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  • A measurement of the proton...
    Ahmed, T.; Aid, S.; Akhundov, a A.; Andreev, V.; Andrieu, B.; Appuhn, R D.; Arpagaus, M.; Babaev, A.; Baehr, J.; Ban, J.; Baranov, P.; Barrelet, E.; Bartel, W.; Barth, M.; Bassler, U.; Beck, H P.; Behrend, H J.; Belousov, A.; Berger, C.; Bergstein, H.; Bernardi, G.; Bernet, R.; Bertrand-Coremans, G.; Besancon, M.; Beyer, R.; Bizot, J C.; Blobel, V.; Borras, K.; Botterweck, F.; Boudry, V.; Braemer, A.; Brasse, F.; Braunschweig, W.; Brisson, V.; Bruncko, D.; Brune, C.; Buchholz, R.; Buengener, L.; Buerger, J.; Bsser, F W.; Buniatian, A.; Burke, S.; Burton, M.; Buschhorn, G.; Campbell, a J.; Carli, T.; Charles, F.; Clarke, D.; Clegg, a B.; Clerbaux, B.; Colombo, M.; Contreras, J G.; Cormack, C.; Coughlan, J A.; Courau, A.; Coutures, C.; Cozzika, G.; Criegee, L.; Cussans, D G.; Cvach, J.; Dagoret, S.; Dainton, J B.; Danilov, M.; Dau, W D.; Daum, K.; David, M.; Deffur, E.; Delcourt, B.; del Buono, L.; de Roeck, A.; de Wolf, E A.; Di Nezza, P.; Dollfus, C.; Dowell, J D.; Dreis, H.B.; Droutskoi, A.; Duboc, J.; Dllmann, D.; Dnger, O.; Duhm, H.; Ebert, J.; Ebert, T R.; Eckerlin, G.; Efremenko, V.; Egli, S.; Erlichmann, H.; Eichenberger, S.; Eichler, R.; Eisele, F.; Eisenhandler, E.; Ellison, R J.; Elsen, E.; Erdmann, M.; Erdmann, W.; Evrard, E.; Favart, L.; Fedotov, A.; Feeken, D.; Felst, R.; Feltesse, J.

    Nuclear physics. B, 04/1995, Volume: 439
    Journal Article

    A measurement of the proton structure function F_{\!2}(x,Q^2) is reported for momentum transfer squared Q^2 between 4.5 GeV^2 and 1600 GeV^2 and for Bjorken x between 1.8\cdot10^{-4} and 0.13 using data collected by the HERA experiment H1 in 1993. It is observed that F_{\!2} increases significantly with decreasing x, confirming our previous measurement made with one tenth of the data available in this analysis. The Q^2 dependence is approximately logarithmic over the full kinematic range covered. The subsample of deep inelastic events with a large pseudo-rapidity gap in the hadronic energy flow close to the proton remnant is used to measure the "diffractive" contribution to F_{\!2}.