000315894 001__ 315894
000315894 003__ SzGeCERN
000315894 005__ 20230114021817.0
000315894 0247_ $$2DOI$$a10.1016/S0550-3213(96)00673-6
000315894 0248_ $$aoai:cds.cern.ch:315894$$pcerncds:FULLTEXT$$pcerncds:CERN:FULLTEXT$$pcerncds:CERN
000315894 037__ $$9arXiv$$ahep-ex/9611022$$chep-ex
000315894 035__ $$9SPIRES$$a3464202
000315894 035__ $$9arXiv$$aoai:arXiv.org:hep-ex/9611022
000315894 035__ $$9Inspire$$a426595
000315894 041__ $$aeng
000315894 084__ $$2PACS$$a13.60.-r
000315894 084__ $$2PACS$$a13.60.Hb
000315894 100__ $$aArneodo, M.$$uINFN, Turin$$uTurin U.$$vTorino University and INFN, Turin, Italy
000315894 110__ $$aCERN. Geneva
000315894 245__ $$aAccurate measurement of $F_{2}^{\rm d}/F_{2}^{\rm p}$ and $R^{\rm d} - R^{\rm p}$
000315894 269__ $$c28 Nov 1996
000315894 260__ $$c1997
000315894 300__ $$a29 p
000315894 340__ $$apaper
000315894 500__ $$9arXiv$$a29 pages, LateX, including figures, prepared with uufiles, arriving with .sty files as used, figures .eps files and a table .tex file. Accepted for publication in Nucl.Phys.B 1997
000315894 520__ $$aResults are presented for $F_{2}^{\rm d}/F_{2}^{\rm p}$ and $R^{\rm d} - R^{\rm p}$ from simultaneous measurements of deep inelastic muon scattering on hydrogen and deuterium targets, at 90, 120, 200 and 280 GeV. The difference $R^{\rm d} - R^{\rm p}$, determined in the range $0.002<x<0.4$ at an average $Q^{2}$ of 5 GeV$^{2}$, is compatible with zero. The $x$ and $Q^{2}$ dependence of $F_{2}^{\rm d}/F_{2}^{\rm p}$ was measured in the kinematic range $0.001<x<0.8$ and $0.1<Q^{2}<145$ GeV$^{2}$ with small statistical and systematic errors. For $x>0.1$ the ratio decreases with $Q^{2}$.
000315894 520__ $$9HEPDATA$$hCERN-SPS. Measurement of the ratio of structure functions F2 in deep inelastic muon scattering from deuterium and hydrogen and the difference in R, the ratio of the longitudinally to transversely polarized virtual photon absorption cross sections. Data are an average of the incident beam energies, 90, 120, 200, and 280 GeV and cover the x region 0.002 to 0.4 for R at an average Q**2 of 5 GeV**2 and 0.001 to 0.8 for the structure function ratio at Q**2 from 0.1 to 145 GeV**2. These data supercede previously published NMC data.
000315894 520__ $$9Elsevier$$aResults are presented for F 2 d / F 2 p and R d − R p from simultaneous measurements of deep inelastic muon scattering on hydrogen and deuterium targets, at 90, 120, 200 and 280 GeV. The difference R d − R p , determined in the range 0.002 < x < 0.4 at an average Q 2 of 5 GeV 2 , is compatible with zero. The x and Q 2 dependence of F 2 d / F 2 p was measured in the kinematic range 0.001 < x < 0.8 and 0.1 < Q 2 < 145 GeV 2 with small statistical and systematic errors. For x > 0.1 the ratio decreases with Q 2 .
000315894 520__ $$9arXiv$$aResults are presented for F2d/F2p and Rd-Rp from simultaneous measurements of deep inelastic muon scattering on hydrogen and deuterium targets, at 90, 120, 200 and 280 GeV. The difference Rd-Rp, determined in the range 0.002<x<0.4 at an average Q^2 of 5 GeV^2, is compatible with zero. The x and Q^2 dependence of F2d/F2p was measured in the kinematic range 0.001<x<0.8 and 0.1<Q^2<145 GeV^2 with small statistical and systematic errors. For x>0.1 the ratio decreases with Q^2.
000315894 542__ $$fCopyright @ unknown. Published by Elsevier B.V.
