Elegent is hosted by Hepforge, IPPP Durham

t-distributions

pp

√s (GeV2)
23 31 53 200 2760 7000 8000 13000 14000
hadronic amplitude full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
hadronic differential cross-section full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
hadronic slope full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
hadronic phase full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
hadronic rho full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
influence of Coulomb interaction full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
importance of the interference term full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|
difference between SWY and KL formulae full range full range full range full range full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t| low |t|

p̅p

√s (GeV2)
31 53 546 630 1800
hadronic amplitude full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
hadronic differential cross-section full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
hadronic slope full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
hadronic phase full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
hadronic rho full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
influence of Coulomb interaction full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
importance of the interference term full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|
difference between SWY and KL formulae full range full range full range full range full range
low |t| low |t| low |t| low |t| low |t|

b-distributions

pp

√s (GeV2)
23 31 53 200 2760 7000 8000 13000 14000
hadronic amplitude full range full range full range full range full range full range full range full range full range

p̅p

√s (GeV2)
31 53 546 630 1800
hadronic amplitude full range full range full range full range full range

s-distributions

pp

hadronic total cross-section full range
hadronic forward rho full range
hadronic forward slope full range

p̅p

hadronic total cross-section full range
hadronic forward rho full range
hadronic forward slope full range