ar X iv : h ep - p h / 99 04 44 5 v 3 6 M ay 1 99 9 Muon g − 2 and New Physics

ar X iv : h ep - p h / 99 04 44 5 v 2 2 9 A pr 1 99 9 Muon g − 2 and New Physics

Here we invoke the current and future perspective on muon g −2 measurement when asking what the muon g − 2 could tell about the underlying structure concerning with the hierarchy problem. Here we take up two such models, the presence of which turns out to alter the standard model prediction for muon g − 2 significantly: one is TeV scale gravity scenario, the other supersymmetric model, in the l...

ar X iv : h ep - p h / 99 04 44 5 v 1 2 4 A pr 1 99 9 Muon g − 2 and New Physics

Here we invoke the current and future perspective on muon g −2 measurement when asking what the muon g − 2 could tell about the underlying structure concerning with the hierarchy problem. Here we take up two such models, the presence of which turns out to alter the standard model prediction for muon g − 2 significantly: one is TeV scale gravity scenario, the other supersymmetric model, in the l...

ar X iv : h ep - p h / 98 05 46 8 v 1 2 6 M ay 1 99 8 COURSE HEAVY QUARK PHYSICS

ar X iv : h ep - p h / 99 05 46 9 v 1 2 5 M ay 1 99 9 DESY 99 – 060 hep - ph / 9905469 May 1999 W Boson Production at NLO ∗

We discuss W boson production at HERA including NLO QCD corrections. A detailed comparison with previous work is presented.

ar X iv : h ep - e x / 96 04 01 1 v 1 1 M ay 1 99 6 FACTORIZATION AND COLOR - SUPPRESSION IN HADRONIC B → D ( ∗ ) nπ DECAYS Jorge