Experimental determination of the proton electromagnetic form factor at Q2=12.4(GeV/c)2

1992 ◽  
Author(s):  
T. Armstrong ◽  
D. Bettoni ◽  
V. Bharadwaj ◽  
C. Biino ◽  
G. Borreani ◽  
...  

1997 ◽  
Vol 36 (24) ◽  
pp. 6009 ◽  
Author(s):  
Sang Whoe Dho ◽  
Young Je Park ◽  
Hong Jin Kong




2016 ◽  
Vol 119 ◽  
pp. 25020
Author(s):  
Zhenzhu Wang ◽  
Zongming Tao ◽  
Dong Liu ◽  
Chenbo Xie ◽  
Yingjian Wang


1973 ◽  
Vol 44 (4) ◽  
pp. 393-396 ◽  
Author(s):  
M. Bernardini ◽  
D. Bollini ◽  
P.L. Brunini ◽  
E. Fiorentino ◽  
T. Massam ◽  
...  




2006 ◽  
Vol 21 (40) ◽  
pp. 3021-3030 ◽  
Author(s):  
F. CARVALHO ◽  
A. A. NATALE ◽  
C. M. ZANETTI

We use the QCD pomeron model proposed by Landshoff and Nachtmann to compute the differential and the total cross-sections for pp scattering in order to discuss a QCD-based approach to the proton form factor. This model is quite dependent on the experimental electromagnetic form factor, and it is not totally clear why this form factor gives good results even at moderate transferred momentum. We exchange the electromagnetic form factor by the asymptotic QCD proton form factor determined by Brodsky and Lepage (BL) plus a prescription for its low energy behavior dictated by the existence of a dynamically generated gluon mass. We fit the data with this QCD inspired form factor and a value for the dynamical gluon mass consistent with the ones determined in the literature. Our results also provide a determination of the proton wave function at the origin, which appears in the BL form factor.



2020 ◽  
Vol 80 (12) ◽  
Author(s):  
M. Albaladejo ◽  
◽  
I. Danilkin ◽  
S. Gonzàlez-Solís ◽  
D. Winney ◽  
...  

AbstractIn light of recent experimental results, we revisit the dispersive analysis of the $$\omega \rightarrow 3\pi $$ ω → 3 π decay amplitude and of the $$\omega \pi ^0$$ ω π 0 transition form factor. Within the framework of the Khuri–Treiman equations, we show that the $$\omega \rightarrow 3\pi $$ ω → 3 π Dalitz-plot parameters obtained with a once-subtracted amplitude are in agreement with the latest experimental determination by BESIII. Furthermore, we show that at low energies the $$\omega \pi ^0$$ ω π 0 transition form factor obtained from our determination of the $$\omega \rightarrow 3\pi $$ ω → 3 π amplitude is consistent with the data from MAMI and NA60 experiments.





1983 ◽  
Vol 73 (4) ◽  
pp. 347-363 ◽  
Author(s):  
G. Bassompierre ◽  
M. A. Schneegans ◽  
G. Binder ◽  
G. Gissinger ◽  
S. Jacquey ◽  
...  


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