Bulten, H.J.Anthony, P.L.Arnold, R.G.Arrington, J.Beise, E.J.Belz, E.van Bibber, K.Bosted, P.E.van den Brand, J.F.J.Chapman, M.S.Coulter, K.P.Dietrich, F.S.Ent, R.Epstein, M.Filippone, B.W.Gao, H.Gearhart, R.A.Geesaman, D.F.Holt, R.J.Jackson, H.E.Jones, C.E.Keppel, C.E.Kinney, E.Kuhn, S.E.Lee, K.Lorenzon, W.Lung, A.Makins, N.C.R.Margaziotis, D.J.McKeown, R.D.Milner, R.G.Mueller, B.Napolitano, J.Nelson, J.O'Neill, T.G.Papavassiliou, V.Petratos, G.G.Rock, S.E.Spengos, M.Szalata, Z.M.Tao, L.H.White, J.L.Zeidman, B.Cross sections are presented for the reaction 2H(e,e′p)n for momentum transfers in the range 1.2≤Q2≤6.8(GeV/c)2 and for missing momenta from 0 to 250 MeV/c. The longitudinal-transverse interference structure function has been separated at Q2 = 1.2(GeV/c)2. The observables are compared to calculations performed in nonrelativistic and relativistic frameworks. The data are best described by a fully relativistic calculation.en-USdeuteriumelectron scatteringArticle