By Asoke N. Mitra
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W. Negle, ibid, p. 148 and private communication. G. W. , private communication. J. D. , private communication. L. Rosen, Nucl. Appl. S_ (1968) 375. M. M. Kligerman, Proc. Int'l Particle Radiation Therapy Workshop, Key Biscayne, FL (1975). P. M. Grant, B. R. Erdal, and H. A. , J. of Nucl. Medicine 1£ (1975) 300. An abbreviated form is used. AN OBE-MODEL INCLUDING THE N- Δ -INTERACTION, TWO-NUCLEON AND NUCLEAR MATTER RESULTS by K. B 1 e u 1 e r, K. H o l i n d e , R. g. 2) HM1 ) has been replaced by a so-called eikonal form factor, which arises from a simplified summation of multiple vector meson exchange processes.
The continuum ambiguity. Even smoother dependence then can be obtained using In passing we remark that of the 2 =64 possible ways to conjugate Barrelet zeros at each of the 25 energies considered some 50% of all newly generated amplitudes proved to be unitary! Neglecting Coulomb effects in this case is hardly justified, to be contrasted with πΝ and KN scattering. For 20) πΝ the full exploration J of the continuum ambiguity including spin and isospin is near completion showing considerable ambiguity corridors at higher energies, r· · 1«.
F. Turner, and N. W. Kindsay, IEEE Trans. Nucl. Sei. NS-12 (1965) 138. E. A. Knapp, В. С. Knapp and J. M. Potter, Rev. Sei. Instr. 3£ (1968) 979. D. С Hagerman, IEEE Trans. Nucl. Sei. NS-20 (1973). H. Butler, IEEE Trans. Nucl. Sei. 1 (1971) 336. H. H. Howard, "LAMPF USERS HANDBOOK," Los Alamos Report, MP-D0-1-UHB (1974). It describes details of beam channels, LAMPF organization, and procedure for submitting proposals. J. E. Simmons, Proc. High Energy Phys. and Nucl. , Santa Fe (1975) 103. C. , Proc.
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