
Clear resonant behaviour can be observed!
(All data for Q2 < 9 (GeV/c)2)
Now able to extract F2, F1, FL and study duality!...
R = L/T <
R = / T
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Rosenbluth Rosenbluth SeparationsSeparations
180 L/T separations total (most with 4-5 points)
Spread of points about the linear fits is fairly Gaussian with ~ 1.6 %- consistent with the estimated pt-pt experimental uncertainty
a systematic “tour de force”
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Duality now observed in all unpolarized structure functions
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…and in Nuclei (F2)
p
Fe
d
= 2x[1 + (1 + 4M2x2/Q2)1/2]
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Quark-Hadron Duality (F2) in Nuclei
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Duality and the EMC Effect
J. Arrington, et al., in preparation
Medium modifications to the pdfs are the same in the resonance region
Rather surprising (deltas in nuclei, etc.)
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…and in Spin Structure Functions
A1p
g1
HERMES JLab Hall B
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Experimentally, duality holds in all unpolarized structure functions, in tested spin structure functions, even better in nuclei, all down to surprisingly low Q2
Apparently a non-trivial property of nucleon structure
If we had used only scintillators, scaling would be thought to hold
down to low Q2!
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QuantificationIntegral Ratio Res / Scaling
For tomorrow
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QuantificationLarge x Structure Functions
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Close and Isgur Approach
Phys. Lett. B509, 81 (2001):
q = h
Relative photo/electroproduction strengths in SU(6)
“The proton – neutron difference is the acid test for quark-hadron duality.”
How many states does it take to approximate closure?
Proton W~1.5
Neutron W ~ 1.7
n p
e-
The BONUS experiment will measure neutron
structure functions…….
To spectrometer
To recoil detector
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Experimental Setup
Hall B CLAS spectrometer for electron detection
Thin deuterium target (7.5 atm)
Radial Time Projection Chamber (RTPC) for spectator proton detection
DVCS solenoid to contain Moller background
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“Very Important Protons” Deuteron ~ free proton +
free neutron at small nucleon momenta
Will target Tp ~ 2 – 5 MeV spectator protons
30% of momentum distribution is in
chosen ps range
Tp > 5 MeV spectators will also be detected
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RTPC Design
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F2n / F2
p Ratio at Large x – Projected Results
Yellow shaded area represents current theoretical uncertainty
RR data begin the Resonance Region
(W2 > 3 GeV2, Q2 ~ 5)
Gray shaded areas represent systematic uncertainty Light = total Dark = normalized,
point-to-point
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Duality in QCD Moments of the Structure Function
Mn(Q2) = S dx xn-2F(x,Q2)
If n = 2, this is the Bloom-Gilman duality integral! Operator Product Expansion
Mn(Q2) = (nM02/ Q2)k-1 Bnk(Q2)
higher twist logarithmic dependence
(pQCD)
Duality is described in the Operator Product Expansion as higher twist effects being small or cancelling DeRujula, Georgi, Politzer (1977)
0
1
k=1
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0
1
Mn(Q2) = S dx xn-2F(x,Q2)For moments add
elastics……
F2
DualityAbove Q2=1
Below Q2=1,duality breaks
Down (empiricalfits shown)
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n = 2 Moments of Fn = 2 Moments of F22, F, F
11 and F and FLL: : Mn(Q2) = ∫ dx x2-2F(x,Q2)
Elastic Contributions
Flat Q2 dependence small higher twist! - not true for contributions from the elastic peak (bound quarks)
Elastic contribution excluded
DIS: SLAC fit to F2 and R
RES: E94-110 resonance fit
F1EL = G
M2 (x-1)
F2EL = (G
E2 + G
M2 )(x-1)
FL
EL = GE
2 (x-1)
1 +
= q2/4Mp
2
PreliminaryF2
F1
FL
0
1
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n = 4 Moments of Fn = 4 Moments of F22, F, F
11 and F and FLL
Neglecting elastics, n = 4 moments have only a small Q2 dependence as well.
Momentum sum rule
This is only at leading twist and neglecting TM effects.⇒ Must remove TM effects from data to extract moment of xG…we’re working on it…..
Preliminary
ML
(n) = s(Q2){ 4M
2(n) + 2c∫dx xG(x,Q2)}
3(n+1) (n+1)(n+2)
Gluon distributions!
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D. Dolgov et al., Phys. Rev. D 66:034506, 2002
X Data from JLab Hall C
× Current (data) uncertainties are in nuclear extraction of F2
n
Moments are Calculated on the Lattice: F2
n – F2p
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Another approach And some new experiments
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Close and Isgur Approach
Phys. Lett. B509, 81 (2001):
q = h
Relative photo/electroproduction strengths in SU(6)
“The proton – neutron difference is the acid test for quark-hadron duality.”
How many states does it take to approximate closure?
Proton W~1.5
Neutron W ~ 1.7
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Duality in Meson Electroproduction
Duality and factorization possible for Q2,W2 3 GeV2
(Close and Isgur, Phys. Lett. B509, 81 (2001))
d/dz iei2qi(x,Q2)Dqi
m(z,Q2) + qi(x,Q2)Dqim(z,Q2)
Requires non-trivial cancellations of decay angular distributions
If duality is not observed, factorization is questionable
hadronic description quark-gluon description
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(Semi-)Exclusive Meson Electroproduction
Large z = Eh/ to emphasize duality and factorization (Berger criterion)
Meson electroproduced along q, i.e. emphasize forward angles
SHMS in Hall C well suited to detect these mesons (cf. pion form factor)
If Berger criterion and duality factorization
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More of the experimental future
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Separated Unpolarized Structure Functions at 11 GeV
Also necessary for polarized structure function measurements...
x = 0.8
HMS
SHMS
Hall C
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Polarized Structure Functions at 11 GeV
Hall C
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A1
n from 3He(e,e’) JLab Hall A
2
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Summary Quark-hadron duality is a non-trivial property of QCD Soft-Hard Transition! Duality has been shown to hold in all experimental tests thus far
All unpolarized structure functions Polarized structure functions Nuclei
More experiments are planned Neutron Polarized structure functions Neutrino scattering
Duality may provide a valuable tool to access high x regime Duality violations obscure comparison with lattice QCD through the structure
function moments