Light front quantization: Difference between revisions

Revision as of 03:20, 31 December 2017

Revision as of 03:23, 31 December 2017

Line 146:

journal=[[Physics Reports]] | volume= 8 | pages= 75–172 | year=1973 |

doi= 10.1016/0370-1573(73)90009-4|bibcode = 1973PhR.....8...75K }}</ref>

(see [[#Infinite momentum frame]] )

The same results are obtained in the front

form for any frame; e.g., the structure functions and other

Line 156:

doi= 10.1103/PhysRevD.69.076001|arxiv = hep-ph/0311218 |bibcode = 2004PhRvD..69g6001B }}</ref>

the eigensolution of the light-front

Hamiltonian. The [[James Bjorken|Bjorken]] kinematic variable <math>x_{bj}</math> of deep

inelastic scattering becomes identified with the light-front fraction at small

<math>x</math>. The Balitsky-Fadin-Kuraev-LipatovBalitsky–Fadin–Kuraev–Lipatov

(BFKL)<ref name="Fadin:1998py">{{ cite journal |author1=V. S. Fadin |author2=L. N. Lipatov |

title= BFKL pomeron in the next-to-leading approximation |

Line 172:

arxiv=hep-ph/9910492|bibcode = 1999AcPPB..30.3679S }}</ref>

of structure functions and the

Efremov–Radyushkin–Brodsky–Lepage (ERBL)

Efremov-Radyushkin-Brodsky-Lepage (ERBL)

evolution<ref name="Lepage:1980fj">{{ cite journal |author1=G. P. Lepage |author2=S. J. Brodsky |

title= Exclusive Processes in Perturbative Quantum Chromodynamics |