By H. Staub (auth.), Dr. W. Grüebler, Dr. V. König (eds.)
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B. R. O'Fallon, Particle Accel, ~. F. G. C. Bro"~Jn, W. C. W. D. E. A. B. M. R. O'Fallon, Phys. Rev. Lett. ]1, (1973) 783; 32, (1974) 77, 34, (1975) 558; Phys. Lett. M. , 2nd International Symposium on Polarization Phenomena, Karlsruh (1965) pp. 322-323 High Energy Experimente 47 7) M. Froisart and R. Stora, Nucl. Instr. and Meth. 7, (1960), 297 D. Cohen, Rev. Sci. Inst. B. Roberts editor DISCUSSION Raynal: Is it more difficult to look in the vertical plane than to add a polarimeter ? In the vertical plane you get a coefficient as interesting as Cnn Krisch: It is very difficult to rotate the scattering plane into the vertical plane since the spectrometer is 30 m long and contains heavy magnets.
3. This measures the left-right asymmetry in p-C scattering of the recoil protons from a 13cm carbon target. The analyzing power of this polarimeter was calibrated using the ZGS polarized beam accelerated to about 250 MeV. For each of the 4 initial spin states we measured the number of recoil protons in each final spin state; we thus obtained the cross sections for the 8 different 3-spin states such as o(tt+Ot). Our notation is o(Beam, Target + Scattered, Recoil) and O denotes unmeasured. , o(tt + +t)=O.
Perimental values. c) If one reduces yOBE to a static, maximum local ansatz10}, one gets for large distances (r >1 fm) the same expressions as with the phenomenological (maximum local)-potentials (Reid or Hamada-Johnston potentiala). In this way, the long range part of the N-N potential becomes clearly physically interpretable ·on the basis of OBE. (For large r, non-localities are expected to play a minor role so that all OBE potentiala should be equivalent in this region). The dif:ferenţ parts o:f the N-N interaction then have the following interpretation10J.