000030796 001__ 30796
000030796 005__ 20140130021112.0
000030796 037__ $$9arXiv$$aarXiv:0911.3989$$chep-ex
000030796 035__ $$9arXiv$$zoai:arXiv.org:0911.3989
000030796 037__ $$aDESY-09-165
000030796 035__ $$9DESY$$zD10-07481
000030796 035__ $$9SPIRESTeX$$zAaron:2009jy
000030796 100__ $$aAaron, F.D.
000030796 245__ $$aMeasurement of the D*+- Meson Production Cross Section and F(2)**(c c-bar), at High Q**2, in ep Scattering at HERA
000030796 246__ $$9arXiv$$aMeasurement of the D* Meson Production Cross Section and F_2^{ccbar}, at High Q^2, in ep Scattering at HERA
000030796 269__ $$c2009-10
000030796 300__ $$a22
000030796 500__ $$aDedicated to the memory of our dear friend and colleague, Beate Naroska
000030796 520__ $$9arXiv$$aThe inclusive production of D*(2010) mesons in deep-inelastic ep scattering is measured in the kinematic region of photon virtuality 100 < Q^2 < 1000 GeV^2 and inelasticity 0.02 < y < 0.7. Single and double differential cross sections for inclusive D* meson production are measured in the visible range defined by |eta(D*)| < 1.5 and p_T(D*) > 1.5 GeV. The data were collected by the H1 experiment during the period from 2004 to 2007 and correspond to an integrated luminosity of 351 pb^{-1}. The charm contribution, F_2^{ccbar}, to the proton structure function F_2 is determined. The measurements are compared with QCD predictions.
000030796 65017 $$2INSPIRE$$aExperiment-HEP
000030796 690C_ $$2INSPIRE$$aPublished
000030796 695__ $$2INSPIRE$$ap: structure function
000030796 695__ $$2INSPIRE$$aelectron p: deep inelastic scattering
000030796 695__ $$2INSPIRE$$adifferential cross section
000030796 695__ $$2INSPIRE$$aquantum chromodynamics: perturbation theory
000030796 695__ $$2INSPIRE$$aD*(2010): inclusive production
000030796 695__ $$2INSPIRE$$aDESY HERA Stor
000030796 695__ $$2INSPIRE$$aD*(2010): electroproduction
000030796 695__ $$2INSPIRE$$astructure function: charm
000030796 695__ $$2INSPIRE$$achannel cross section
000030796 695__ $$2INSPIRE$$aH1
000030796 695__ $$2INSPIRE$$a318 GeV-cms
000030796 700__ $$aAlexa, C.
000030796 700__ $$aAlimujiang, K.
000030796 700__ $$aAndreev, V.
000030796 700__ $$aAntunovic, B.
000030796 700__ $$aBackovic, S.
000030796 700__ $$aBaghdasaryan, A.
000030796 700__ $$aBarrelet, E.
000030796 700__ $$aBartel, W.
000030796 700__ $$aBegzsuren, K.
000030796 700__ $$aBelousov, A.
000030796 700__ $$aBizot, J.C.
000030796 700__ $$aBoudry, V.
000030796 700__ $$aBozovic-Jelisavcic, I.
000030796 700__ $$aBracinik, J.
000030796 700__ $$aBrandt, G.
000030796 700__ $$aBrinkmann, M.
000030796 700__ $$aBrisson, V.
000030796 700__ $$aBruncko, D.
000030796 700__ $$aBunyatyan, A.
000030796 700__ $$aBuschhorn, G.
000030796 700__ $$aBystritskaya, L.
000030796 700__ $$aCampbell, A.J.
000030796 700__ $$aCantun Avila, K.B.
000030796 700__ $$aCerny, K.
000030796 700__ $$aCerny, V.
000030796 700__ $$aChekelian, V.
000030796 700__ $$aCholewa, A.
000030796 700__ $$aContreras, J.G.
000030796 700__ $$aCoughlan, J.A.
000030796 700__ $$aCozzika, G.
000030796 700__ $$aCvach, J.
000030796 700__ $$aDainton, J.B.
000030796 700__ $$aDaum, K.
000030796 700__ $$aDeak, M.
000030796 700__ $$aDelcourt, B.
000030796 700__ $$aDelvax, J.
000030796 700__ $$aDe Wolf, E.A.
000030796 700__ $$aDiaconu, C.
000030796 700__ $$aDodonov, V.
000030796 700__ $$aDossanov, A.
000030796 700__ $$aDubak, A.
000030796 700__ $$aEckerlin, G.
000030796 700__ $$aEfremenko, V.
