topical seminar on frontier of particle physics 2004: qcd and light hadrons lecture 2
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Topical Seminar on Frontier of Particle Physics 2004: QCD and Light Hadrons Lecture 2. Wei Zhu East China Normal University. Outline of Lecture Two. DGLAP Equations. BFKL Equations. 1. A simplest derivation of DGLAP equations. Bjorken Frame, A + =0. - PowerPoint PPT PresentationTRANSCRIPT
Topical Seminar on Frontier of Particle Physics 2004: QCD and Light Had
rons Lecture 2
Wei ZhuEast China Normal University
2. A simplest derivation of BFKL equationsBjorken fram
eThe virtual probe has almost zero-energy and zero-longitudinal momentum, so that the momentum of the probe is mainly transverse to the nucleon direction.
Resolution of probe
At small x and fixed Q2, beyond impulse approximation
DGLAP amplitude (for gluon)
Impulse approximation
NQ xx
What will happen?
BFKL equation
We separated out the probe vertex using the W -W approximation, where the transverse momenta of initial gluons are unvanished.
Note that z1 >>z2 at the LLA(1/x), we insert δ(z1 -1) and obtain the evolution equation
where y = ln(1/z) and