Above 104 GeV/c projectile momenta, the total cross-sections for pp and( p) ̅ p collisions as a function of laboratory beam momentum and center of mass energy, are independent. In the range, 0.1 up to 104 GeV/c the total cross-section depends on the nature of the interacting particles and on the geometrical interpretations in terms of the impact parameter. This could explain in terms of the Quantum Molecular Dynamic QMD model and its ultra relativistic approach UrQMD, in terms of the isospin of the colliding particles, their flavor, and center of mass energies. The model can give also a qualitative success for such dependencies for π^+ p and k^+ p interactions.
Published in | International Journal of High Energy Physics (Volume 1, Issue 1) |
DOI | 10.11648/j.ijhep.20140101.12 |
Page(s) | 6-12 |
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Total Cross-Section, Meson, Proton, Collisions
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APA Style
Ahmed Mohamed Abdalla. (2014). Relativistic Meson-Proton and Proton-Proton Cross- Sections and Quantum Molecular Dynamics Model. International Journal of High Energy Physics, 1(1), 6-12. https://doi.org/10.11648/j.ijhep.20140101.12
ACS Style
Ahmed Mohamed Abdalla. Relativistic Meson-Proton and Proton-Proton Cross- Sections and Quantum Molecular Dynamics Model. Int. J. High Energy Phys. 2014, 1(1), 6-12. doi: 10.11648/j.ijhep.20140101.12
AMA Style
Ahmed Mohamed Abdalla. Relativistic Meson-Proton and Proton-Proton Cross- Sections and Quantum Molecular Dynamics Model. Int J High Energy Phys. 2014;1(1):6-12. doi: 10.11648/j.ijhep.20140101.12
@article{10.11648/j.ijhep.20140101.12, author = {Ahmed Mohamed Abdalla}, title = {Relativistic Meson-Proton and Proton-Proton Cross- Sections and Quantum Molecular Dynamics Model}, journal = {International Journal of High Energy Physics}, volume = {1}, number = {1}, pages = {6-12}, doi = {10.11648/j.ijhep.20140101.12}, url = {https://doi.org/10.11648/j.ijhep.20140101.12}, eprint = {https://article.sciencepublishinggroup.com/pdf/10.11648.j.ijhep.20140101.12}, abstract = {Above 104 GeV/c projectile momenta, the total cross-sections for pp and( p) ̅ p collisions as a function of laboratory beam momentum and center of mass energy, are independent. In the range, 0.1 up to 104 GeV/c the total cross-section depends on the nature of the interacting particles and on the geometrical interpretations in terms of the impact parameter. This could explain in terms of the Quantum Molecular Dynamic QMD model and its ultra relativistic approach UrQMD, in terms of the isospin of the colliding particles, their flavor, and center of mass energies. The model can give also a qualitative success for such dependencies for π^+ p and k^+ p interactions.}, year = {2014} }
TY - JOUR T1 - Relativistic Meson-Proton and Proton-Proton Cross- Sections and Quantum Molecular Dynamics Model AU - Ahmed Mohamed Abdalla Y1 - 2014/03/20 PY - 2014 N1 - https://doi.org/10.11648/j.ijhep.20140101.12 DO - 10.11648/j.ijhep.20140101.12 T2 - International Journal of High Energy Physics JF - International Journal of High Energy Physics JO - International Journal of High Energy Physics SP - 6 EP - 12 PB - Science Publishing Group SN - 2376-7448 UR - https://doi.org/10.11648/j.ijhep.20140101.12 AB - Above 104 GeV/c projectile momenta, the total cross-sections for pp and( p) ̅ p collisions as a function of laboratory beam momentum and center of mass energy, are independent. In the range, 0.1 up to 104 GeV/c the total cross-section depends on the nature of the interacting particles and on the geometrical interpretations in terms of the impact parameter. This could explain in terms of the Quantum Molecular Dynamic QMD model and its ultra relativistic approach UrQMD, in terms of the isospin of the colliding particles, their flavor, and center of mass energies. The model can give also a qualitative success for such dependencies for π^+ p and k^+ p interactions. VL - 1 IS - 1 ER -