Electromagnetic proton form factors in largeNcQCD
Author(s) -
C. A. Domínguez,
Teboho L Thapedi
Publication year - 2004
Publication title -
journal of high energy physics
Language(s) - English
Resource type - Journals
SCImago Journal Rank - 0.998
H-Index - 261
eISSN - 1126-6708
pISSN - 1029-8479
DOI - 10.1088/1126-6708/2004/10/003
Subject(s) - quantum chromodynamics , physics , proton , momentum transfer , particle physics , realization (probability) , polarization (electrochemistry) , limit (mathematics) , range (aeronautics) , yield (engineering) , zero (linguistics) , nuclear physics , quantum electrodynamics , quantum mechanics , scattering , mathematics , mathematical analysis , thermodynamics , chemistry , linguistics , statistics , materials science , philosophy , composite material
The electromagnetic form factors of the proton are obtained using aparticular realization of QCD in the large $N_c$ limit (${QCD}_{\infty}$),which sums up the infinite number of zero-width resonances to yield an Euler'sBeta function (Dual-${QCD}_{\infty}$). The form factors $F_1(q^2)$ and$F_2(q^2)$, as well as $G_M(q^2)$ agree very well with reanalyzed space-likedata in the whole range of momentum transfer. In addition, the predicted ratio$\mu_p G_E/G_M$ is in good agreement with recent polarization transfermeasurements at Jefferson Lab.Comment: 10 page
Accelerating Research
Robert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom
Address
John Eccles HouseRobert Robinson Avenue,
Oxford Science Park, Oxford
OX4 4GP, United Kingdom