Compensation of temporal and spatial dispersion for multiphoton acousto-optic laser-scanning microscopy

In laser-scanning microscopy, acousto-optic (AO) deflection provides a means to quickly position a laser beam to random locations throughout the field-of-view. Compared to conventional laser-scanning using galvanometer-driven mirrors, this approach increases the frame rate and signal-to-noise ratio, and reduces time spent illuminating sites of no interest. However, random-access AO scanning has not yet been combined with multi-photon microscopy, primarily because the femtosecond laser pulses employed are subject to significant amounts of both spatial and temporal dispersion upon propagation through common AO materials. Left uncompensated, spatial dispersion reduces the microscope’s spatial resolution while temporal dispersion reduces the multi-photon excitation efficacy. In previous work, we have demonstrated, 1) the efficacy of a single diffraction grating scheme which reduces the spatial dispersion at least 3-fold throughout the field-of-view, and 2) the use of a novel stacked-prism pre-chirper for compensating the temporal dispersion of a pair of AODs using a shorter mechanical path length (2-4X) than standard prism-pair arrangements. In this work, we demonstrate for the first time the use of these compensation approaches with a custom-made large-area slow-shear TeO2 AOD specifically suited for the development of a high-resolution 2-D random-access AO scanning multi-photon laser-scanning microscope (AO-MPLSM).

[1]  Rafael Yuste,et al.  Imaging calcium dynamics in dendritic spines , 1996, Current Opinion in Neurobiology.

[2]  P. Saggau,et al.  High-speed, random-access fluorescence microscopy: II. Fast quantitative measurements with voltage-sensitive dyes. , 1999, Biophysical journal.

[3]  D. Piston Imaging living cells and tissues by two-photon excitation microscopy. , 1999, Trends in cell biology.

[4]  P. Saggau,et al.  High-speed, random-access fluorescence microscopy: I. High-resolution optical recording with voltage-sensitive dyes and ion indicators. , 1997, Biophysical journal.

[5]  R. Stroud,et al.  Acousto-optic devices : principles, design, and applications , 1992 .

[6]  Da-Ting Lin,et al.  Multi-photon laser scanning microscopy using an acoustic optical deflector. , 2002, Biophysical journal.

[7]  J. Gordon,et al.  Negative dispersion using pairs of prisms. , 1984, Optics letters.

[8]  S W Hell,et al.  Ca2+ fluorescence imaging with pico- and femtosecond two-photon excitation: signal and photodamage. , 1999, Biophysical journal.

[9]  E. Treacy Optical pulse compression with diffraction gratings , 1969 .

[10]  Jean-Claude Diels,et al.  Ultrashort Laser Pulse Phenomena: Fundamentals, Techniques, and Applications on a Femtosecond Time Scale , 1996 .

[11]  J. Magee Dendritic integration of excitatory synaptic input , 2000, Nature Reviews Neuroscience.

[12]  F. Engert,et al.  Dendritic spine changes associated with hippocampal long-term synaptic plasticity , 1999, Nature.

[13]  Peter Saggau,et al.  Compensation of spatial and temporal dispersion for acousto-optic multiphoton laser-scanning microscopy. , 2003, Journal of biomedical optics.

[14]  J. Squier,et al.  Dispersion pre‐compensation of 15 femtosecond optical pulses for high‐numerical‐aperture objectives , 1998, Journal of microscopy.

[15]  Peter Saggau,et al.  Dispersion compensation for acousto-optic scanning two-photon microscopy , 2002, SPIE BiOS.