Can a chaos solution in QCD evolution equation restrain high energy collider physics? - PowerPoint PPT Presentation

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Can a chaos solution in QCD evolution equation restrain high energy collider physics?

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Title: Can a chaos solution in QCD evolution equation restrain high energy collider physics?


1
Can a chaos solution in QCD evolution equation
restrain high energy collider physics?
  • ??, ???, ???
  • East China Normal University

2
LHC - THE LARGE HADRON COLLIDER
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1
5
The kinematic domains probed by the various
experiments, shown together with the partons that
they constrain
6
Gluon 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
8
QCD????????
9
QCD 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
10
Fusion
Corrections of Gluon Fusion
DGLAP BFKL
DGLAP GLR-MQ-ZRS BFKL BK
to
3
11
DGLAP Equation
  • Dokshitzer-Gribov-Lipatov 1975
  • Altarelli-Parisi 1977

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BFKL Equation
  • Balitsky-Fadin-Kuraev-Lipatov 1975-1978

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GLR-MQ-ZRS Equation
  • Gribov-Levin-Ryskin 1983

16
Where is the GLR equations?
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Mueller-Qiu 1986
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Zhu-Ruan-Shen 1999-2005
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BK Equation
  • Balitsky-Kovchegov 1996-2000

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JIMWLK Equation
  • Jalilia-Marian, Iancu,McLerra,Weigert,Leonidov
    and Kovne 1997-2001

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Color Glass Condensation
29
From saturation scale QS2, QCD evolution is
stopped
Saturation Scale
DGLAP
MD-DGLAP
JIMWLK
TRUE ?
Qs2 ?
30
?????????????
31
DGLAP amplitude (for gluon)
Impulse approximation
  • At small x and fixed Q2, beyond impulse
    approximation

What will happen?
32
BFKL
DGLAP
Modified BFKL
GLR-MQ-ZRS
33
QCD, Parton Model, Tree Level


a
b
c


e
d
2


f
Beyond impulse approximation
34
Some Results
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??
  • ????
  • ?????????,?????

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?????"??"
  • ?????????????
  • 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)

42
Time 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.

43
MD-BFKL Equation NEW
44
Consistency 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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Schematic kinematic regions of four evolution
equations
49
Solutions 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

50
Input distribution
51
Gluon disappearance bellower the saturation
region.
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Lyapunov exponents
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The rapid increase of the gluon density with
increasing energy will be stopped due to the
gluon disappearance when xltx_c
61
Discussions
  • 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.

62
Will 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.

63
In summary
  • ???????????????????????
  • QCD???????????????????
  • DGLAP, BFKL, GLR-MQ-ZRS, BK??
  • ?????????
  • . ?????????????????????QCD????MD-BFKL??.

64
?MD-BFKL?????????????????Choas.
  • ????????x???????,???????????????????????
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