Beautiful Braids by Mary Beth Janssen-Fleischman

By Mary Beth Janssen-Fleischman

В книге представлен огромный выбор причёсок с длинными волосами, преимущественно косы. Подробные поэтапные инструкции помогут выполнить понравившуюся причёску.

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By rotation  i   t wave approximation, only the items containing factor e  ml   1 /   ml  are remained. Let n  l in the fifth and sixth items of the formula, the transition probability amplitude is    2 am  t   ml     i   t  i   t Fˆ1ml Fˆ1ll  Fˆ1ll  e  ml   1 Fˆ1ml Fˆ1ll  Fˆ1ll  e  ml   1        2   ml   2ml   ml  (34) Therefore, after the second order process is considered, the total transition probability amplitude is  1 2 am  t    am  t    am  t   ml ml ml  i   t Fˆ1ml  e  ml   1  ˆ ˆ   1  F1ll  F1ll        ml  ml   (35)  Because we have ll  0 and l r l  0 , when m  l , the first item in (18) and (19) are equal to zero, but the second items are not equal to zero in general.

The propagation direction  of electromagnetic wave should be changed from k to  k under time reversal (Otherwise retarded wave would become advanced wave so that the law of causality would be Retarded Electromagnetic Interaction and Symmetry Violation of Time Reversal in High Order Stimulated Radiation and Absorption Processes of Lights as Well as Nonlinear Optics ... ). Let subscript T represent time reversal, from (3), (5) and (6), we have     Hˆ 1 T  x , t   Hˆ 1  x , t  and Hˆ 2T  x , t   Hˆ 2  x , t  .

With higher order revision, we have B12  B21 . Under the circumstance of having no electron population revision N 2  N 1 , as long as B21 is larger enough than B12 , we still have B21N 2  B12 N 1 . This means that without the reversion of electron population, laser can still be produced. At present, many experiments have verified this result [7]. In fact, the number of electrons on an energy level can not be determined directly at present. What can be determined by experiments is the number of photons emitted by atoms.

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