D. von Harrach
University of Mainz
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Featured researches published by D. von Harrach.
Nuclear Physics | 1997
M. Arneodo; A. Arvidson; B. Badelek; M. Ballintijn; G. Baum; J. Beaufays; I. Bird; P. Björkholm; Michiel Botje; C. Broggini; W. Brückner; A. Brüll; Wj Burger; J. Ciborowski; R. van Dantzig; A. Dyring; H. Engelien; M.I. Ferrero; L. Fluri; U. Gaul; T. Granier; M. Grosse-Perdekamp; D. von Harrach; M. van der Heijden; C. A. Heusch; Q. Ingram; M. de Jong; E. Kabuß; R. Kaiser; T. Ketel
The muon-proton and muon-deuteron inclusive deep inelastic scattering cross sections were measured in the kinematic range 0.002 < x < 0.60 and 0.5 < Q(2) < 75 GeV2 at incident muon energies of 90, 120, 200 and 280 GeV. These results are based on the full data set collected by the New Muon Collaboration, including the data taken with a small angle trigger. The extracted values of the structure functions F-2(p) and F-2(d) are in good agreement with those from other experiments. The data cover a sufficient range of y to allow the determination of the ratio of the longitudinally to transversely polarised virtual photon absorption cross sections, R = sigma(L)/sigma(T), for 0.002 < x < 0.12. The values of R are compatible with a perturbative QCD prediction; they agree with earlier measurements and extend to smaller x.The muon-proton and muon-deuteron inclusive deep inelastic scattering cross sections were measured in the kinematic range 0.002<x<0.60 and 0.5<Q2<75 GeV2 at incident muon energies of 90, 120, 200 and 280 GeV. These results are based on the full data set collected by the New Muon Collaboration, including the data taken with a small angle trigger. The extracted values of the structure functions F2p and F2d are in good agreement with those from other experiments. The data cover a sufficient range of y to allow the determination of the ratio of the longitudinally to transversely polarised virtual photon absorption cross sections, R= sigma(L)/sigma(T), for 0.002<x<0.12 . The values of R are compatible with a perturbative QCD prediction; they agree with earlier measurements and extend to smaller x.
Physics Letters B | 1992
P. Amaudruz; M. Arneodo; C. Scholz; G. van Middelkoop; H. Engelien; F. Klein; S. Kullander; J.-L. Vuilleumier; U. Krüner; T. Walcher; F. Sever; R. van Dantzig; J. Domingo; R. Schumacher; U. Landgraf; C.H.Quentin Ingram; U. Sennhauser; A. Staiano; M. van der Heijden; M.I. Ferrero; C. Mariotti; D. Nowotny; K. Rith; A. Sandacz; R. Rieger; K. Kurek; J. Drinkard; N. Pavel; A. Brüll; R. Windmolders
The structure functions F2p and F2d measured by deep inelastic muon scattering at incident energies of 90 and 280 GeV are presented. These measurements cover a large kinematic range, 0.006 less-tha ...
Physics Letters B | 1995
M. Arneodo; A. Arvidson; B. Badelek; M. Ballintijn; G. Baum; J. Beaufays; I.G. Bird; P. Björkholm; M. Botje; C. Broggini; W. Brückner; A. Brüll; W.J. Burger; J. Ciborowski; R. van Dantzig; A. Dyring; H. Engelien; M.I. Ferrero; L. Fluri; U. Gaul; T. Granier; M. Grosse-Perdekamp; D. von Harrach; M. van der Heijden; C. A. Heusch; G. Igo; Q. Ingram; M. de Jong; E.M. Kabuß; R. Kaiser
The proton and deuteron structure functions F2p and F2d were measured in the kinematic range 0.006<x<0.6 and 0.5<Q^2<75 GeV^2, by inclusive deep inelastic muon scattering at 90, 120, 200 and 280 GeV. The measurements are in good agreement with earlier high precision results. The present and earlier results together have been parametrised to give descriptions of the proton and deuteron structure functions F2 and their uncertainties over the range 0.006<x<0.9.The proton and deuteron structure funtions F2p and F2d were measured in the kinematic range 0.006 < x < 0.6 and 0.5 < Q2 < 75 GeV2, by inclusive deep inelastic muon scattering at 90, 120, 200 and 280 GeV. The measurements are in good agreement with earlier high precision results. The present and earlier results together have been parametrised to give descriptions of the proton and deuteron structure functions F2 and their uncertainties over the range 0.006 < x < 0.9.
