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High-speed two-photon imaging based on multi-foci excitation requires the use of spatially resolved detectors, such as charge coupled device (CCD) cameras, instead of single channel photomultiplier tube (PMT). The performance of systems based on both a PMT and a CCD in turbid medium was evaluated by measuring the image point spread function (PSF) and the image contrast as a function of depth and scattering coefficient with single point scanning. We found no significant change in the full-width at half maximum of the point spread function (PSF) for depth up to 100 μm. However, the CCD lost contrast significantly faster as a function of depth and increase scattering. This discrepancy is resolved by measuring a low amplitude but broad tail in the PSF distribution. The tail of the PSF distribution can be up to 200 μm in diameter. We further evaluate scattering effects in the imaging of GFP neurons in a mouse brain slice.

By coherently adding the spherical wavefronts of two opposing lenses, two-photon excitation 4Pi-confocal fluorescence microscopy has achieved three-dimensional imaging with an axial resolution 3–7 times better than confocal microscopy. So far this improvement was possible only in glycerol-mounted, fixed cells. Here we report 4Pi-confocal microscopy of watery objects and its application to the imaging of live cells. Water immersion of 4Pi-confocal microscopy of membrane stained live Escherichia coli bacteria attains a 4.3-fold better axial resolution as compared to the best water immersion confocal microscope. The resolution enhancement results into a vastly improved threedimensional representation of the bacteria. The first images of live biological samples with an all-directional resolution in the 190–280 nm range are presented here, thus establishing a new resolution benchmark in live-cell microscopy. # 2001 Elsevier Science B.V. All rights reserved.

We propose and demonstrate a method employing ferroelectric monomolecular layers, by which it is possible to precisely measure the planar light field polarization in the focus of a lens. This method allowed us to establish for the first time to our knowledge, the perpendicularly oriented field that is anticipated at high apertures. For a numerical aperture 1.4 oil immersion lens illuminated with linearly polarized plane waves, the integral of the modulus square of the perpendicular component amounts to (1.51 r 0.2) % of that of the initial polarization. It is experimentally proven that depolarization decreases with decreasing aperture angle and increases when using annular apertures. Annuli formed by a central obstruction with a diameter of 89 % of that of the entrance pupil raise the integral to 5.5 %. This compares well with the value of 5.8% predicted by electromagnetic focusing theory; however, the depolarization is also due to imperfections connected with focusing by refraction. Besides fluorescence microscopy and single molecule spectroscopy, the measured intensity of the depolarized component in the focal plane is relevant to all forms of light spectroscopy combining strong focusing with polarization analysis.