TY - JOUR
T1 - Relativistic antihydrogen production by pair production with positron capture
AU - Şengül, M. Y.
AU - Güçlü, M. C.
PY - 2012/4
Y1 - 2012/4
N2 - Antihydrogen atoms may rarely be produced by the collision of antiprotons with ions. At relativistic velocities, the antiproton may pass around the Coulomb field of the nucleus and the electronpositron pairs can be produced electromagnetically. After this pair production, not so often, positron can be captured by the antiproton and as a result, antihydrogen atoms may be produced. In this work, we have calculated the antihydrogen production cross section in the framework of perturbation theory, by applying Monte-Carlo integration techniques. In order to compute the lowest-order Feynman diagrams amplitudes, we used Darwin wave functions for the bound states of the positrons and SommerfeldMaue wave functions for the continuum states of the electrons.
AB - Antihydrogen atoms may rarely be produced by the collision of antiprotons with ions. At relativistic velocities, the antiproton may pass around the Coulomb field of the nucleus and the electronpositron pairs can be produced electromagnetically. After this pair production, not so often, positron can be captured by the antiproton and as a result, antihydrogen atoms may be produced. In this work, we have calculated the antihydrogen production cross section in the framework of perturbation theory, by applying Monte-Carlo integration techniques. In order to compute the lowest-order Feynman diagrams amplitudes, we used Darwin wave functions for the bound states of the positrons and SommerfeldMaue wave functions for the continuum states of the electrons.
KW - Antihydrogen production
KW - Monte Carlo calculations
KW - Positron capture
UR - http://www.scopus.com/inward/record.url?scp=84859161226&partnerID=8YFLogxK
U2 - 10.1016/j.ppnp.2012.01.037
DO - 10.1016/j.ppnp.2012.01.037
M3 - Article
AN - SCOPUS:84859161226
SN - 0146-6410
VL - 67
SP - 612
EP - 615
JO - Progress in Particle and Nuclear Physics
JF - Progress in Particle and Nuclear Physics
IS - 2
ER -