Ultrafast Photoconversion of the Green Fluorescent Protein Studied by Accumulative Femtosecond Spectroscopy  Florian Langhojer, Frank Dimler, Gregor Jung,

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Ultrafast Photoconversion of the Green Fluorescent Protein Studied by Accumulative Femtosecond Spectroscopy  Florian Langhojer, Frank Dimler, Gregor Jung, Tobias Brixner  Biophysical Journal  Volume 96, Issue 7, Pages 2763-2770 (April 2009) DOI: 10.1016/j.bpj.2008.11.049 Copyright © 2009 Biophysical Society Terms and Conditions

Figure 1 Simple potential energy scheme of T203V GFP. (Left) Photocycle of the RH form of GFP including excitation, excited state proton transfer, fluorescence, and reprotonation. In this study, it was found that further excitation from RH∗ with 800 nm leads to a higher excited state RH∗∗, which is responsible for decarboxylation under femtosecond excitation conditions (dotted arrow). Time constants (†,‡) taken from the literature (10,17). (Right) Photoconverted form R−pc. Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 2 Normalized absorption (solid line) and fluorescence (dashed line) spectra of the T203V mutant of GFP used in this work. Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 3 Schematics of the experimental setup. Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 4 Calibration scan of the accumulation setup. Data shown as dots, best fit to model function shown as shaded surface. (Inset) Concentrations Ci in different volumes i defined by beam geometry with rates for diffusion di and product accumulation η (see text). Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 5 Power studies: (a) Fluorescence upon excitation with 800-nm pulses. (b) Photoconversion efficiency upon excitation with 800-nm pulses. (c) Fluorescence upon excitation with 400-nm pulses. (d) Photoconversion efficiency upon excitation with 400-nm pulses. The abscissas of all plots (a–d) represent the peak intensities in the sample. Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions

Figure 6 Time-resolved two-color experiment on photoconversion. After initial excitation of RH to RH∗ with a 400-nm pulse, a 800-nm pulse induces photoconversion, and the diffusion-corrected conversion efficiency (for a single laser pulse sequence) is shown as a function of pump-repump time delay. The constant offset at negative time delays is due to the photoconversion caused by the single 800- and 400-nm pulses. Biophysical Journal 2009 96, 2763-2770DOI: (10.1016/j.bpj.2008.11.049) Copyright © 2009 Biophysical Society Terms and Conditions