Amaliy yadro fiziкasi

А

J.2 l-r1ш11. ""РЬ og ·ir .fragmenti l10sil /,о· lis higa olib kel1Ncl1i 111rli parc/щlo11i.•l1lar 11ch1111 klasler Q parc/щ[ш1isl1 e11erg 1·asi11i11g chiчayolgan
klas/er massa soniga bog '[a11isl1i.

Bu 1·as111da klaste1· parcliala11isl1 eпergiyasi Q niпg, ⁰⁰' РЬ hosil bo'lisl1iga olib kelu,•cl1i turli parc lшlan is hlar 11chun, chiqayotgan klas­

terlar inassa\ariga bog'la11isl1i ko'1·satilga11. E11g katta el1tiшollikdagi cl1iq isl 1la1· sel1rli sonli fi-ag111entlarga to'g•ri keladi. А,= 208 (Z, = 82,
N_' = 126) va А_.,= 14. 24, 28. 34 (N,_. = 8, 14, 20) yadrolar eng katta chi-
qisl1larga ega .
43

Klaster parchalanishlarni nazariy tнslшn(irish ucht1n tшli modellar taklif etilgan. Ushbн modellar yordamida keyingi va lшli kasl1f e(ilma­ gan klaster parchalanishlar oldindan bashorat qili111110qda.
Tajribalar shнni ko'rsatdiki, t1sl1bt1 modellar Ьilan l1isoЫ,111gan klas­ ter parcl1alanisl1 parametrlari tajriba natijalari Ьilan jнda пюs tнsl1ar ekan.
Klaster parcl1alanish n10della1·idaп eng oxiгgilaгitian Ьiri yorclamida hisoЫangan yarim parclialanisl1lar dav1·i 1.2-jшlvalda kelti1·ilgan. Slш­ ningdek, Ьн jad,,alda tajribada olingan natijalar ham solisl1tirisl1 uchtш alohida ust11nda keltirilgan.
1.2-jatlval.
Klaste,· 1·(1{fioak1i1•/ik 11ch1m taj,·ibacla о 'lclia nga 11 ylll"im pa,-c/шlanish c/a1'l"i Ьi/а1111a::a,-iy hisoЬ/ang:an ушiт pш·clialanish clm•r/(ll"i11i solisl1ti1·is/1.

А ,А + А1

Q,MeV