Physics Letters B | 1988
Jg Ashman; B. Badelek; Günter Baum; J. Beaufays; C.P. Bee; C. Benchouk; I. Bird; S.C. Brown; M. C. Caputo; H.W.K. Cheung; J. S. Chima; J. Ciborowski; R.W. Clifft; G. Coignet; F. Combley; G. R. Court; G. D'Agostini; J. Drees; M. Düren; N. Dyce; A. Edwards; M. Edwards; T. Ernst; M.I. Ferrero; David Francis; E. Gabathuler; J. Gajewski; R. Gamet; V. Gibson; J. Gillies
Measurement of the ratios of deep inelastic muon-nucleus cross sections on various nuclei compared to deuterium
Physical Review Letters | 2001
J. Ahrens; M. Lang; S. Goertz; T. Speckner; F. Klein; A. W. Thomas; W. Meyer; A. Braghieri; K. Hansen; K. Helbing; F. Zapadtka; G. Reicherz; B. Schoch; A. Wakai; V. Lisin; M. Schumacher; G. Zeitler; J. C. McGeorge; B. Seitz; T. Matsuda; Tadahisa Iwata; D. Ryckbosch; S. Hasegawa; N. Takabayashi; Michael Sauer; C. Bradtke; G. Anton; R. Leukel; F. Sadiq; R. Kondratiev
A direct measurement of the helicity dependence of the total photoabsorption cross section on the proton was carried out at MAMI (Mainz) in the energy range 200<E_gamma<800 MeV. The experiment used a 4
Physical Review Letters | 2009
S. Baunack; K. Aulenbacher; D. Balaguer Ríos; L. Capozza; J. Diefenbach; B. Gläser; D. von Harrach; Y. Imai; E. Kabuß; R. Kothe; J. H. Lee; H. Merkel; M. C. Mora Espí; U. Müller; E. Schilling; G. Stephan; C. Weinrich; J. Arvieux; M. A. El-Yakoubi; R. Frascaria; R. Kunne; Frank Maas; M. Morlet; S. Ong; J. Van de Wiele; S. B. Kowalski; Y. Prok; S. Taylor
\pi
Physics Letters B | 1985
W. Brückner; H. Döbbeling; F. Güttner; D. von Harrach; H. Kneis; S. Majewski; M. Nomachi; S. Paul; B. Povh; R.D. Ransome; T.-A. Shibata; M. Treichel; Th. Walcher
detection system, a circularly polarized tagged photon beam and a frozen spin target. The contributions to the Gerasimov-Drell-Hearn sum rule and to the forward spin polarizability
Physics Letters B | 1986
W. Brückner; H. Döbbeling; F. Güttner; D. von Harrach; H. Kneis; S. Majewski; M. Nomachi; S. Paul; B. Povh; R.D. Ransome; T.-A. Shibata; M. Treichel; Th. Walcher
\gamma_0
European Physical Journal C | 1991
J.G. Ashman; B. Badelek; Günter Baum; J. Beaufays; C. P. Bee; C. Benchouk; I.G. Bird; S. Brown; M. C. Caputo; H. W. K. Cheung; J. S. Chima; J. Ciborowski; R.W. Clifft; G. Coignet; F. Combley; G.R. Court; G. D'Agostini; J. Drees; M. Düren; N. Dyce; A. Edwards; M. Edward; T. Ernst; M.I. Ferrero; D. Francis; E. Gabathuler; R. Gamet; V. Gibson; J. Gillies; P. Grafström
determined from the data are 226 \pm 5 (stat)\pm 12(sys) \mu b and -187 \pm 8 (stat)\pm 10(sys)10^{-6} fm^4, respectively, for 200<E_\gamma<800 MeV.
Nuclear Physics | 1995
M. Arneodo; A. Paic; C. Scholz; G. van Middelkoop; H. Engelien; Y. Tzamouranis; F. Klein; A. Witzmann; S. Kullander; J.-L. Vuilleumier; E. Rondio; H.J. Kessler; T. Walcher; F. Sever; R. van Dantzig; G.K. Mallot; U. Landgraf; C. Whitten; A. Mücklich; C.H.Quentin Ingram; D. Sanders; R. Windmolders; M. van der Heijden; M.I. Ferrero; A. Milsztajn; C. Mariotti; D. Nowotny; K. Rith; A. Sandacz; R. Rieger
A new measurement of the parity violating asymmetry in elastic electron scattering on hydrogen at backward angles and at a four momentum transfer of Q;{2} = 0.22 (Ge V / c);{2} is reported here. The measured asymmetry is A_{LR} = (-17.23 +/- 0.82_{stat} +/- 0.89_{syst}) x 10;{-6}. The standard model prediction assuming no strangeness is A_{0} = (-15.87 +/- 1.22) x 10;{-6}. In combination with previous results from measurements at forward angles, it is possible to disentangle for the first time the strange form factors at this momentum transfer, G_{E};{s} = 0.050 +/- 0.038 +/- 0.019 and G_{M};{s} = -0.14 +/- 0.11 +/- 0.11.