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8
< jZ[hl_
[2]
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(1.11)
(1.10)
(1.9.)
8 < jZ[hl_ [2] ijb\h^blky \ujZ`_gb_ ^ey lhdZ \ _^bgbqghf l_e_kghf m]e_ dI eh ′p ∑ ∫d 2 = 3 r ′ f (p, r)H ′ψ n (r ′) , (1.9.) dΩ m n \ dhlhjhf kmffbjh\Zgb_ \_^_lky ih \k_f \hafh`guf gZqZevguf khklhygbyfn. LZdbfh[jZahfbgl_gkb\ghklvnhlhbhgbaZpbbhij_^_ey_lkyd\Z^jZlhf Zfieblm^u jZkk_ygby f(p,r) dhlhjZy \uqbkey_lky q_j_a Zkbfilhlbq_kdmx nhjfmnmgdpbb=jbgZ JZkkfhljbfgZb[he__ijhklhckemqZciehkdbo \hegdh]^Z\aZbfh^_ckl\b_hlkmlkl\m_lbnmgdpby=jbgZbf__l\b^ 2 d 3k e ik ( r − r ′ ) ∫ ( 2π ) 2m G( r, r ′, p )= 2 2m h′ 3 p 2 − k 2 + iδ Fgh`bl_ev iδ \\h^blky \ agZf_gZl_ev ^ey \uiheg_gby ]jZgbqguo mkeh\bc\kemqZ_jZkoh^ys_cky\heguBgl_]jZe lZ[ebqgucihwlhfm 2 2m 1 ipR G( r, r ′, p )=− e , 2m h ′ 2 4πR (1.10) ]^_R=|r - r′|. <ij_^_e_ijbr→∞ \ujZ`_gb_ ^Z_l [ ] (1.11) = r − r ′ cos θ + O r ′ 1 2 lim R = lim r − 2rr ′ cos θ + r ′ 2 2 2 r →∞ r →∞ r
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