000030796 700__ $$aEgli, S.
000030796 700__ $$aEliseev, A.
000030796 700__ $$aElsen, E.
000030796 700__ $$aFalkiewicz, A.
000030796 700__ $$aFavart, L.
000030796 700__ $$aFedotov, A.
000030796 700__ $$aFelst, R.
000030796 700__ $$aFeltesse, J.
000030796 700__ $$aFerencei, J.
000030796 700__ $$aFischer, D.-J.
000030796 700__ $$aFleischer, M.
000030796 700__ $$aFomenko, A.
000030796 700__ $$aGabathuler, E.
000030796 700__ $$aGayler, J.
000030796 700__ $$aGhazaryan, Samvel
000030796 700__ $$aGlazov, A.
000030796 700__ $$aGlushkov, I.
000030796 700__ $$aGoerlich, L.
000030796 700__ $$aGogitidze, N.
000030796 700__ $$aGouzevitch, M.
000030796 700__ $$aGrab, C.
000030796 700__ $$aGreenshaw, T.
000030796 700__ $$aGrell, B.R.
000030796 700__ $$aGrindhammer, G.
000030796 700__ $$aHabib, S.
000030796 700__ $$aHaidt, D.
000030796 700__ $$aHelebrant, C.
000030796 700__ $$aHenderson, R.C.W.
000030796 700__ $$aHennekemper, E.
000030796 700__ $$aHenschel, H.
000030796 700__ $$aHerbst, M.
000030796 700__ $$aHerrera, G.
000030796 700__ $$aHildebrandt, M.
000030796 700__ $$aHiller, K.H.
000030796 700__ $$aHoffmann, D.
000030796 700__ $$aHorisberger, R.
000030796 700__ $$aHreus, T.
000030796 700__ $$aJacquet, M.
000030796 700__ $$aJanssen, X.
000030796 700__ $$aJonsson, L.
000030796 700__ $$aJung, Andreas Werner$$iINSPIRE-00183962
000030796 700__ $$aJung, H.
000030796 700__ $$aKapichine, M.
000030796 700__ $$aKatzy, J.
000030796 700__ $$aKenyon, I.R.
000030796 700__ $$aKiesling, C.
000030796 700__ $$aKlein, M.
000030796 700__ $$aKleinwort, C.
000030796 700__ $$aKluge, T.
000030796 700__ $$aKnutsson, A.
000030796 700__ $$aKogler, R.
000030796 700__ $$aKostka, P.
000030796 700__ $$aKraemer, M.
000030796 700__ $$aKrastev, K.
000030796 700__ $$aKretzschmar, J.
000030796 700__ $$aKropivnitskaya, A.
000030796 700__ $$aKruger, K.
000030796 700__ $$aKutak, K.
000030796 700__ $$aLandon, M.P.J.
000030796 700__ $$aLange, W.
000030796 700__ $$aLastovicka-Medin, G.
000030796 700__ $$aLaycock, P.
000030796 700__ $$aLebedev, A.
000030796 700__ $$aLendermann, V.
000030796 700__ $$aLevonian, S.
000030796 700__ $$aLi, G.
000030796 700__ $$aLipka, K.
000030796 700__ $$aLiptaj, A.
000030796 700__ $$aList, B.
000030796 700__ $$aList, J.
000030796 700__ $$aLoktionova, N.
000030796 700__ $$aLopez-Fernandez, R.
000030796 700__ $$aLubimov, V.
000030796 700__ $$aMakankine, A.
000030796 700__ $$aMalinovski, E.
000030796 700__ $$aMarage, P.
000030796 700__ $$aMarti, Ll.
000030796 700__ $$aMartyn, H.-U.
000030796 700__ $$aMaxfield, S.J.
000030796 700__ $$aMehta, A.
000030796 700__ $$aMeyer, A.B.
000030796 700__ $$aMeyer, H.
000030796 700__ $$aMeyer, H.
000030796 700__ $$aMeyer, J.
000030796 700__ $$aMikocki, S.
000030796 700__ $$aMilcewicz-Mika, I.
000030796 700__ $$aMoreau, F.
000030796 700__ $$aMorozov, A.
000030796 700__ $$aMorris, J.V.
000030796 700__ $$aMozer, M.U.
000030796 700__ $$aMudrinic, M.
000030796 700__ $$aMuller, K.
000030796 700__ $$aMurin, P.
000030796 700__ $$aNaumann, Th.
000030796 700__ $$aNewman, P.R.
000030796 700__ $$aNiebuhr, C.
000030796 700__ $$aNikiforov, A.