000315894 595__ $$aLANL EDS
000315894 65017 $$2SzGeCERN$$aParticle Physics - Experiment
000315894 65027 $$2arXiv$$aNuclear Physics - Experiment
000315894 65027 $$2arXiv$$bParticle Physics - Phenomenology
000315894 693__ $$aCERN SPS$$eSMC NA47
000315894 695__ $$9LANL EDS$$aHigh Energy Physics - Experiment
000315894 690C_ $$aCERN
000315894 690C_ $$aARTICLE
000315894 700__ $$aArvidson, A.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aBadełek, B.$$uUppsala U.$$uWarsaw U.$$vUppsala University, Uppsala, Sweden$$vWarsaw University, Warsaw, Poland 3
000315894 700__ $$aBallintijn, M.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aBaum, G.$$uBielefeld, ZiF$$vBielefeld University, Bielefeld, Germany 1 1 Supported by Bundesministerium für Bildung und Forschung.
000315894 700__ $$aBeaufays, J.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aBird, I.G.$$uHeidelberg, Max Planck Inst.$$uNWO, The Hague$$uNikhef, Amsterdam$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aBjörkholm, P.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aBotje, M.$$uPSI, Villigen$$vPaul Scherrer Institut, Villigen, Switzerland
000315894 700__ $$aBroggini, C.$$vNeuchâtel University, Neuchâtel, Switzerland
000315894 700__ $$aBrückner, W.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aBrüll, A.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$aBurger, W.J.$$uPSI, Villigen$$vPaul Scherrer Institut, Villigen, Switzerland
000315894 700__ $$aCiborowski, J.$$uWarsaw U.$$vWarsaw University, Warsaw, Poland 3
000315894 700__ $$avan Dantzig, R.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aDyring, A.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aEngelien, H.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$aFerrero, M.I.$$uINFN, Turin$$uTurin U.$$vTorino University and INFN, Turin, Italy
000315894 700__ $$aFluri, L.$$vNeuchâtel University, Neuchâtel, Switzerland
000315894 700__ $$aGaul, U.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aGranier, T.$$uIRFU, SPP, Saclay$$vSaclay DAPNIA/SPP, Saclay, France 4 4 Laboratory of CEA, Direction des Sciences de la Matière.
000315894 700__ $$aGrosse-Perdekamp, M.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$avon Harrach, D.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$avan der Heijden, M.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aHeusch, C.$$uUC, Santa Cruz$$vUniversity of California, Santa Cruz, USA
000315894 700__ $$aIngram, Q.$$uPSI, Villigen$$vPaul Scherrer Institut, Villigen, Switzerland
000315894 700__ $$ade Jong, M.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aKabuβ, E.M.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aKaiser, R.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$aKetel, T.J.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aKlein, F.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aKullander, S.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aLandgraf, U.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$aLindqvist, T.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aMallot, G.K.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aMariotti, C.$$uINFN, Turin$$uTurin U.$$vTorino University and INFN, Turin, Italy
000315894 700__ $$avan Middelkoop, G.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aMilsztajn, A.$$uIRFU, SPP, Saclay$$vSaclay DAPNIA/SPP, Saclay, France 4 4 Laboratory of CEA, Direction des Sciences de la Matière.
000315894 700__ $$aMizuno, Y.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aMost, A.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aMücklich, A.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aNassalski, J.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aNowotny, D.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aOberski, J.$$uNWO, The Hague$$uNikhef, Amsterdam$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aPaić, A.$$vNeuchâtel University, Neuchâtel, Switzerland
000315894 700__ $$aPeroni, C.$$uINFN, Turin$$uTurin U.$$vTorino University and INFN, Turin, Italy
000315894 700__ $$aPovh, B.$$uHeidelberg, Max Planck Inst.$$uHeidelberg U.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1$$vHeidelberg University, Heidelberg, Germany 1
000315894 700__ $$aPrytz, K.$$uUppsala U.$$vUppsala University, Uppsala, Sweden
000315894 700__ $$aRieger, R.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aRith, K.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aRöhrich, K.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aRondio, E.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aRopelewski, L.$$uWarsaw U.$$vWarsaw University, Warsaw, Poland 3
000315894 700__ $$aSandacz, A.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aSanders, D.$$uBielefeld, ZiF$$uFreiburg U.$$uHeidelberg, Max Planck Inst.$$uHeidelberg U.$$uMainz U.$$uUMH, Mons$$uNWO, The Hague$$uNikhef, Amsterdam$$uIRFU, SPP, Saclay$$uUC, Santa Cruz$$uPSI, Villigen$$uINFN, Turin$$uTurin U.$$uUppsala U.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vBielefeld University, Bielefeld, Germany 1 1 Supported by Bundesministerium für Bildung und Forschung.$$vFreiburg University, Freiburg, Germany 1$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1$$vHeidelberg University, Heidelberg, Germany 1$$vMainz University, Mainz, Germany 1$$vMons University, Mons, France$$vNeuchâtel University, Neuchâtel, Switzerland$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.$$vSaclay DAPNIA/SPP, Saclay, France 4 4 Laboratory of CEA, Direction des Sciences de la Matière.$$vUniversity of California, Santa Cruz, USA$$vPaul Scherrer Institut, Villigen, Switzerland$$vTorino University and INFN, Turin, Italy$$vUppsala University, Uppsala, Sweden$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.$$vWarsaw University, Warsaw, Poland 3
000315894 700__ $$aScholz, C.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aSeitz, R.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aSever, F.$$uBielefeld, ZiF$$uNWO, The Hague$$uNikhef, Amsterdam$$vBielefeld University, Bielefeld, Germany 1 1 Supported by Bundesministerium für Bildung und Forschung.$$vNIKHEF, Amsterdam, The Netherlands 2 2 Supported in part by FOM, Vrije Universiteit Amsterdam and NWO.
