Quark model description of low energy proton—antiproton annihilation into two mesons

1985 ◽  
Vol 152 (5-6) ◽  
pp. 303-307 ◽  
Author(s):  
M. Kohno ◽  
W. Weise
1995 ◽  
Vol 588 (4) ◽  
pp. 783-800 ◽  
Author(s):  
R. Thierauf ◽  
T. Gutsche ◽  
Y. Yan ◽  
A. Muhm ◽  
Amand Faessler

1996 ◽  
Vol 386 (1-4) ◽  
pp. 50-54
Author(s):  
E. Bauer ◽  
T. Gutsche ◽  
A. Muhm ◽  
R. Thierauf ◽  
Y. Yan ◽  
...  

1983 ◽  
Vol 124 (6) ◽  
pp. 443-445 ◽  
Author(s):  
M. Lacombe ◽  
B. Loiseau ◽  
B. Moussallam ◽  
R. Vinh Mau

1963 ◽  
Vol 3 (7) ◽  
pp. 334-335 ◽  
Author(s):  
J.G. Loken ◽  
M. Derrick

1972 ◽  
Vol 5 (5) ◽  
pp. 1217-1219 ◽  
Author(s):  
R. Bizzarri ◽  
P. Guidoni ◽  
F. Marzano ◽  
E. Castelli ◽  
M. Sessa

1991 ◽  
Vol 535 (3-4) ◽  
pp. 651-668 ◽  
Author(s):  
J. Carbonell ◽  
O.D. Dalkarov ◽  
K.V. Protasov ◽  
I.S. Shapiro

2020 ◽  
Vol 56 (9) ◽  
Author(s):  
Gábor Balassa ◽  
György Wolf

Abstract In this work, we extended our statistical model with charmed and bottomed hadrons, and fit the quark creational probabilities for the heavy quarks, using low energy inclusive charmonium and bottomonium data. With the finalized fit for all the relevant types of quarks (up, down, strange, charm, bottom) at the energy range from a few GeV up to a few tens of GeV’s, the model is now considered complete. Some examples are also given for proton–proton, pion–proton, and proton–antiproton collisions with charmonium, bottomonium, and open charm hadrons in the final state.


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