| Primary Source |
[18] D. S. Correa, L. Boni, D. S. Santos, Jr., N. M. B Neto, O. N. Oliveira, Jr., S. C. Misoguti Zilio, and C. R. Mendonca, “Reverse saturable absorption in chlorophyll a,” Appl. Phys. B, vol. 74, pp. 559–561, 2002. [19] L. De Boni, D. S. Chorrea, F. J. Pavinatto, D. S. Dos Santos, Jr., and C. R. Mendonca, “Excited state absorption spectrum of chlorophyll a obtained with white-light continuum,” J. Chem. Phys., vol. 126, pp. 165102– 165104, 2007. [20] H. Linschitz and K. Sarkanen, “The absorption spectra and decay kinetics of the metastable states of chlorophyll A and B,” J. Amer. Chem. Soc., vol. 80, pp. 4826–4832, 1958. [21] J. Baugher, J. C. Hindman, and J. J. Katz, “Determination of the triplet and excited singlet absorption spectra of chlorophyll a with a tunable dye laser,” Chem. Phys. Lett., vol. 63, pp. 159–162, 1979. [22] N.V. Tkachenko,D.Grandell, M. Ikonen, A. Jutila,V. Moritz, andH. Lemmetyinen, “Excitation energy relaxation in chlorophyll a Langmuir– Blodgett multilayer films,” Proc. SPIE, vol. 1921, pp. 254–260, 1992.PubMed ID17477634
|
| Method |
The theoretically simulated switching characteristics namely,
the variation in the normalized transmission of probe beam intensity
(NTPI) with time, obtained by computer simulations, using
(1)–(9), considering the S0 , S1 , and T1 states, corresponding
to the experimental conditions with typical parameters given in
Table I [primary sources], are shown in Fig. 3(b). |