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By Baldassase Di Bartolo, Baldassare Di Bartolo, Xuesheng Chen

ISBN-10: 9810247281

ISBN-13: 9789810247287

This quantity describes advances in either experimental and theoretical remedies within the box of strength move techniques which are suitable to varied fields, reminiscent of spectroscopy, laser know-how, phosphors, synthetic solar power conversion, and photobiology. It provides the rules and to be had options via particular examples. additionally, it examines present and attainable purposes, together with the latest advancements, and initiatives destiny advances and study percentages within the box.

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Read Online or Download Advances in energy transfer processes: proceedings of the 16th course of the International School of Atomic and Molecular Spectroscopy: Erice, Sicily, Italy, 17 June-1 July, 1999 PDF

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Additional resources for Advances in energy transfer processes: proceedings of the 16th course of the International School of Atomic and Molecular Spectroscopy: Erice, Sicily, Italy, 17 June-1 July, 1999

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6 A for transition metal ions. In view of these small values exchange interactions are generally small and negligible. 4. Phonon-Assisted Energy Transfer The probability for energy transfer between two ions in solids is proportional to the overlap integral \gA{E)gB{E)dE = h\gA{a)gB(a)do (105) where gA(a>) and gB((o) are the line shape functions for ions A and B, respectively. If we consider the case of two Lorentzian lines of width ACOA and ACOB, centered at (OA and (OB, respectively, we find a \gA(a)gB(o))dco = - (A©) +((O.

The Relevant Energy Transfer Hamiltonian Let us consider again a two-atom system as in Figure 4. Each atom has a nucleus of charge z and one electron. _ z„zbe R zazhe R e '12 r„ „2 2 zbe a2 '41 r„0 T^ •+ 2 zae r„ n, (52) zbe -R + l, Let |a) and \a') be the ground state and excited state wavefunctions of atom A, respectively and \b) and \b') the ground state and excited state wavefunctions of atom B, respectively. We shall consider a transition from an initial state |1) to a final state |2) of the two-atom system, where \l) = \a'b), \2)=\ab') (53) The relevant matrix element is given by Fig.

Pulsed Excitation Assume that we have a number No of donors and NA of acceptors and call CODA the probability of D —> D energy transfer per unit time. Assume also that O>DD the probability of D —> D energy transfer is negligible. The question we shall try to answer is the following: If we excite a number of donors with a light pulse, how will the system respond? 0) no relevant D —>A transfer takes place. If Nd(0) = number of donors in the ground state at time t=0 Na(0) = number of acceptors in the ground state at time t=0 then Nd(0) = ND-Nd,(0) (112) Na(0) = NA (113) We shall call x the lifetime of the donor, in the absence of the activator: v-l=P + wnr (114) where P = probability of spontaneous emission per unit time wnr = probability of nonradiative decay per unit time We shall define pi(t) = probability that the donor at position Rt is excited at time t and p{t) = statistical average of p0) The number of excited donors at time t is given by Nd{0) p(t) and the probability of finding a donor excited at time t by p ( 0 ^ » ND > «~>0 « (115) ND The number of quanta emitted as luminescence by the donors per unit time is PNjQWt) (116) 33 The total number of quanta emitted as luminescence by the donors is N = PNce(0)j~p(t)dt (117) The total number of quanta emitted by the donors, in the absence of activators, is N0 = PNj (0)j"V ( ' / r ) rff = PNd, (0)T (118) The quantum yield of luminescence is iL^r-pwt (H9) Summary The excitation of the donor atoms is generally accomplished by sending a light beam on the sample.

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Advances in energy transfer processes: proceedings of the 16th course of the International School of Atomic and Molecular Spectroscopy: Erice, Sicily, Italy, 17 June-1 July, 1999 by Baldassase Di Bartolo, Baldassare Di Bartolo, Xuesheng Chen


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