1979
DOI: 10.1016/0375-9474(79)90001-0
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Fluctuations in polarized proton scattering from 28Si

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Cited by 5 publications
(11 citation statements)
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“…The condition (14) can be proved for rather wide range of scattering angles near ~c/2 when N=Nma X [4,5] and N I=N 2 = Nmax/2 (see Appendix 1). Proceeding away from ~/2 value into the range of forward and backward angles where the effective number of independent channels becomes smaller N<Nma X [4,5], one cannot succeed in establishing the statistical independence of a and b in the general case because of the complicated calculations involved here.…”
Section: Afl=a(as) Bfl=b(;js) Afi=af+bfl=o((~s )mentioning
confidence: 97%
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“…The condition (14) can be proved for rather wide range of scattering angles near ~c/2 when N=Nma X [4,5] and N I=N 2 = Nmax/2 (see Appendix 1). Proceeding away from ~/2 value into the range of forward and backward angles where the effective number of independent channels becomes smaller N<Nma X [4,5], one cannot succeed in establishing the statistical independence of a and b in the general case because of the complicated calculations involved here.…”
Section: Afl=a(as) Bfl=b(;js) Afi=af+bfl=o((~s )mentioning
confidence: 97%
“…In deriving (19) it has been taken into account that the effective number of independent channels N corresponding to the total cross section is twice as great as those (N~ and N2) for the cross sections a and b. The last statement is the straightforward consequence of uncorrelation condition (14). For N=2 (19) leads to the result of [24].…”
Section: Rn(x Z) = Rn~ (X ) Rn~(z)mentioning
confidence: 99%
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