Higgs boson production via the Bjorken process ${\mathit{e}}^{+}$${\mathit{e}}^{\mathrm{-}}$→${\mathit{H}}^0$${\mathrm{\mu }}^{+}$${\mathrm{\mu }}^{\mathrm{-}}$ at high energy ${\mathit{e}}^{+}$${\mathit{e}}^{\mathrm{-}}$ colliders

Production of the standard Higgs boson via the Bjorken process, ${\mathit{e}}^{+}$ ${\mathit{e}}^{\mathrm{-}}$→${\mathit{H}}^0$ ${\mathrm{\mu }}^{+}$ ${\mathrm{\mu }}^{\mathrm{-}}$, at the center-of-mass energy √s ≊200 GeV (i.e., for the CERN Large Electron-Positron Collider LEP II) is investigated in detail for a Higgs boson mass ranging from 60 GeV to about 120 GeV. We focus on physical quantities which have not been emphasized so far, including the differential cross sections in the various ${\mathrm{\mu }}^{+}$ (or ${\mathrm{\mu }}^{\mathrm{-}}$) scattering angles (with the remaining angles integrated out completely) and the anticipated charge asymmetry. Numerical results on these quantities, in addition to the total production cross section, are described.