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crc press - E-Lib FK UWKS

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Model Amphipathic Peptides 89<br />

At the end of each protocol the integrity of the plasma membrane was verified<br />

by addition of trypan blue and measurement of the trypan blue fluorescence (λexc =<br />

543 nm, λem > 590 nm).<br />

To monitor the fluorescence images and measure the fluorescence intensities an<br />

LSM 410 invert confocal laser scanning microscope (Carl Zeiss, Jena GmbH, Jena,<br />

Germany) was used. Excitation was performed at 488 nm (Fluos) or 543 nm (Trypan<br />

Blue) using an argon-krypton or helium-neon laser and a dichroitic mirror FT 510<br />

or NT 543/80/20 for respective wavelength selection. Emission was measured at<br />

wavelengths >515 or >570 nm with cut-off filters LP 515 and LP 570, respectively,<br />

in front of the detector. The fluorescence intensities inside and outside the cell were<br />

recorded in predetermined regions of interest (ROIs, 16 × 16 pixel; 30 scans with<br />

a scan time of 2 sec with double averaging) as described by Lorenz et al. 30 The<br />

background fluorescence intensity was determined before addition of the peptide<br />

solution for 300 sec. For measurement of the intracellular fluorescence, three ROIs<br />

were selected in the cytosol and one in the nucleus of three cells in such a manner<br />

that the diffuse fluorescence could be recorded without interference with vesicular<br />

fluorescence.<br />

The intracellular fluorescence signal was corrected for contributions from the<br />

extracellular fluorescence arising from nonideal confocal properties of the CLSM<br />

by estimating the distribution function of sensitivity in the Z direction of the microscope,<br />

according to Wiesner et al. 31<br />

4.6.4.2 Measurement of Axial Response of the Confocal System<br />

Dye solution of 400 µl (carboxyfluorescein or fluorescein-labeled peptide; 1.25 µ M)<br />

was transferred to the cover slip. The fluorescence of the dye and the reflection<br />

signal of the excitation source were detected in a two-channel measurement. The<br />

scan plane (XY-plane) was moved in 1-µm steps in the Z direction up to 200 µm,<br />

beginning at the middle of the cover slip. Adjacent to the optical boundary (cover<br />

slip-dye) the step width was decreased to 0.2 µm. At each step a two-channel image<br />

(512 × 512 pixel) with a scan time of 2 sec and a double averaging was captured.<br />

The intensities of the fluorescence and reflection signals were obtained directly from<br />

the single-channel image after each scan. The values of the intensities were stored<br />

according to the Z position. The registration of the reflection signal was used for<br />

determining the Z position of the optical boundary.<br />

4.6.4.3 Calculation of Contributions from Out-of-Focus Planes<br />

to Intracellular Fluorescence Intensity<br />

After preincubating the cells for 10 min with 1.25 µM solutions of the dye or the<br />

flurescently labeled peptide respectively, and subsequent transfer of 400 µl of the<br />

cell suspension to the cover slip, optical measurements were performed using the<br />

experimental setup that follows.<br />

The XY-plane was positioned in the middle of a cell in the Z-axis using the<br />

reflection and the transmission modes of the microscope. Regions of interest (ROIs,<br />

16 × 16 pixel) were fixed between the center of the cell and the extracellular medium.

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