By Stuart A. Rice
This sequence offers the chemical physics box with a discussion board for serious, authoritative reviews of advances in each quarter of the self-discipline. This stand-alone unique subject matters quantity stories fresh advances in electron-transfer examine with major, updated chapters via the world over famous researchers.
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The fact that the 1-TS and 2-TS paths scatter mainly in opposite directions is also the reason for the alternation in sign of ÁPn0 n ðJ; EÞ pointed out above. It is important to realize that this alternation is not exact. For example, in Fig. 3 eV, the alternation is broken by ÁPn0 n ð2; EÞ ¼ 0. We can explain the approximate alternation of ÁPn0 n ðJ; EÞ ¼ 0 by substituting Eq. (19) into Eq. (35), to obtain ÁPn0 h i ½1ÀTS 2 Ã ½2ÀTS ðJ; EÞ ¼ À2FðJÞ Re S ðJ; EÞ S ðJ; EÞ 0 0 n n n n n ð36Þ We then invert Eq.