Современные методы исследования и описания кристаллических структур. Самойлов А.М. - 5 стр.

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ВГУ | Воронеж

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2
FZdkbfZevgZyqZklhlZ
νν
max
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λλ
min
khhl\_lkl\m_liheghc
hklZgh\d_we_dljhgh\ (
E
2
= 0 ).
h
νν
max
= hc/
λλ
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= E
1
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( 1.3 )
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√√
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= (Z
−−
σσ
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( 1.5 )
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                                                   2
      FZdkbfZevgZyqZklhlZνmax fbgbfZevgZy^ebgZ\hegu λmin khhl\_lkl\m_liheghc

hklZgh\d_we_dljhgh\ ( E2 = 0 ).

        hνmax = hc/λmin = E1 = eU,                                    ( 1.3 )

      ]^_U -mkdhjyxs__gZijy`_gb_

      Ihkdhevdm E2 fh`_lbf_lvex[mx\_ebqbgmf_gvrmx E1lhg_ij_ju\gucki_dlj
kh klhjhgu ^ebgguo \heg h]jZgbq_g ebrv ih]ehs_gb_f fy]dbo emq_c \ fZl_jbZe_
hdhrdZljm[dbb\\ha^mo_
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EgZ\ZdZglgh_f_klh\h\gmlj_gg_ch[hehqd_bkimkdZxlnhlhgu
             hν = E − E0                                    ( 1.4 )
<_ebqbgZ hij_^_ey_lky oZjZdl_jghc ^ey dZ`^h]h we_f_glZ kbkl_fhc _]h wg_j]_lbq_kdbo
mjh\g_c Ebgbb ki_dljZ jZa^_eyxlky gZ k_jbb K, L, M, N ...\aZ\bkbfhklbhllh]hk

dZdhch[hehqdb[uem^Ze_gwe_dljhgjm]b_ ebgbb bf_xl _s_ f_gvrmx bgl_gkb\ghklv QZklhlZ dZdhc-
eb[hebgbbbaf_gy_lkyijbi_j_oh^_hlh^gh]hwe_f_glZd^jm]hfmihaZdhgmFhaeb

         √ ν = (Z − σ ),                                         ( 1.5 )

      ]^_Z -aZjy^y^jZcbσ -ihklhyggu_


      < j_gl]_ghkljmdlmjghf ZgZeba_ \ dZq_kl\_ fhghojhfZlbq_kdh]h baemq_gby  qZs_

\k_]hbkihevamxlkyebgbb Kα1b Kα2 f_lZeeh\hlojhfZ  Z  ^hfheb[^_gZ Z =
 ^ebgu\hegdhlhjuoe_`Zl\bgl_j\Ze_hl^hgf
      Wdki_jbf_glZevgu_ b l_hj_lbq_kdb_ hkgh\u j_gl]_ghkljmdlmjgh]h b nZah\h]h
ZgZebaZ  l\_j^uo  l_e  [ueb  aZeh`_gu  \  -191  ]]  \  jZ[hlZo F EZmw1 b _]h

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