Title: Can a chaos solution in QCD evolution equation restrain high energy collider physics?
1Can a chaos solution in QCD evolution equation
restrain high energy collider physics?
- ??, ???, ???
- East China Normal University
2LHC - THE LARGE HADRON COLLIDER
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5The kinematic domains probed by the various
experiments, shown together with the partons that
they constrain
6Gluon distribution and unintegrated gluon
distribution
- The gluon distributions of the nucleon cannot be
extracted directly from the measured structure
functions in deep inelastic scattering
experiments. - They mainly are predicted by using the QCD
evolution equations.
7?
DGLAP or BFKL
2
8QCD????????
9QCD Evolution Equations
BFKL (by Balitsky, Fadin, Kuraev and Lipatov)
GLR-MQ (by Gribov, Levin and Ryskin , Mueller and
Qiu)
Small x
DGLAP (by Dokshitzer, Gribov, Lipatov, Altarelli
and Parisi )
Modified DGLAP (by Zhu, Ruan and Shen)
JIMWLK (by Jalilian-Marian, Iancu, McLerran,
Weigert, Leonidov and Kovner)
Balitsky-Kovchegov equation
Various versions of the evolution equations based
on the color dipole picture
10Fusion
Corrections of Gluon Fusion
DGLAP BFKL
DGLAP GLR-MQ-ZRS BFKL BK
to
3
11DGLAP Equation
- Dokshitzer-Gribov-Lipatov 1975
- Altarelli-Parisi 1977
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13BFKL Equation
- Balitsky-Fadin-Kuraev-Lipatov 1975-1978
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15GLR-MQ-ZRS Equation
16Where is the GLR equations?
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18Mueller-Qiu 1986
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20Zhu-Ruan-Shen 1999-2005
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22BK Equation
- Balitsky-Kovchegov 1996-2000
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25JIMWLK Equation
- Jalilia-Marian, Iancu,McLerra,Weigert,Leonidov
and Kovne 1997-2001
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2828
Color Glass Condensation
29From saturation scale QS2, QCD evolution is
stopped
Saturation Scale
DGLAP
MD-DGLAP
JIMWLK
TRUE ?
Qs2 ?
30?????????????
31DGLAP amplitude (for gluon)
Impulse approximation
- At small x and fixed Q2, beyond impulse
approximation
What will happen?
32BFKL
DGLAP
Modified BFKL
GLR-MQ-ZRS
33QCD, Parton Model, Tree Level
a
b
c
e
d
2
f
Beyond impulse approximation
34Some Results
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36??
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41?????"??"
- ?????????????
- W. Zhu, Nucl. Phys. B551, 245 (1999).
- W. Zhu and J.H. Ruan, Nucl. Phys. B559,
378(1999). - W. Zhu, Z.Q. Shen and J.H. Ruan, Nucl. Phys.
B692, 417 (2004)
42Time ordred perturbation theory
- The sum of cut graphs is necessary not only for
infrared safety, but also for collecting the
leading contributions and restoring unitarity. - The TOPT-cutting rules are proposed to present
the simple connections among the relating
cut-diagrams including real- and virtual-diagrams.
43MD-BFKL Equation NEW
44Consistency of four evolution equations
- The DGLAP and BFKL equations have the same
evolution dynamics, which evolve on the Q2-axis
and the k_T-plane,respectively. - The MD-DGLAP and MD-BFKL equations also have the
same evolution dynamics , which evolve on the
Q2-axis and the k_T-plane, respectively.
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48 Schematic kinematic regions of four evolution
equations
49Solutions of the MD-BFKL equation
- A stronger shadowing suppresses the gluon density
and even leads to the gluon disappearance bellow
the saturation region. - This unexpected effect is caused by a chaotic
solution of the new equation
50Input distribution
51Gluon disappearance bellower the saturation
region.
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57Lyapunov exponents
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60The rapid increase of the gluon density with
increasing energy will be stopped due to the
gluon disappearance when xltx_c
61Discussions
- Many higher order corrections areneglected, such
as possible mixture of the operators with
different twists, the NLL (next leading
logarithmic) and NLO (next leading order)
corrections, singularities from
non-perturbativeparts in the factorization
procedure.
62Will the chaos effect in the MD-BFKL equation
disappear after further corrections are
considered?
- We could expect that more interesting chaos
phenomena will appear in new MD-BFKL
equation.These phenomena will most be interested
to high energy physics and nonlinear science.
63In summary
- ???????????????????????
- QCD???????????????????
- DGLAP, BFKL, GLR-MQ-ZRS, BK??
- ?????????
- . ?????????????????????QCD????MD-BFKL??.
64?MD-BFKL?????????????????Choas.
- ????????x???????,???????????????????????