000030796 700__ $$aNikitin, D.
000030796 700__ $$aNowak, G.
000030796 700__ $$aNowak, K.
000030796 700__ $$aOlsson, J.E.
000030796 700__ $$aOsman, S.
000030796 700__ $$aOzerov, D.
000030796 700__ $$aPahl, P.
000030796 700__ $$aPalichik, V.
000030796 700__ $$aPanagoulias, I.
000030796 700__ $$aPandurovic, M.
000030796 700__ $$aPapadopoulou, Th.
000030796 700__ $$aPascaud, C.
000030796 700__ $$aPatel, G.D.
000030796 700__ $$aPejchal, O.
000030796 700__ $$aPerez, E.
000030796 700__ $$aPetrukhin, A.
000030796 700__ $$aPicuric, I.
000030796 700__ $$aPiec, S.
000030796 700__ $$aPitzl, D.
000030796 700__ $$aPlacakyte, R.
000030796 700__ $$aPokorny, B.
000030796 700__ $$aPolifka, R.
000030796 700__ $$aPovh, B.
000030796 700__ $$aRadescu, V.
000030796 700__ $$aRahmat, A.J.
000030796 700__ $$aRaicevic, N.
000030796 700__ $$aRaspiareza, A.
000030796 700__ $$aRavdandorj, T.
000030796 700__ $$aReimer, P.
000030796 700__ $$aRizvi, E.
000030796 700__ $$aRobmann, P.
000030796 700__ $$aRoland, B.
000030796 700__ $$aRoosen, R.
000030796 700__ $$aRostovtsev, A.
000030796 700__ $$aRotaru, M.
000030796 700__ $$aRuiz Tabasco, J.E.
000030796 700__ $$aRusakov, S.
000030796 700__ $$aSalek, D.
000030796 700__ $$aSankey, D.P.C.
000030796 700__ $$aSauter, M.
000030796 700__ $$aSauvan, E.
000030796 700__ $$aSchmitt, S.
000030796 700__ $$aSchoeffel, L.
000030796 700__ $$aSchoning, A.
000030796 700__ $$aSchultz-Coulon, H.-C.
000030796 700__ $$aSefkow, F.
000030796 700__ $$aShaw-West, R.N.
000030796 700__ $$aShtarkov, L.N.
000030796 700__ $$aShushkevich, S.
000030796 700__ $$aSloan, T.
000030796 700__ $$aSmiljanic, Ivan$$iINSPIRE-00185795
000030796 700__ $$aSoloviev, Y.
000030796 700__ $$aSopicki, P.
000030796 700__ $$aSouth, D.
000030796 700__ $$aSpaskov, V.
000030796 700__ $$aSpecka, A.
000030796 700__ $$aStaykova, Z.
000030796 700__ $$aSteder, M.
000030796 700__ $$aStella, B.
000030796 700__ $$aStoicea, G.
000030796 700__ $$aStraumann, U.
000030796 700__ $$aSunar, D.
000030796 700__ $$aSykora, T.
000030796 700__ $$aTchoulakov, V.
000030796 700__ $$aThompson, G.
000030796 700__ $$aThompson, P.D.
000030796 700__ $$aToll, T.
000030796 700__ $$aTomasz, F.
000030796 700__ $$aTran, T.H.
000030796 700__ $$aTraynor, D.
000030796 700__ $$aTrinh, T.N.
000030796 700__ $$aTruol, P.
000030796 700__ $$aTsakov, I.
000030796 700__ $$aTseepeldorj, B.
000030796 700__ $$aTurnau, J.
000030796 700__ $$aUrban, K.
000030796 700__ $$aValkarova, A.
000030796 700__ $$aVallee, C.
000030796 700__ $$aVan Mechelen, P.
000030796 700__ $$aVargas Trevino, A.A = Vazdik, Y.
000030796 700__ $$aVinokurova, S.
000030796 700__ $$aVolchinski, V.
000030796 700__ $$avon den Driesch, M.
000030796 700__ $$aWegener, D.
000030796 700__ $$aWissing, Ch.
000030796 700__ $$aWunsch, E.
000030796 700__ $$aZacek, J.
000030796 700__ $$aZalesak, J.
000030796 700__ $$aZhang, Z.
000030796 700__ $$aZhokin, A.
000030796 700__ $$aZimmermann, T.
000030796 700__ $$aZohrabyan, H.
000030796 700__ $$aZomer, F.
