Nonlocal Condensate Model for QCD Sum Rules
Ron-Chou Hsieh
Collaborator: Hsiang-nan Liarxiv:0909.4763
2
Outline
Concepts Local and non-local condensates Summary
3
The pion form factor can be written as the convolution of a hard-scattering amplitude and wave function
HT
xHT
Pion form factor
4
ConceptsConcepts
Basic idea : Describing the nonperturbative contribution by a set of phenomenologically effective Feynman rules ------- “quark-hadron duality”.
How to do it ?Dispersion relation : a phenomenological procedure which connect perturbative and non-perturbative corrections with the lowest-lying resonances in the corresponding channels by using of the Borel improved dispersion relations
Borel transformation : a) An improved expansion series
b) Give a selection rule of s0
5
where the state is the exact vacuum which contain non-perturbative information and is axial vector current
Firstly, consider a polarization operator which was defined as the vacuum average of the current product:
Quark-hadron duality
Now, we can insert a complete set of states and the following identity between two currents
6
And with PCAC , we obtain
Here assuming that there exists a threshold value s0 which can separate the matrix element to lowest resonance state and other higher states.
with
7
Dispersion relation
Since the polarization operator can be written as a sum of two independent functions:
with
We then obtain
8
The Borel transformation
The meaning of the Borel transformation becomes clear if we act on a particular term in the power expansion
Act on the Dispersion relation we obtained above, then
9
The choice of s0 in pion form factor for Q2=1.99GeV2
1 .0 1 .5 2 .0 2 .5 3 .00 .1 7 0
0 .1 7 2
0 .1 7 4
0 .1 7 6
0 .1 7 8
M G e V
F
s0 0 .6 9 5
1 .0 1 .5 2 .0 2 .5 3 .00 .1 7 9
0 .1 8 0
0 .1 8 1
0 .1 8 2
0 .1 8 3
0 .1 8 4
0 .1 8 5
M G e V F
s0 0 .7 1 5
10
Local and non-local Local and non-local condensatecondensate
Where does nonperturbtive contribution come from?
11
Operator product expansion
In the QSR approach it is assumed that the confinement effects are sufficiently soft for the Taylor expansion:
12
B.L. Ioffe and A.V. Smilga, NPB216(1983)373-407
Local condensate result of pion form factor
13
The infrared divergence problem
14
In 1986, S. V. Mikhailov and A. V. Radyushkin proposed:
with
Non-local condensate models
A.P. Bakulev, S.V. Mikhailov and N.G. Stefanis, hep-ph/0103119A.P. Bakulev, A.V. Pimikov and N.G. Stefanis, 0904.2304
Other modelsIt has been demonstrated that Λcan be interpreted as the constituent quark mass.---PLB.217, p218(1991); Z.Physics, C68, p451(1995)
15
Compare with the simplest gauge invariant non-local condensate :
Must obey following constrain condition
16
Local condensate:
Nonlocal condensate:
17
Free propagator and exact propagatorFree propagator and exact propagator
An exact propagator :
The Wick theorem :
The normal ordering :
18
The Källén-Lehmann representation
The exact fermion’s propagator :
Non-perturbative part (normal ordering)
Renormalized perturbative part
19
Here means that for s larger than then the lower bound is cs otherwise is
Recast the equation into:
And set the nonperturbative piece as:
20
The quark condensate contribution can be obtained by the normal ordering
The weight functions are parameterized as
21
small s region large s region
m2
m2
s
2
2 scs
22
The dressed propagator for the quark is then given by
With the definitions
Using constrain condition
23
Pion form factor in QSR
24
With the matrix element is given by PCAC:
Again, insert the complete set of states and identity:
25
26
Numerical results
27
28
Pion decay constant in QSR
1 .5 2 .0 2 .5 3 .0 3 .5 4 .0 4 .5 5 .0
0 .1 2 2 5
0 .1 2 3 0
0 .1 2 3 5
0 .1 2 4 0
0 .1 2 4 5
0 .1 2 5 0
M G e V
f
s0 0 .5 9
f 0.1307
29
SummarySummary The infrared divergence problem can be solved by our nonlocal con
densate model. The applicable energy region can be extended to 10 GeV2 in the calc
ulation of pion form factor. The predicted value of pion decay constant is very well. Can we use the Källén-Lehmann representation to improve th
e QSR approach?