Kai Hencken

Exclusive and inclusive muon pair production in collisions of relativistic nuclei

The exclusive production of one

Electron positron pair production in the external electromagnetic field of colliding relativistic heavy ions

{ensuremath{mu}}^{+}{ensuremath{mu}}^{ensuremath{-}}

Testing the electroweak gauge boson coupling in exclusive photoproduction of single W bosons at the LHC

pair in collisions of two ultrarelativistic nuclei is considered. We present a simple method for the calculation of the Born cross section for this process based on an improved equivalent photon approximation. We find that the Coulomb corrections to this cross section (corresponding to multiphoton exchange of the produced

Photon-photon and photon-hadron physics at relativistic heavy ion colliders

{ensuremath{mu}}^{ifmmodepmelsetextpmfi{}}

COHERENT ELECTROMAGNETIC PROCESSES IN RELATIVISTIC HEAVY ION COLLISIONS

with the nuclei) are small, whereas the unitarity corrections (corresponding to the exchange of light-by-light blocks between nuclei) are large. This is in sharp contrast to the exclusive

Continuum excitations in 6He

{e}^{+}{e}^{ensuremath{-}}

Lepton-pair production from deep inelastic scatteringin peripheral relativistic heavy ion collisions

pair production where the Coulomb corrections to the Born cross section are large, whereas the unitarity corrections are small. We calculate also the cross section for the production of one

Numerical Methods in Multivariate Option Pricing

{ensuremath{mu}}^{+}{ensuremath{mu}}^{ensuremath{-}}

Breakup reactions of the halo nuclei 11 Be and 8 B

pair and several

Muon pair production in relativistic nuclear collisions

{e}^{+}{e}^{ensuremath{-}}