000030796 710__ $$gH1 Collaboration
000030796 773__ $$a10.1016/j.physletb.2010.02.024$$c91-100$$pPhys.Lett.$$vB686$$y2010
000030796 8564_ $$uhttp://durpdg.dur.ac.uk/cgi-hepdata/hepreac/8469598$$w8469598$$yDURHAM
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f1a.png$$y00000 a) Distribution of $\Delta m=m(K\pi\pi)-m(K\pi)$ for \dstarpm candidates ($K^\mp \pi^\pm \pi_s^\pm$) and for wrong charge combinations ($K^\pm \pi^\pm \pi_s^\mp$) in the accepted $D^0$ mass window. The fit function is also shown. Comparisons at the detector level between the \dstarpm data sample and the reweighted Monte Carlo models are presented. Background-subtracted distributions are shown as a function of $Q^2$ (b),$p_T(D^*)$ (c) and $\eta(D^*)$ (d).
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f1b.png$$y00001 a) Distribution of $\Delta m=m(K\pi\pi)-m(K\pi)$ for \dstarpm candidates ($K^\mp \pi^\pm \pi_s^\pm$) and for wrong charge combinations ($K^\pm \pi^\pm \pi_s^\mp$) in the accepted $D^0$ mass window. The fit function is also shown. Comparisons at the detector level between the \dstarpm data sample and the reweighted Monte Carlo models are presented. Background-subtracted distributions are shown as a function of $Q^2$ (b),$p_T(D^*)$ (c) and $\eta(D^*)$ (d).
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f1c.png$$y00002 a) Distribution of $\Delta m=m(K\pi\pi)-m(K\pi)$ for \dstarpm candidates ($K^\mp \pi^\pm \pi_s^\pm$) and for wrong charge combinations ($K^\pm \pi^\pm \pi_s^\mp$) in the accepted $D^0$ mass window. The fit function is also shown. Comparisons at the detector level between the \dstarpm data sample and the reweighted Monte Carlo models are presented. Background-subtracted distributions are shown as a function of $Q^2$ (b),$p_T(D^*)$ (c) and $\eta(D^*)$ (d).
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f1d.png$$y00003 a) Distribution of $\Delta m=m(K\pi\pi)-m(K\pi)$ for \dstarpm candidates ($K^\mp \pi^\pm \pi_s^\pm$) and for wrong charge combinations ($K^\pm \pi^\pm \pi_s^\mp$) in the accepted $D^0$ mass window. The fit function is also shown. Comparisons at the detector level between the \dstarpm data sample and the reweighted Monte Carlo models are presented. Background-subtracted distributions are shown as a function of $Q^2$ (b),$p_T(D^*)$ (c) and $\eta(D^*)$ (d).
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2a.png$$y00004 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2b.png$$y00005 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2c.png$$y00006 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2d.png$$y00007 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2e.png$$y00008 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f2f.png$$y00009 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $z(D^*)$, $Q^2$ and $x$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectations of CASCADE (dashed line) and RAPGAP (solid line) are obtained using the parameters as described in section~\ref{simulations}. The band of the HVQDIS prediction (shaded) is obtained using the parameter variation described in section~\ref{uncertainties}. The ratio $R=\sigma_{theory}/\sigma_{data}$ is also shown. In the case of HVQDIS the theoretical uncertainties are taken into account. The inner error bars on the data points at $R=1$ display the relative statistical errors, and the outer error bars show the relative statistical andsystematic uncertainties added in quadrature.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f3.png$$y00010 Double-differential cross sections for \dstarpm production as a function of $y$ in different $Q^2$ bins. For the purpose of presentation the cross sections are multiplied by $Q^4$. The data (closed symbols) are shown with the statistical (inner error bars) and total (full error bars) uncertainties. Predictions from the RAPGAP (solid line) and CASCADE (dashed line) Monte Carlo simulationsand the HVQDIS NLO calculation (shaded area) are also shown.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4a.png$$y00011 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4b.png$$y00012 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4c.png$$y00013 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4d.png$$y00014 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4e.png$$y00015 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f4f.png$$y00016 Differential cross sections for inclusive \dstarpm meson production as a function of $p_T(D^*)$, $\eta (D^*)$, $p^*_T(D^*)$, $Q^2$ and $x$ as measured for $p^*_T(D^*)>2 \, \rm GeV$. The inner error bars indicate the statistical uncertainties, the outer error bars show the statistical and systematic uncertainties added in quadrature. The expectation of HVQDIS (shaded band) is obtained using the parameter variation described in section~\ref{uncertainties}. The prediction in ZMVFNS isrepresented by the hatched band where the uncertainty originates from the scale variation.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f5a.png$$y00017 The charm contribution \ftc\, to the proton structure function. The data (closed symbols) are shown with statistical (inner error bars) and total (full error bars) uncertainties. In a) the data are compared to the H1 measurement of \ftc\, using secondary vertex information (open symbols)~\cite{VTX_H1}, where measurements at \qsq$=300 \, \rm GeV^2$ are shifted to \qsq$=400 \, \rm GeV^2$ using the NLO calculation~\cite{riemersma}. The result of the PDF fit H1PDF2009 (shaded band) is also shown. The uncertainty band accounts for experimental, model and parametrisation uncertainties~\cite{h1f2bulk}. In b) the data are compared to the QCD predictions from the NLO calculation~\cite{riemersma} in FFNS (light thick solid line). The predictions from the global PDF fits MSTW08 at NLO (dashed) and NNLO (dark solid) as well as the results of the ABKM fit~\cite{abkm} at NNLO in FFNS (dotted) andGMVFNS (dashed-dotted) are also shown.