000315894 700__ $$aShibata, T.-A.$$uHeidelberg U.$$vHeidelberg University, Heidelberg, Germany 1
000315894 700__ $$aSiebler, M.$$uBielefeld, ZiF$$vBielefeld University, Bielefeld, Germany 1 1 Supported by Bundesministerium für Bildung und Forschung.
000315894 700__ $$aSimon, A.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aStaiano, A.$$uINFN, Turin$$uTurin U.$$vTorino University and INFN, Turin, Italy
000315894 700__ $$aSzleper, M.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aTłaczała, W.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aTzamouranis, Y.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 700__ $$aVirchaux, M.$$uIRFU, SPP, Saclay$$vSaclay DAPNIA/SPP, Saclay, France 4 4 Laboratory of CEA, Direction des Sciences de la Matière.
000315894 700__ $$aVuilleumier, J.L.$$vNeuchâtel University, Neuchâtel, Switzerland
000315894 700__ $$aWalcher, T.$$uMainz U.$$vMainz University, Mainz, Germany 1
000315894 700__ $$aWindmolders, R.$$uUMH, Mons$$vMons University, Mons, France
000315894 700__ $$aWitzmann, A.$$uFreiburg U.$$vFreiburg University, Freiburg, Germany 1
000315894 700__ $$aZaremba, K.$$uWarsaw U.$$uWarsaw, Inst. Nucl. Studies$$vSoltan Institute for Nuclear Studies, Warsaw, Poland 3 3 Supported by KBN SPUB Nr 621/E - 78/SPUB/P3/209/94.
000315894 700__ $$aZetsche, F.$$uHeidelberg, Max Planck Inst.$$vMax-Planck Institut für Kernphysik, Heidelberg, Germany 1
000315894 710__ $$gNew Muon Collaboration
000315894 710__ $$5PPE
000315894 773__ $$c3-26$$pNucl. Phys. B$$v487$$y1997
000315894 852__ $$cCERN Central Library$$hhep-ex/9611022
000315894 8564_ $$uhttp://durpdg.dur.ac.uk/cgi-hepdata/hepreac/3464202$$w3464202$$yDURHAM
000315894 8564_ $$81354540$$s16789$$uhttps://cds.cern.ch/record/315894/files/slope.png$$y00008 The slope parameter $b_2=\mbox{d}(F_{2}^{\rm d}/F_{2}^{\rm p})/\mbox{d}\ln Q^2$ as a function of $x$. The error bars represent the statistical uncertainties and the band indicates the size of the systematic errors. The curves are results of perturbative QCD calculations, using NMC structure function data {\protect\cite{nmcqcd}} (solid line) and the combined SLAC and BCDMS data {\protect\cite{virch}} (dashed line). The difference between the two curves is within their systematic uncertainties.
000315894 8564_ $$81354541$$s12184$$uhttps://cds.cern.ch/record/315894/files/deltar.png$$y00003 E140X {\protect\cite{e140x}}. The inner error bars correspond to statistical errors and the full ones to the quadratic sum of statistical and systematic errors; for the E140X results only statistical error bars are given.
000315894 8564_ $$81354542$$s38612$$uhttps://cds.cern.ch/record/315894/files/f2dpxq_a.png$$y00005 The structure function ratio $F_2^{\rm d}/F_2^{\rm p}$ as a function of $Q^2$ for each $x$ bin. The error bars represent the statistical uncertainties and the size of the systematic errors is indicated by the bands.
