Abstract
The possible manifestations of new physics indirect effects in the annihilation process of W pair production has been studied. It was shown that the sensitivity of differential cross section to such kind of effects significantly increases with energy in certain kinematical regions (mostly in backward hemisphere of outgoing W boson) due to the enhancement mechanism. (author). 7 refs, 4 figs.
Citation Formats
Pankov, A A, and Paver, N.
On the enhancement mechanism of new physics effects in e{sup +}+e{sup -}{yields}W{sup +}W{sup -}.
IAEA: N. p.,
1991.
Web.
Pankov, A A, & Paver, N.
On the enhancement mechanism of new physics effects in e{sup +}+e{sup -}{yields}W{sup +}W{sup -}.
IAEA.
Pankov, A A, and Paver, N.
1991.
"On the enhancement mechanism of new physics effects in e{sup +}+e{sup -}{yields}W{sup +}W{sup -}."
IAEA.
@misc{etde_10126130,
title = {On the enhancement mechanism of new physics effects in e{sup +}+e{sup -}{yields}W{sup +}W{sup -}}
author = {Pankov, A A, and Paver, N}
abstractNote = {The possible manifestations of new physics indirect effects in the annihilation process of W pair production has been studied. It was shown that the sensitivity of differential cross section to such kind of effects significantly increases with energy in certain kinematical regions (mostly in backward hemisphere of outgoing W boson) due to the enhancement mechanism. (author). 7 refs, 4 figs.}
place = {IAEA}
year = {1991}
month = {Oct}
}
title = {On the enhancement mechanism of new physics effects in e{sup +}+e{sup -}{yields}W{sup +}W{sup -}}
author = {Pankov, A A, and Paver, N}
abstractNote = {The possible manifestations of new physics indirect effects in the annihilation process of W pair production has been studied. It was shown that the sensitivity of differential cross section to such kind of effects significantly increases with energy in certain kinematical regions (mostly in backward hemisphere of outgoing W boson) due to the enhancement mechanism. (author). 7 refs, 4 figs.}
place = {IAEA}
year = {1991}
month = {Oct}
}