000030796 8564_ $$uhttp://inspirebeta.net/record/837434/files/d09-165f5b.png$$y00018 The charm contribution \ftc\, to the proton structure function. The data (closed symbols) are shown with statistical (inner error bars) and total (full error bars) uncertainties. In a) the data are compared to the H1 measurement of \ftc\, using secondary vertex information (open symbols)~\cite{VTX_H1}, where measurements at \qsq$=300 \, \rm GeV^2$ are shifted to \qsq$=400 \, \rm GeV^2$ using the NLO calculation~\cite{riemersma}. The result of the PDF fit H1PDF2009 (shaded band) is also shown. The uncertainty band accounts for experimental, model and parametrisation uncertainties~\cite{h1f2bulk}. In b) the data are compared to the QCD predictions from the NLO calculation~\cite{riemersma} in FFNS (light thick solid line). The predictions from the global PDF fits MSTW08 at NLO (dashed) and NNLO (dark solid) as well as the results of the ABKM fit~\cite{abkm} at NNLO in FFNS (dotted) andGMVFNS (dashed-dotted) are also shown.
000030796 902__ $$aAachen, Tech. Hochsch.
000030796 902__ $$aVINCA Inst. Nucl. Sci., Belgrade
000030796 902__ $$aBirmingham U.
000030796 902__ $$aBrussels U., IIHE
000030796 902__ $$aAntwerp U.
000030796 902__ $$aBucharest, IFIN-HH
000030796 902__ $$aRutherford
000030796 902__ $$aCracow, INP
000030796 902__ $$aDortmund U.
000030796 902__ $$aDubna, JINR
000030796 902__ $$aDSM, DAPNIA, Saclay
000030796 902__ $$aDESY
000030796 902__ $$aHamburg U.
000030796 902__ $$aHeidelberg, Max Planck Inst.
000030796 902__ $$aHeidelberg U.
000030796 902__ $$aKirchhoff Inst. Phys.
000030796 902__ $$aKosice, IEF
000030796 902__ $$aLancaster U.
000030796 902__ $$aLiverpool U.
000030796 902__ $$aQueen Mary, U. of London
000030796 902__ $$aLund U.
000030796 902__ $$aMarseille, CPPM
000030796 902__ $$aMerida, IPN
000030796 902__ $$aCINVESTAV, IPN
000030796 902__ $$aMoscow, ITEP
000030796 902__ $$aLebedev Inst.
000030796 902__ $$aMunich, Max Planck Inst.
000030796 902__ $$aOrsay, LAL
000030796 902__ $$aEcole Polytechnique
000030796 902__ $$aParis U., VI-VII
000030796 902__ $$aMontenegro U.
000030796 902__ $$aPrague, Inst. Phys.
000030796 902__ $$aCharles U.
000030796 902__ $$aRome III U.
000030796 902__ $$aINFN, Rome3
000030796 902__ $$aSofiya, Inst. Nucl. Res.
000030796 902__ $$aUlan Bator, Inst. Phys. Tech.
000030796 902__ $$aPSI, Villigen
000030796 902__ $$aWuppertal U.
000030796 902__ $$aYerevan Phys. Inst.
000030796 902__ $$aDESY, Zeuthen
000030796 902__ $$aZurich, ETH
000030796 902__ $$aZurich U.
000030796 909CO $$ooai:jdsweb.jinr.ru:30796$$pglobal
000030796 961__ $$x2009-11-22
000030796 961__ $$c2010-08-23
000030796 970__ $$aSPIRES-8469598
000030796 980__ $$aPublished
000030796 980__ $$aarXiv
000030796 980__ $$aCiteable
000030796 980__ $$aCORE
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