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By Donald F Geesaman

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Extra resources for Future directions in particle and nuclear physics of Multi-GeV hadron beam facilities : the proceedings of the Workshop held at Brookhaven National Laboratory, March 4-6 1993

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The procedure used here to analyze the Brookhaven data can be applied directly to quasi-elastic electroproduction experiments such as the SLAC-NE18. For consistency, these experiments should see the same attenuation cross sections at the same Q2. The free space scattering cross section in the case of electroproduction is also expected to receive significant contribution from large distance components of the proton wave function. Therefore, based on our experience with proton initiated experiment, the hard scattering in this case should again be quite different from free space scattering and should be closer to pQCD predictions.

195. Using data beyond that shown in Fig. 1, the ratio of the D-Y yield from W to that from an isoscalar target (C + D) was obtained [19]. Fig. 2 shows a plot of the values obtained for A(z2) as compared to some published sea quark distributions that account for the observed violation of the GSR. Two comments are in order. p(z) being greater than _p(z). The distribution that best fits the data is one [17] where the aT(z) -ii(z) difference occurs at small z. It should be noted that some of the approaches [14, 16] that associate the violation of the GSR with virtual mesons obtain o_ distributions similar to P_f.

Lett. 18, 1174 (1967). [10] D. A. Ross and C. T. Sachrajda, Nucl. Phys. B149, 497 (1979). [11] E. M. Henley and G. A. Miller, Phys. Lett. B251, 453 (1980). [12] S. Kumano and J. T. Londergan, 717 (1991). Phys. Rev. D44, [13] A. Signal, A. W. Schreiber, and A. W. Thomas, Mod. Phys. Lett. A6, 271 (1991). - 26 - [14] A. Szczurek and J. Speth, private communication. [15] E. Eichten, I. Hinchliffe, and C. Quigg, Phys. Rev. D45, [16] E. Eichten, I. Hinchliffe, and C. Qui_, 2269 (1991). Phys. ltev. D4T, 747 (1993).

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