1976
DOI: 10.1007/978-3-0348-5506-8_202
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Analyzing power Fluctuations in the % MathType!MTEF!2!1!+- % feaagCart1ev2aaatCvAUfeBSjuyZL2yd9gzLbvyNv2CaerbuLwBLn % hiov2DGi1BTfMBaeXatLxBI9gBaerbd9wDYLwzYbItLDharqqtubsr % 4rNCHbGeaGqiVu0Je9sqqrpepC0xbbL8F4rqqrFfpeea0xe9Lq-Jc9 % vqaqpepm0xbba9pwe9Q8fs0-yqaqpepae9pg0FirpepeKkFr0xfr-x % fr-xb9adbaqaaeGaciGaaiaabeqaamaabaabaaGcbaWaaWbaaSqabe % aacaaIXaGaaGyoaaaakiaadAeadaqadaqaaiqadchagaWcaiaacYca % caWGWbaacaGLOaGaayzkaaGaamyyaiaad6gacaWGKbWaaWbaaSqabe % aacaaIXaGaaGyoaaaakiaadAeadaqadaqaaiqadchagaWcaiaac

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“…The relation (6) implies that in the averaged cross section there is no interference between DI and CN processes, while for fixed energy the cross sections a, b and cr contain compound-direct interference terms which are proportional to Re((S)6S*). Our consideration is based on the initial statistical provisions of Ericson's fluctuation theory [1][2][3][4][5].…”
Section: Afl=a(as) Bfl=b(;js) Afi=af+bfl=o((~s )mentioning
confidence: 98%
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“…The relation (6) implies that in the averaged cross section there is no interference between DI and CN processes, while for fixed energy the cross sections a, b and cr contain compound-direct interference terms which are proportional to Re((S)6S*). Our consideration is based on the initial statistical provisions of Ericson's fluctuation theory [1][2][3][4][5].…”
Section: Afl=a(as) Bfl=b(;js) Afi=af+bfl=o((~s )mentioning
confidence: 98%
“…Here AP for the direct reaction denoted by A d reads (20) and Ya = aj(a) (21) is the relative contribution of the cross section of direct processes into the total averaged cross section (6). 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.…”
Section: Rn(x Z) = Rn~ (X ) Rn~(z)mentioning
confidence: 99%
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