000315894 8564_ $$81354543$$s39125$$uhttps://cds.cern.ch/record/315894/files/f2dpxq_b.png$$y00006 The structure function ratio $F_2^{\rm d}/F_2^{\rm p}$ as a function of $Q^2$ for each $x$ bin. The error bars represent the statistical uncertainties and the size of the systematic errors is indicated by the bands.
000315894 8564_ $$81354544$$s31308$$uhttps://cds.cern.ch/record/315894/files/comp_3.png$$y00007 Comparison of the present results with the ones from SLAC {\protect\cite{slacnp}} and BCDMS {\protect\cite{bcdmsnp}} for selected $x$ bins. The SLAC data were rebinned in $x$ and $Q^2$. The error bars represent the statistical uncertainties.
000315894 8564_ $$81354545$$s33463$$uhttps://cds.cern.ch/record/315894/files/aufsicht_eng.png$$y00001 The NMC spectrometer for the 1989 data taking. The beam calibration spectrometer is located downstream and not shown.
000315894 8564_ $$81354546$$s300793$$uhttps://cds.cern.ch/record/315894/files/arXiv:hep-ex_9611022.pdf
000315894 8564_ $$81354547$$s20090$$uhttps://cds.cern.ch/record/315894/files/ple665.png$$y00010 (a) Comparison of the $x$ dependence of the present data for $F_{2}^{\rm n}/F_{2}^{\rm p}$ with the results from the E665 collaboration {\protect\cite{e665np}}. The error bars represent the statistical errors and the bands at the bottom indicate the systematic uncertainties.\,\,\,\, (b) The average $Q^2$ of the E665 and the present data versus $x$.
000315894 8564_ $$81354548$$s17308$$uhttps://cds.cern.ch/record/315894/files/f2np_model.png$$y00009 (a) The structure function ratio $F_{2}^{\rm n}/F_{2}^{\rm p}$ as a function of $x$. The error bars represent the statistical errors and the band at the bottom indicates the systematic uncertainty. The numbers given across the top of the figure are the average $Q^2$ values. (b) Model predictions for $\delta/F_2^{\rm p}$, the corrections to $F_{2}^{\rm n}/F_{2}^{\rm p}$ due to shadowing in the deuteron, from ref.\,{\protect\cite{bk}} line(1), ref.\,{\protect\cite{wmshad}} line (2) and ref.\,{\protect\cite{nz}} line (3).
000315894 8564_ $$81354549$$s10774$$uhttps://cds.cern.ch/record/315894/files/explain.png$$y00002 Comparison of $F_{2}^{\rm d}/F_{2}^{\rm p}$ (dashed line) and $\sigma_{\rm d}/\sigma_{\rm p}$ (solid lines) for different incident muon energies of 90, 120, 200 and 280~GeV assuming $\Delta R=0.05$. The ratios are shown as a function of $Q^2$ at $x=0.025$ for the $Q^2$ range covered by the data at each incident energy.
000315894 8564_ $$81354550$$s15988$$uhttps://cds.cern.ch/record/315894/files/deltar_qcd.png$$y00004 Comparison of the present results to predictions from perturbative QCD. The solid line was calculated using the same gluon distribution for the proton and the deuteron, the dashed and dotted ones assuming an increase of $xG$ for the deuteron of 10\% and 20\%, respectively. The numbers given at the bottom of the figure are the average $Q^2$ values for some $x$ bins.
000315894 8564_ $$82338482$$s9563$$uhttps://cds.cern.ch/record/315894/files/fig00000.png$$y00000 noimg: Kinematic cuts applied to the eleven data sets classified by energy and trigger. The scattered muon momentum is indicated by $p'$.: Values of $\Delta R=R^{\rm d}-R^{\rm p}$ determined at $x$ and $\langle Q^2 \rangle$. The calculation of $\langle Q^2 \rangle$ takes into account the sensitivity of the data points to $\Delta R$. In addition the $y$ and $\varepsilon$ range of the data for each $x$ bin are given.: The ratio $F_{2}^{\rm d}/F_{2}^{\rm p}$ and the logarithmic slopes $b_2=\mbox{d}(F_{2}^{\rm d}/F_{2}^{\rm p})/\mbox{d}\ln Q^2$ determined at $x$ and $\langle Q^2 \rangle$.
000315894 916__ $$sn$$w199650
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